8.474bo.com

CPC(HEP&NP),2012,36(12):1157–1286ChinesePhysicsCVol.
36,No.
12,Dec.
,2012TheNUBASE2012evaluationofnuclearpropertiesG.
Audi1,§,F.
G.
Kondev2,M.
Wang1,3,4,B.
Pfeiffer5,,X.
Sun1,J.
Blachot1,andM.
MacCormick61CentredeSpectrometrieNucleaireetdeSpectrometriedeMasse,CSNSM,CNRS/IN2P3,UniversiteParis-Sud,Bat.
108,F-91405OrsayCampus,France2ArgonneNationalLaboratory,9700S.
CassAvenue,Argonne,IL60439,USA3Max-Planck-Institutf¨urKernphysik,Saupfercheckweg1,D-69117Heidelberg,Germany4InstituteofModernPhysics,CAS,509NanchangRd.
,Lanzhou730000,China5GSIHelmholtzzentrumf¨urSchwerionenforschung,Planckstr.
1,D-64291Darmstadt,Germany6InstitutdePhysiqueNucleaire,CNRS/IN2P3,UniversiteParis-Sud,F-91406Orsaycedex,FranceAbstractThispaperpresentstheNUBASE2012evaluationthatcontainstherecommendedvaluesfornuclearanddecaypropertiesofnuclidesintheirgroundandexcitedisomeric(T1/2≥100ns)states.
Allnuclidesforwhichsomeexperimentalinformationisknownareconsidered.
NUBASE2012coversalluptodateexperimentaldatapublishedinprimary(journalarticles)andsecondary(mainlylaboratoryreportsandconferenceproceedings)references,togetherwiththecorrespondingbibliographicalinformation.
DuringthedevelopmentofNUBASE2012,thedataavailableinthe"EvaluatedNuclearStruc-tureDataFile"(ENSDF)databasewereconsulted,andcriticallyassessedoftheirvalidityandcompleteness.
Furthermore,alargeamountofnewandsomewhatolderexperimentalresultsthatweremissinginENSDFwerecompiled,evaluatedandincludedinNUBASE2012.
Theatomicmassvaluesweretakenfromthe"AtomicMassEvaluation"(AME2012,secondandthirdpartsofthepresentissue).
Incaseswherenoexperimentaldatawereavailableforaparticularnuclide,trendsinthebehaviorofspecicpropertiesinneighboringnuclei(TNN)wereexamined.
Thisapproachallowedtoestimate,wheneverpossible,valuesforarangeofproperties,andarelabeledinNUBASE2012as"non-experimental"(agged"#").
Evaluationproceduresandpoliciesthatwereusedduringthedevelopmentofthisdatabasearepresented,togetherwithadetailedtableofrecommendedvaluesandtheiruncertainties.
AMDC:http://amdc.
in2p3.
fr/andhttp://amdc.
impcas.
ac.
cn/1IntroductionTheNUBASE2012evaluationrespondstotheneedsexpressedbythebroadernuclearphysicscommunity,fromfundamentalphysicstoappliednuclearsciences,foradatabasethatcontainsvaluesofthemainnuclearprop-ertiessuchasmasses,excitationenergiesofisomers,half-lives,spinsandparities,decaymodesandtheirintensities,forallknownnucleiintheirgroundandexcitedisomericstates.
TheinformationpresentedinNUBASE2012repre-sentsthefundamentalbuildingblocksofthemodernnu-clearphysics,andspecically,ofthenuclearstructureandnuclearastrophysicsresearch.
ThemainapplicationofNUBASE2012isthe"AtomicMassEvaluation"(AME2012,secondandthirdpartsofthisissue)whereitisimperativetohaveanunambiguousidenticationofallstatesinvolvedinaparticulardecay,reactionormass-spectrometermeasurement.
Thisistheprimaryreasonforwhichthetwoevaluationsarecoupledtogetherinthepresentissue,forthesecondtimesincetheexistenceofthe"AtomicMassEvaluation".
Furthermore,withtheadvancesofmodernmass-spectrometrytechniques(seeforexampleRef.
[1]forarecentreview)andtheavailabilityofintensestableandrare-isotopebeams,alargenumberofunstablenucleicanbeproducedinasingleexperimentintheirgroundand/orisomericstates,andtheirmassesmeasuredwithhighpre-cision.
Thus,NUBASE2012canbeparticularlyusefulforfuturemassmeasurements,whereanunambiguousidenti-cationofcomplexmass-spectrometrydatawouldbere-quired.
Applicationsofthisdatabaseinastrophysicsnetworkcalculationsandintheoreticalstudiesofnuclearproper-ties,wherecompleteandreliabledataforallknownnucleiareneeded,arealsoenvisioned.
Least,butnotlast,theevaluateddatapresentedinNUBASE2012couldalsobeusefulforspecialistsina*ThisworkhasbeenundertakenwiththeencouragementoftheIUPAPCommissiononSymbols,Units,Nomenclature,AtomicMassesandFundamentalConstants(SUNAMCO).
§Correspondingauthor.
E-mailaddress:amdc.
audi@gmail.
com(G.
Audi).
Presentaddress:II.
PhysikalischesInstitut,Justus-Liebig-Universit¨at,Heinrich-Buff-Ring16,D-35392Gieen.
c2012ChinesePhysicalSocietyandtheInstituteofHighEnergyPhysicsoftheChineseAcademyofSciencesandtheInstituteofModernPhysicsoftheChineseAcademyofSciencesandIOPPublishingLtd1158ChinesePhysicsC(HEP&NP)Vol.
36numberofappliednuclearelds,suchasreactorengi-neeringanddesign,fuelmanufactureandtransport,wastemanagement,materialanalysis,medicaldiagnosticsandradiotherapy,andanywherewhenoneneedstoaccessba-sicinformationonanynuclide.
TheinformationpresentedinNUBASE2012fulllsseveraluser-demandedrequirements,namelythatitis:a)completeincludesallmeasuredquantitiesandtheirun-certainties,b)up-to-dateresultsfromthemostrecentpublicationsareincluded,c)credibleandreliableiden-tiesandresolvescontradictoryresultsthatexistinthescienticliterature,aswellasinothernuclearphysicsdatabases,d)properlyreferencedprovidescomprehen-siveinformationonthevalidityofallincludeddata.
MostofthedataincludedinNUBASE2012areinprincipleavailableintwootherevaluateddatabases:the"EvaluatedNuclearStructureDataFile"(ENSDF)[2]andthe"AtomicMassEvaluation"(AME2012).
Therefore,thedemandforNUBASEcouldbepartiallyfullledbycombiningthesetwodatabasesintoasingle,'horizontal'structure,whichexistsinAME,butnotinENSDF.
There-fore,NUBASE2012couldbeconsidered,atarstlevel,asacriticalcompilationofthosetwoevaluations.
DuringthedevelopmentofthepresentversionofNUBASE,itwasimperativetoexamineallavailablelitera-tureforseveralnuclidesinordertoreviseresultsadoptedinENSDF,andtoensurethattherecommendeddataarepresentedinaconsistentway(credibilityandreliabil-ityrequirement).
Itwasalsonecessarytoincludealltheavailableexperimentaldata,i.
e.
notonlyresultsthatwerepublishedrecently(up-to-daterequirement),butalsosomewhatolderdatathatweremissinginENSDF(com-pletenessrequirement).
Thisimpliedthatsomeextraeval-uationworkwascarriedout,andthecorrespondingcon-clusionsareaddedasremarksintheNUBASE2012table,andinthediscussionsbelow.
CompletebibliographicalreferencesaregivenforalladdedexperimentaldatainTa-bleI(seeSection2.
7).
Thereisnostrictliteraturecut-offdatefortheresultspresentedintheNUBASE2012evaluation:alldataavail-abletotheauthorsuntilthematerialwassentforpubli-cation(November18,2012)havebeenincluded.
Resultsthatwerenotincorporatedforspecialreasons,e.
g.
theneedforaheavyrevisionoftheevaluationatatoolatestageofdevelopment,areadded,wheneverpossible,inremarkstotherelevantdata.
Noteaddedinproof:ref.
[2012Ku.
1]reportsalargeamountofimportantinformation,inparticulartheidenti-cationofaseriesofNZ=42nuclidesbetweenEuandYbthatweincludewithoutanyestimatedmass,half-lifeorspin/parity.
ThecontentsofNUBASE2012aredescribedbelow,togetherwiththeadoptedpoliciesthatwereusedduringthedevelopmentofthisdatabase.
Section3presentstheupdatingprocedures,whiletheelectronicdistributionandinteractivedisplayofNUBASE2012contentsbymeansofaWorldWideWebJavaprogram,andbyastand-alonePC-programaredescribedinSection4.
ThepresentpublicationincludesandupdatesalltheinformationgiveninthepreviousversionsofNUBASE:NUBASE1997[3],andNUBASE2003[4].
2ContentsofNUBASE2012TheNUBASE2012evaluationcontainsrecommendedvaluesforsomeofthebasicnucleargroundstateproper-ties,for3350nuclides,derivedfromallavailableexper-imentalresults,togetherwithsomevaluesestimatedbyextrapolatingneighboringones.
NUBASE2012alsocontainsdataonisomericstates(seeSection2.
2forourcurrentdenition).
Wepresentlyknow1256nuclideswhichhaveone,ormore,excitedisomersinaccordancewithourdenition.
Intheveryrstversion,NUBASE1997,weusedalimiteddeni-tionofisomerswhereonlystateswithhalf-livesgreaterthan1millisecondwereconsidered.
InNUBASE2003westartedtoextendthedenitionofisomerstonuclidicspecieslivinglongerthan100ns.
Now,inNUBASE2012,weincludeallisomersthathavehalf-livesbeyond100ns.
WealsoincludethedescriptionofthosestatesthatareinvolvedinmassmeasurementsandthusfoundinAME2012,seethere,PartI,Section1.
1,p.
1288).
NUBASE2012alsocontainsdataon186isobaricana-logstates(IAS),whichhavetheirexcitationenergiesde-terminedeitherthroughan"internalrelation"andtakenfromENSDF,orthroughan"externalrelation"andthendeterminedbytheAME2012evaluation.
Foreachnuclide(A,Z),andforeachstate(groundorexcitedisomer),thefollowingpropertieswerecompiledand,whennecessary,evaluated:massexcess,excitationenergyofexcitedisomericstates,half-life,spinandparity,decaymodesandtheirintensities,isotopicabundance(forastablenuclide),yearofdiscoveryandthecorrespondingbibliographicalinformationforallexperimentalvaluesoftheaboveitems.
Referencestopublishedarticlesinthedescriptionsec-tionsbelowaregivenbymeansofthekeynumberstyleusedinthe"NuclearScienceReference"(NSR)biblio-graphicaldatabase[5].
However,referencesquotedintheNUBASE2012tablesareabbreviatedwiththersttwodigitsoftheyearofpublicationbeingomittedfromtheNSRkeynumbers.
Thecompletereferencelistisgivenattheendofthisissue,togetherwiththereferencesusedinAME(seeAME2012,PartII,p.
1863inthisissue).
No.
12G.
Audietal:TheNUBASE2012evaluationofnuclearproperties1159InNUBASE1997,thenamesandchemicalsymbolsusedforelements104to109werethoserecommendedbytheCommissiononNomenclatureofInorganicChem-istryoftheInternationalUnionofPureandAppliedChemistry(IUPAC)[6]atthattime.
Unfortunately,thosenameswerechangedshortlybeforethepublicationofNUBASE2003,andtwoofthemweredisplaced,thusre-sultinginsomeconfusion(seealsoAME2012,PartI,Section6.
8,p.
1317).
Therefore,theusersshouldbecarefulwhencomparingresultsbetweenNUBASE1997,NUBASE2003andthepresentNUBASE2012evaluationsfornuclideswithZ≥104.
Thenaladoptednamesandsymbols,asrecommendedbyIUPACare:104rutherfordium(Rf),105dubnium(Db),106seaborgium(Sg),107bohrium(Bh),108hassium(Hs),109meitnerium(Mt),110darmstadtium(Ds),111roentgenium(Rg),112copernicium(Cn),114erovium(Fl),and116livermorium(Lv).
TheprovisionalsymbolsEd,Ef,Eh,andEiareusedinNUBASE2012foryetunnamedelementswithZ=113,115,117,and118,respectively.
NUBASE2012containsnumericalandbibliographicaldataforallknownnuclidesforwhichatleastonepropertyisknownexperimentally,intheirgroundstate,excitediso-mericstateswithT1/2≥100ns,andisobaricanalogstates.
However,italsoincludesinformationon,asyet,unob-servednuclides.
Thesewereestimatedfromtheobservedtrendsinexperimentaldataofneighboringnuclei(TNN),inordertoensurecontinuityinthesetofconsiderednu-clidessimultaneouslyinN,inZ,inAandinNZ.
Thechartofnuclidesdenedinthiswayhasasmoothcontour.
Fortheyetexperimentallyunknownproperties,valueswereestimated,herealso,fromtheobservedtrendsinex-perimentaldataofneighboringnuclei(TNN).
SimilarlytoAME2012,wheremassesestimatedfromtrendsinthemasssurface(TMS)areaggedwiththesymbol'#',thesamesymbolisusedinNUBASE2012toindicateTNNnon-experimentalinformation.
SuchanapproachallowedtofollowthebehaviorofaparticularnuclearpropertyasafunctionofNandZinaconsistentway,anditprovedbenecialindeducingval-uesforotherrelevantproperties.
Forexample,theexcita-tionenergyoftheJπ=11/2(h11/2)isomerin179Tlisnotknownexperimentally.
However,fromtheextrapolationofvaluesknownforthesamecongurationintheneigh-boring177Tlm,181Tland183Tlmnuclides,onecanesti-mateEx=825#(10#)keVfor179Tlm.
Thisvalue,togetherwiththeknowndecaypropertiesofthedaughter(175Aum)andgrand-daughter(171Irm)nuclides,allowedtoobtainestimatesoftheexcitationenergiesofsimilarisomersinthelatternuclidesatEx=167#(12#)and160#(14#)keV,respectively,whicharenotdirectlymeasuredyet.
Asarule,onestandarddeviations(1σ)areusedinNUBASE2012torepresenttheuncertaintiesassociatedwiththequotedexperimentalvalues.
Unfortunately,au-thorsofresearcharticlesdonotalwaysdenethemean-ingoftheirreporteduncertaintiesand,undersuchcircum-stances,thosevalueswereassumedtobeonestandardde-viations.
Inmanycases,uncertaintiesarenotevengivenatall.
Theyareestimatedbyus,consideringthelimitationsoftheexperimentalmethod.
ValuesandcorrespondinguncertaintiesforpropertiesgiveninNUBASE2012areroundedoff,evenifunroundedvaluesweregivenintheliteratureorinENSDF.
Incaseswherethetwofurthest-leftsignicantdigitsintheuncer-taintywerelargerthanagivenlimit(setto30fortheen-ergylevels,andtobeconsistentwithAME2012,andsetat25forallotherquantities,asusedinENSDF),valuesanduncertaintieswereroundedoffaccordingly(seeex-amplesinthe'Explanationoftable').
Inafewcases,thatweredeemedessentialfortraceabilitypurposes(e.
g.
iso-topicabundances),theoriginal(unrounded)valueisalsoprovidedintheassociatedcomment.
2.
1MassexcessInNUBASE2012themassexcessvalues(inkeV),de-nedasbeingdifferencesbetweentheatomicmass(inmassunits)andthemassnumber,togetherwiththeironestandarddeviationuncertainty,aretakenfromthemassta-blesoftheAME2012evaluation(inthethirdpartofthisissue,seep.
1608).
Ingeneral,knowledgeofmassescanprovidevaluableinformationondecaymodes,andinparticularonparticle-decayinstability,orbeta-delayedparticle-decay,fornu-cleifarfromthelineofstability.
SuchinformationisusedinNUBASE2012,andcanbeseen,forexample,in10He,39Sc,62As,or63As.
Insomecases,theclaimedobserva-tionsofdecaymodeswererejectedwhenitwasfoundthattheywerenotallowedthroughsimpleenergetics.
Fig.
1isacomplementofthemaintable,anddisplaysthemassprecisions,inacolor-codedchart,asafunctionofNandZ.
1160ChinesePhysicsC(HEP&NP)Vol.
36Figure1:Chartofthenuclidesdisplayingtheaccuracy'u'ofmasses(createdbyNUCLEUS-AMDC).
No.
12G.
Audietal:TheNUBASE2012evaluationofnuclearproperties11612.
2IsomersIntheveryrstversionofNUBASEin1997[3],asim-pledenitionforexcitedisomers,asbeingexcitedstateswithahalf-lifelongerthan1millisecond,wasadopted.
Allβ-decayingstateswereincludedinthiscategory,sincetheyhavealowerhalf-lifelimitof1millisecond(theshortest-livedknownβ-decayingnuclideis35Nawithahalf-lifeof1.
5millisecond).
However,alreadyatthattime,itwasnoticedthatsuchadenitionhadseveraldrawbacks,particularlyforneutron-decientalpha-andproton-decayingnuclides,wheremuchshorter-livedstateswereknowntoexist.
Moreover,severalcasesareknownwhereisomerswithhalf-livesfarbelow1millisecondsur-vivelongerthanthegroundstateitself(e.
g.
216Fr).
InNUBASE2003,thedenitionofisomerswasex-tendedtoincludeexcitedstateswithhalf-liveslongerthan100ns,andinthisneweditionallsuchstatesarenowin-cluded.
Themainreasonsforthischangeweretoinclude:a)allshorter-livedproton-andalpha-decayingstatesob-servedinmanyneutron-decientnuclei,b)short-livedisomersthatmaybedetectedinmass-spectrometryexperimentsperformedatacceleratorfacil-itiesfollowingtheimmediatedetectionoftheproducednuclei,andc)allpossibleisomersthatmaybedetectedinsuchexper-imentsinthefuture.
InNUBASE2012,isomersaregiveninorderofin-creasingexcitationenergy,andidentiedbyappendingtheletters'm','n','p','q',or'r'tothenuclidename,e.
g.
90Nbforthegroundstate,90Nbmfortherstexcitedisomer,90Nbnforthesecondone,and90Nbp,90Nbq,and90Nbrforthethird,fourthandfthones,respectively.
Inonlytwoinstances,179Taand214Ra,asixthisomerhadtobeincluded.
Theywerelabeledprovisionallywiththeletter'x'.
Theexcitationenergyofagivenisomercanbede-terminedusingdifferentexperimentalmethods,which,ingeneral,belongtothecategoryofeitherinternalorexter-nalrelations.
Atypicalinternalrelationisviatheγ-rayde-cayenergy,oracombinationofsuchγ-rayenergies.
ThemostaccuratevaluesfortheexcitationenergiesofisomersthatarededucedbythisapproachcanbefoundinENSDF,wherealeast-squaresttingprocedureisappliedtoallγraysalongthedecaypathofaparticularisomer.
However,whennosuchinternalrelationscanbeestablished,thentherelationtoothernuclides(externalrelations)canbeusedtodeducethemass(orenergy)differencebetweenexcitedandgroundstateisomers.
Inallsuchcases,themostaccuratevaluescanonlybederivedusingtheAMEevaluationprocedure.
ThevaluesarethereforetakenfromAME2012.
Theorigin(themethodusedtoestablishtheexternalrelation)ofeachisomerdataelementisthenin-dicatedbyatwo-lettercode,nexttotheisomerexcita-tionenergy,intheNUBASE2012table(seetheExplana-tionofTableI,p.
1176).
Forinternalrelations,theorigineldisleftblankandthenumericalvaluesaretakeneitherfromENSDForfromliteratureupdates.
Inthelattercase,aleast-squaresttothemeasuredγ-raydecayenergiesfromcomplexlevelschemeswasapplied,inaccordancewiththecurrentENSDFpolicies.
Aninterestingexampleistheprotondecayof167Ir,studiedusingaparent-daughtercorrelationtechnique[1997Da07],wheretheexcitationenergyoftheisomerwasdeterminedasEx=175.
3(2.
2)keV.
Thisinformationisdisplayedbythe'p'symbolintheorigineld.
Inad-dition,recentα-decaystudiesofproton-richnuclidesus-ingaspatialandtimecorrelationtechniquewithhighly-segmentedsiliconstripdetectorsnotonlyshowedthatanumberofαlinesassignedearliertogroundstatesbelonginrealitytoisomers,buttheyalsodeterminedvaluesfortheirexcitationenergies.
Anotherexampleis181Pb,wheretheα-decayhalf-lifethatwaspreviouslyassignedto181Pbmisnowasso-ciatedwiththegroundstate[1996To01].
Morerecentwork[2005Ca.
A,2005Ca43,2009An20]establishedthatthemainαlinefeedsthe77keVexcitedstatein177Hg,andsubsequentlydecaystothegroundstateviaγ-rayemission.
Italsohappensthatconnectionsbetweenexcitedandgroundstateisomerscanbeobtainedbybothinternalre-lationsandone,ormore,externalrelationswithcompara-bleaccuracies.
AllrelationsarethencombinedwithintheAME2012databyaddinganequationthatrelatestheex-citationenergyobtainedfromENSDF(orfromliterature),sothattheAME2012derivesthebestcombinationofalldata.
Forexample,theAME2012derivesthemassof178Lumat66%fromEx(IT)=120(3)keV[1993Bu02]andat34%from176Lu(t,p)178Lum=4482(5)keV[1981Gi01].
Theadjustedexcitationenergyisthus123.
8(2.
6)keV.
Insomecasesexcitationenergiesknownfrominternalrelationsareessentialinordertodeterminethemassofthegroundstate.
ThosevaluesarelabeledintheNUBASEtablewith'IT'intheorigineld.
TheyareenteredasanequationinAME2012sothatthegroundstatemasscanbederived(e.
g.
72Znm,197Pbm,or234Pam).
Similarly,whentheprecisionoftheexcitationenergyisnotmuchhigherthanthatdeducedfromtheenergyrelationtoanothernu-clide,theinternalrelationisthenaddedtotheAME2012dataset,inordertousethisaccuracy(e.
g.
181Hgmor185Tlm).
Aninterestingcaseisthemassandexcitationen-ergyofthesecondexcitedisomerof186Tl(186Tln),whereonlyitsmassisexperimentallyknownfromaPenningtrap(ISOLTRAP)measurement[2012Bo.
A].
However,thewell1162ChinesePhysicsC(HEP&NP)Vol.
36knowntransitionfrom186Tlnto186Tlmallowstodeter-minenotonlythemassofthelatterisomer,butalsotheexcitationenergyoftheα-decayingisomerintheparentnuclide,190Bim.
Whentheexistenceofanisomerisunderdiscussion,itisaggedwith'EU'("existenceuncertain")intheori-gineld(e.
g.
73Znn).
Acommentisgenerallyaddedtoindicatewhythisexistenceisquestioned,orwherethismatterisdiscussedinmoredetail.
Dependingonthede-greeofcondenceintheexistenceofaparticularstate,themassexcessandexcitationenergyvaluescanbegivenoromittedintheNUBASEtable(e.
g.
138Pmn).
Inthelattercase,thelabel"nonexistent"appearsintheplaceoftheexcitationenergyeld.
Whenaparticularisomerwasinitiallyreportedas"discovered",butlateritwasprovedtobeanerror,itisaggedwith'RN'intheorigineld,indicating"reported,nonexistent"(e.
g.
248Esm).
Insuchcases,nomassexcessorexcitationenergyvaluesaregiven,and,similarlytothe'EU'choiceabove,a"nonexistent"labelisadded.
Note:theuseofthetwoags,'EU'and'RN',wasex-tendedtocaseswherethediscoveryofanuclideisques-tioned(e.
g.
260Fmor289Lv).
However,anestimateforthegroundstatemass,derivedfromtrendsinthemasssurface(TMS),isalwaysgiveninAME2012andNUBASE2012.
Inseveralinstances,lowerandhigherlimitsfortheexcitationenergyofaparticularisomerarepresentedinENSDF.
ThepolicyofNUBASE2012isthatauniformdistributionofprobabilitiesisassumed,whichyieldsamid-rangevalueanda1σuncertaintycorrespondintto29%oftherange(seeAppendixBoftheAME2012,PartI,p.
1326,foracompletedescriptionofthisproce-dure).
Forexample,theexcitationenergyofthe162TmmisomerisknownfromENSDFtobeabovethe66.
90keVlevel.
However,thereisalsosolidexperimentalevidencethatitisbelowthe192keVlevel,andsothisinforma-tionispresented(afterroundingoff)asEx=130(40)keVinNUBASE2012.
Whensuchavalueisbasedontheo-reticalconsiderations,orfromTNN,theresultingExisconsideredasanon-experimentalquantityandthevalueisconsequentlyaggedwiththe'#'symbol.
Incaseswheretheuncertaintyoftheexcitationen-ergy,σ,isrelativelylargeascomparedtotheExvalue,theassignmentofthelevelasagroundorisomericstateisuncertain.
Ifσ>Ex/2,a''agisaddedintheNUBASE2012table.
TheorderingofseveralgroundandexcitedisomericstateswerereversedascomparedtotherecommendationsinENSDF.
Thesecasesareaggedwiththe'&'sym-bolintheNUBASE2012table.
Inseveralotherinstances,evidencewasfoundforstateslocatedbelowtheadoptedgroundstateinENSDF.
Therearealsocaseswherethetrendsinneighboringnuclides,withthesameparitiesinNandZ,stronglysuggestthatsuchalowerstateshouldexist.
SuchresultswereaddedintheNUBASE2012tableandareeasilylocated,astheyareaggedwiththe'&'symbol.
Inagrowingnumberofcases,newexperimen-talinformationonmassesledtoareversaloftheorderingbetweenpreviouslyassignedgroundandexcitedisomericstates.
ThankstothecouplingoftheNUBASE2012andAME2012evaluations,allchangesintheorderingofnu-clearlevelshavebeencarefullysynchronized.
Finally,therearecaseswheredataexistontheorderoftheisomers,e.
g.
ifoneofthemisknowntodecayintotheotherone,oriftheGallagher-Moszkowskirule[7]forrelativepositionsofcombinationspointsstronglytooneofthetwoasbeingtheground-state.
Detaileddis-cussionscanbefoundinRef.
[8].
Onlyfor256Md,wedis-coveredtoolate,relativetothepublicationdeadline,thattheadoptedorderinghadtobereversed,weonlyaddedaremarkto256Mdm(seep.
1278).
2.
2.
aIsobaricanalogstates(IAS)Therecentrevivedinterestinisomericstateshasnat-urallyledtotakingacloserlookatthehistoricallyverypopularsubjectofisobaricanalogstates(seeAME2012,PartI,Section6.
4,p.
1314).
InNUBASE2012wehaveincludedmainlytheT=3/2toT=3experimentallyob-servedIAS.
Thesestatesaregenerallylabelledwithiorjsuperscripts,formembersofsuccessivelyhighermulti-plets.
Somenuclidesbelongsimultaneouslytoseveralcate-gories,forexample,theymaybeintheirgroundstatebuttheymayalsobetheIASofsomeothergroundstatenu-cleus,asisthegeneralcaseforgroundstatemirrornuclei.
Here,theIASlabelisnotpresentsincethesenuclidesarealreadynaturallyincludedinthedatabase.
Anotherexcep-tionisthesetofN=ZT=1odd-oddgroundstatenu-clides,accessibleviasuper-allowedbetadecay,andwhicharealsoalreadypartoftheoriginaldatasetofgroundstatemasses.
Theyare:34Cl17,42Sc21,46V23,50Mn25,54Co27,62Ga31and70Br35.
ThereadermightnotethatonlytheZ=29andZ=33donotshowupinthisseries,sincetheirgroundstatesareT=0,asexpectedfromtheory.
Finally,thereareeightexcitedisomers,16Nm,26Alm34Clm,38Km,46Vm,50Mnm,54Comand72GamwhicharealsoIAS.
Insuchcases,theisomerlabels('m','n',.
.
.
)areusedpref-erentiallyovertheIASlabels.
Herewenotewithinterestthatveofthemhaveexperimentalexcitationenergiesde-termined,atleastpartly,bytheJYFLTRAP-Jyv¨askyl¨aPen-ningtrap(seeAME2012,PartI,Section6.
2,p.
1311).
InNUBASE2012thereareroughly180uniqueIASNo.
12G.
Audietal:TheNUBASE2012evaluationofnuclearproperties1163masses,ofwhich107areevaluatedintheAMEviaexter-nalrelations,and70casespreviouslyevaluatedthroughinternalrelationsandpublishedinENSDF.
Therearearemainingsevencaseswherenoclearexperimentaldataisavailable,andalthoughsomeIsobaricMultipletMassEquation(IMME)[9]andCoulombDisplacementEnergy(CDE)[10]calculationspointtoalikelyIASstate,theirexistencecannotyetbecertiedexperimentally(seeforexample56Zniandthediscussionin[2007Do17]).
TheisospinmultipletappartenancegiveninthetableisthelogicalIASmultipletvalue,andhasnotnecessarilybeendeducedexperimentally.
2.
3Half-lifeForsomelightnuclei,thehalf-life(T1/2)isdeducedfromthetotallevelwidth(Γcm)bytheequationΓcmT1/2h*ln2:T1/2(s)4.
5621022/Γcm(MeV).
Thefollowingunitsareusedforaconvenientdis-play:seconds(s)anditssub-units,minutes(m),hours(h),days(d)andyears(y)anditssub-units.
Conversionbe-tweenyearsandsecondsordayscouldfollowvariousdef-initions:Julianyear,Gregorianyear,tropicalyear1900,epoch2000,.
.
.
,differingonlyslightlyfromeachother.
Axedvalueof:1y=31556926sor1y=365.
2422dwasadoptedinNUBASE2012.
Asymmetricuncertaintiesforhalf-lives,T1/2+ab,areoftenpresentedintheliterature.
However,inorderforthesevaluestobeusedinpracticalapplications,theyneedtobesymmetrized.
Aroughsymmetrizationprocedurewasusedearlier(seeAME1995)wherethecentralvaluewastakenasthemid-valuebetweentheupperandlower1σ-equivalentlimits,T1/2+(ab)/2,andtheuncertaintywasdenedtobetheaverageofthetwouncertainties,(a+b)/2.
Astrictstatisticalderivation(seeAppendixA)showsthatabetterapproximationforthecentralvaluecanbeobtainedbyusingT1/2+0.
64*(ab).
Theexactexpressionforasymmetricuncertainties,adoptedinNUBASE2012,ispresentedinAppendixA.
Whentwoormoreindependentmeasurementswerereportedintheliterature,thecorrespondingvalueswereweightedbytheirreportedprecisionsandthenaveraged.
Whiledoingthis,theNORMALIZEDCHI,χn(or'consis-tencyfactor'or'Birgeratio'),asdenedinAME2012,PartI,Section5.
2,p.
1306)isconsidered.
Onlywhenχnislargerthan2.
5,departurefromthestatisticalresultisal-lowed,andtheexternaluncertaintyfortheaverageresultisadopted.
ThisfollowsthesamepolicythatisdiscussedandadoptedinAME2012,PartI,Section5.
4,p.
1307.
Veryrarely,whenχnissolargethatallindividualun-certaintiescanbeconsideredasirrelevant,thearithmetic(unweighed)averageisadoptedandthecorrespondingun-certaintyisbasedonthedispersionofthevalues.
Insuchcases,thelistofvaluesthatwereaveraged,togetherwiththeχnvalue(whenrelevant)andthereasonforthischoice,aregivenintheNUBASE2012table.
Whencontradic-tory(conicting)resultswereidentiedintheliterature,agreatdealofattentionwasfocusedonestablishingthereasonforsuchdiscrepancies,andconsequently,torejectthecorrespondingbaddata.
Thereasonsforsuchdeci-sionsaregivenascommentsintheNUBASE2012table.
Inexperimentswhereextremelyrareeventsarede-tectedandwheretheresultsareveryasymmetric(e.
g.
studiesofsuper-heavynuclei),thehalf-lifevaluesre-portedindifferentpublicationswerenotdirectlyaver-aged.
Instead,whentheinformationpresentedintheliter-aturewassufcient(e.
g.
264Hsor269Hs),thedelaytimesassociatedwiththeindividualeventswerecombined,asprescribedbySchmidtet.
al.
[1984Sc13].
Someexperimentalresultsarereportedintheliteratureasarangeofvalueswithamostprobablelowerandupperlimit.
Thesearetreated,asinthecaseofisomerexcitationenergies(seeprecedingpage),asauniformdistributionofprobabilities.
IntheNUBASE2012table,anupperoralowerlimitonthehalf-lifevalueisgivenfornuclidesidentiedusingatime-of-ighttechnique.
Thefollowingpolicieswereconsidered:i)Forobservednuclides,thelowerlimitforthehalf-lifeisgiveninplaceoftheuncertainty(see44Si,p.
1188).
How-ever,suchlimitsshouldbeusedwithcaution,sinceitmaybefarbelowtheactualhalf-life.
Inordertoavoidconfu-sion,asomewhatmorerealisticestimate(aggedwith#),derivedfromtrendsinthehalf-lifevaluesofneighboringnuclides(TNN),isalsogiven.
ii)Fornuclidesthatweresoughtfor,butnotobserved,theupperlimitisgiveninplaceoftheactualhalf-lifeuncer-tainty.
UpperlimitsforadozenofundetectednuclideswereevaluatedbyF.
Pougheon[1993Po.
A],basedonthetime-of-ightoftheexperimentalsetupandtheproduc-tionyieldsexpectedfromTNN(e.
g.
21Al).
Whengroundstatehalf-livesfornuclideswiththesameparitiesinZandNarefoundtovarysmoothly(seeFig.
2),interpolationorextrapolationprocedureisusedtoobtainreasonableestimatesforunknownnuclei.
1164ChinesePhysicsC(HEP&NP)Vol.
36Figure2:Chartofthenuclidesdisplayinghalf-lives(createdbyNUCLEUS-AMDC).
No.
12G.
Audietal:TheNUBASE2012evaluationofnuclearproperties1165Figure3:Chartofthenuclidesdisplayingspinsandparities.
Onlytheodd-Zeven-Nnuclidesareshown(createdbyNUCLEUS-AMDC).
1166ChinesePhysicsC(HEP&NP)Vol.
36Figure4:Chartofthenuclidesdisplayingspinsandparities.
Onlytheeven-Zodd-Nnuclidesareshown(createdbyNUCLEUS-AMDC).
No.
12G.
Audietal:TheNUBASE2012evaluationofnuclearproperties1167Figure5:Chartofthenuclidesdisplayingspinsandparities.
Onlytheodd-Zodd-Nnuclidesareshown(createdbyNUCLEUS-AMDC).
1168ChinesePhysicsC(HEP&NP)Vol.
36Figure6:Chartofthenuclidesdisplayingdecaymodes(createdbyNUCLEUS-AMDC).
No.
12G.
Audietal:TheNUBASE2012evaluationofnuclearproperties1169Figure7:Chartofthenuclidesdisplayingtheyearsofdiscovery(createdbyNUCLEUS-AMDC).
1170ChinesePhysicsC(HEP&NP)Vol.
362.
4SpinandparitySimilarlytoENSDF,spinandparityvaluesarepre-sentedwithandwithoutparentheses,basedonstrongandweakassignmentarguments,respectively(seetheintro-ductorypagesofRef.
[11]).
Unfortunately,thelatterincludeestimatesfromtheoryorfromTNN(trendsinneighboringnuclides).
InNUBASE2012,followingourpolicyofmakingacleardistinctionbetweenexperimentalandnon-experimentalinformation,parenthesesareusediftheso-called"weak"argumentisbasedonexperimen-talobservations,whilethesymbol'#'isusedfortheothercases.
Itshouldalsobenotedthatdespitethewelldenedevaluationpolicies[11],thereareanumberofinconsis-tenciesinENSDFregardingthespinsandparitiesforex-citedstates.
Often,proposedassignmentsreecttheinter-pretationofaparticularENSDFevaluator,ratherthanthatofrmpolicyrules.
Asaresult,assignmentstosimilarstatesinneighboringnucleiareputinparenthesisbyoneevaluator,butnotbyother,althoughsimilarexperimentalinformationisavailable.
Wehavetriedtouseaconsistentapproachinassigningspinsandparitiestoexcitedstates,butthesurveyisstillfarfromcompleteandthereadermaystillndinconsistencies.
Theauthorswouldgratefullyap-preciatefeedbackfromusersonsuchcases,inordertoimprovefutureversionsofNUBASE.
Ifspinsandparitiesarenotdeterminedexperimentally,theycanbeestimatedfromtrendsinneighboringnuclides(TNN)withthesameparitiesinNandZ.
Although,thisisfrequentlythecaseforodd-Anuclides(seeFig.
3andFig.
4),suchtrendsarealsosometimesvalidforodd–oddisotopes,especiallyintheneighborhoodofmagicnum-bers,ascanbeseeninFig.
5.
Inallcases,theestimatedvaluesareaggedwiththe'#'symbol.
ThereviewofnuclearradiiandmomentsofOtten[1989Ot.
A],inwhichthespinswerecompiled,wasusedtocheckandcompletethespinvaluesinNUBASE2012.
Noteaddedinproof:Anoveltechniquebasedonacondensed-matterdeviceallowstodetermineabsolutevaluesforthespin[2012Vi.
1],similarlytothehypernemethod.
Thistechniquewasappliedto159Tbandcon-rmedthewellknownspinof3/2.
2.
5DecaymodesandtheirintensitiesThemostimportantpolicyinassemblingtheinfor-mationforthedecaymodeswastoestablishaverycleardistinctionbetweenadecaymodethatisenergeticallyal-lowed,butnotexperimentallyobservedyet(representedbyaquestionmarkalone,whichthusreferstothede-caymodeitself),andadecaymodewhichisactuallyob-served,butforwhichtheintensitycouldnotbedetermined(representedby'=',thequestionmarkreferringheretothequantityaftertheequalsign).
SimilarlytoENSDF,nocorrectionsweremadetonor-malizetheprimaryintensitiesto100%.
Inadditiontoapplyingdirectupdatesfromthelitera-ture,partialevaluationscompletedbyotherauthorswerealsoconsidered,whichareproperlyreferenced.
Thosecasesarementionedbelow,whendiscussingsomepartic-ulardecaymodes.
β+decayInthecourseofthisworksomedenitionsandno-tationsforβ+decaywererened,inordertoprovideaclearerpresentationoftheavailableinformation.
Specif-ically,β+denotesthedecayprocessthatincludesbothelectroncapture,labeledε,anddecaybypositronemis-sion,labelede+.
Onecanthensymbolicallywrite:β+=ε+e+.
Itiswellknownthatforanavailableenergybe-low1022keV,onlyelectroncapture,ε,isallowed,whilstabovethatvaluethetwoprocessesareincompetition.
Remark:thisnotationisnotthesameastheoneusedimplicitlyinENSDF,wherethecombinationofbothmodesisdenoted"ε+β+".
Whenbothmodescompete,theseparatedintensitiesarenotalwaysexperimentallyavailableandfrequentlytheyarededucedfrommodelcalculations,asisthepolicyinENSDF.
IncontinuationofoneofthegeneralNUBASEpolicies,inwhichonlyexperimentalinformationisusedwheneverpossible,itwasdecidednottoretainthesepa-ratedvaluescalculatedinENSDF(whicharescarceandnotalwaysupdated).
Onlyinafewveryspeciccases,wherethedistinctionisofimportance,suchasinthecaseofrareorextremelyrareprocesses(e.
g.
91Nb,54Mn,119Tem),separatevaluesaregiven.
Bythesametoken,bothelectroncapture-delayeds-sion(εSF)andpositron-delayedssion(e+SF)aregivenwiththesamesymbolβ+SF.
Double-βdecayInthecourseofthisworkitwasfoundthathalf-livesfordoubleβ-decayingnuclideswerenotalwaysconsis-tentlygiveninENSDF.
Sincethetwo-neutrinogs-gstran-sitionisthedominantdecayprocess(oneexceptionmaybe98Mo,forwhichtheneutrinolessdecayispredictedtobefaster,see[2002Tr04]),onlythosehalf-lifevaluesortheirupper-limitswerepresentedintheNUBASE2012ta-ble.
Noattemptwasmadetoconvertthehalf-lifevaluestothesamestatisticalcondencelevel(CL)upperlimitresultsgivenbydifferentauthors.
TheexcellentcompilationofTretyakandZdesenko[2002Tr04]wasofgreathelpincoveringsuchdecays.
No.
12G.
Audietal:TheNUBASE2012evaluationofnuclearproperties1171β-delayedparticledecaysFordelayedparticledecays,intensityrelationshavetobecarefullyconsidered.
Bydenition,theintensityofadecaymodeisthepercentageofdecayingparentnu-cleiinthatmode.
Buttraditionally,theintensitiesofthepureβdecayaresummedwiththoseofthedelayedpar-ticlesinordertogiveanintensitythatisassignedtothepureβdecay.
Forexample,ifthe(A,Z)nuclidehasadecaydescribedtraditionallyby'β=100;βn=20',thismeansthatfor100decaysoftheparent,80(A,Z+1)and20(A–1,Z+1)daughternucleiareproducedandthat100electronsand20delayedneutronsareemitted.
Astrictnotationinthiscase,usingthedenitionabove,wouldbe'β=80;βn=20'.
However,inthepresentwork,ithasbeendecidedtofollowthetraditionalnotation,andsowewrite:'β=100;βn=20'.
Thisalsoholdsformorecomplexdelayedemis-sions.
Forexample,adecaydescribedby:'β=100;βn=30;β2n=20;βα=10'correspondstotheemis-sionof100electrons,(30+2*20=70)delayed-neutronsand10delayed-αparticles;andintermsofresidualnu-clides,to40(A,Z+1),30(A–1,Z+1),20(A–2,Z+1)and10(A–4,Z–1).
Moregenerally,thenumberofemittedneu-tronsper100decays,Pn,canbewrittenas:Pn=∑ii*βin;andsimilarexpressionscanbewrittenforαandpro-tonemission.
Thenumberofresidualdaughternuclides(A,Z+1)populatedviaβdecayisthen:β∑iβin∑jβjα.
.
.
Anotherspecialremarkconcernstheintensityofapar-ticularβ-delayedmode.
Ingeneral,theprimary(parent)βdecaypopulatesseveralexcitedstatesinthedaugh-ternuclide,whichcanfurtherdecaybyparticleemis-sion.
However,inacasewherethegroundstateofthedaughternuclidedecaysalsobythesameparticleemis-sion,someauthorsincludeditsdecayinthevalueforthecorrespondingβ-delayedintensity.
IthasbeendecidedtonotusesuchanapproachinNUBASE2012fortwomainreasons.
First,theenergiesofdelayedparticlesemittedfromexcitedstatesaregenerallymuchhigherthanthoseemittedfromthegroundstate,henceimplyingdifferentsubsequentprocesses.
Secondly,sincethecharacteristicdecaytimesfromexcitedstatesarerelatedtotheparent,whereasdecaysfromthedaughter'sgroundstatearecon-nectedtothedaughternuclideitself.
Forexample9Cde-caysviaβ+withanintensityof100%ofwhich12%and11%populatetwoexcitedproton-emittingstatesin9B,and17%goestoanα-emittingstate.
Thus,β+p=23%andβ+α=17%,fromwhichtheuseroftheNUBASE2012tablecanderivea60%directfeedingofthegroundstateof9B.
Inaslightlydifferentexample,8Bdecaystoonlytwoexcitedstatesin8Be,whichinturndecaybyα-andγ-rayemissions,butnottothe8Begroundstate.
Thus,onemaywriteβ+=100%andβ+α=100%,thedifferenceofwhichleaves0%forthefeedingofthedaughter'sgroundstate.
Finally,theusersshouldbeawarethatthepercentagesgivenintheNUBASE2012tablearerelatedto100par-entdecayingnuclei,ratherthantotheprimarybeta-decayfraction.
Anillustrativeexampleisgivenbythedecayof228Np,forwhichthedelayed-ssionprobabilityisgivenintheoriginalpaperas0.
020(9)%[1994Kr13],butthisvalueisrelativetotheεprocess,whichhasanintensityof59(7)%.
Thus,therenormalizeddelayed-ssionintensityis0.
020(9)%*0.
59(7)=0.
012(6)%ofthetotaldecayintensity.
Incompilingthedatafordelayedprotonandαac-tivities,theremarkableworkofHardyandHagberg[1989Ha.
A],inwhichthecorrespondingphysicswasre-viewedanddiscussedindetail,wasconsulted.
ThereviewofHonkanen,¨Ayst¨oandEskola[12]ondelayedprotondecayshasalsobeenused.
Similarly,thereviewofdelayedneutronemissionbyHansenandJonson[13]wascarefullyexaminedandusedintheNUBASE2012table,togetherwiththeevaluationofRudstam,AleklettandSihver[1993Ru01].
2.
6IsotopicabundancesIsotopicabundancesaretakenfromthecompilationofM.
BerglundandM.
E.
Wieser[2011Be53]andthevaluesarelistedinthedecayeldwiththesymbolIS.
ThesedataaregivenintheNUBASE2012tableaspresentedorigi-nallyin[2011Be53],andsointhiscasetheroundingoffpolicywasnotapplied.
2.
7ReferencesTheyearofthearchivalleforthenuclidesevaluatedinENSDFisindicated,otherwisethisentryisleftblank.
ReferencesforalloftheexperimentalupdatesaregivenbytheNSRkeynumberstyle[5],andarelistedattheendofthisissue(p.
1863).
Theyarefollowedbyone,twoorthreeone-lettercodeswhichspecifytheaddedormodiedphysicalquantities(seetheExplanationofTa-bleI,p.
1176).
Incaseswheremorethanonereferenceisneededtodescribeaparticularupdate,theyaregivenasaremark.
Noreferenceisgivenforestimatedvalues.
Theinitialsofthepresentauthors,AHW,FGK,GAU,JBL,MMC,WGM,areusedasreferencekeysincaseswhereitmaynotbepreciselyclearthatthere-interpretationofdataweremadebythepresentauthors.
1172ChinesePhysicsC(HEP&NP)Vol.
363UpdatingprocedureIngeneral,NUBASEisupdatedviatworoutes:fromENSDFaftereachnewA-chainevaluationispublished(orfromthebi-annualreleases),anddirectlyfromtheliter-ature.
Dataavailableinthe"UnevaluatedNuclearDataList"(XUNDL)arealsoregularilyconsulted[14].
ENSDFlesareretrievedfromNNDCusingtheon-lineservice[2].
Theprograms,originallydevelopedbyO.
Bersillonandoneofthepresentauthors(JB)[15],areusedtosuccessively:checkthateachZintheA-chainhasan'adoptedlevels'dataset;ifnot,acorrespondingdatasetisgeneratedfromthe'decay'or'reaction'dataset,extractthe'adoptedlevels'datasetsfromENSDF,extracttherequiredphysicalquantitiesfromthesedatasets,andconvertthemintotheNUBASEformat.
TheprocesseddataareusedtomanuallyupdatethepreviousversionofNUBASE.
Thisstepisrepeatedinde-pendentlybytwo,andsometimesbythree,ofthepresentauthors,andcross-checkeduntilcompleteagreementisreached.
ENSDFisupdatedgenerallybyA-chainsandmorere-centlyalsobyindividualnuclides.
Itscontents,however,areverylarge,sinceitencompassesallofthecomplexnuclearstructureanddecayproperties.
Thisisahugeef-fort,anditisnotsurprisingthatoccasionallysomeolderdata(inparticularannualreports,conferenceproceedings,andtheses)aremissing,andthatsomerecentdatahavenotyetbeenincluded.
Whensuchcaseswererevealed,theywereanalyzedandevaluated,asdescribedabove,andtheNUBASE2012databasewasupdatedaccordingly.
Inprinciple,thesenewdatawillbeincludedinfutureENSDFevaluationsandthecorrespondingreferencescanthenberemovedfromfutureNUBASEdistributions.
Un-fortunately,ithasbeenobservedinthepastthatsuchaprocedurewasnotalwaysadheredto.
Infact,insomenewerENSDFles,quotationstoearlierNUBASEpub-licationswerefound,whichleadstoanindesirableloopresultinginnon-traceableinformation.
4DistributionanddisplaysofNUBASE2012Thefullcontentsofthepresentevaluationisavail-ableon-lineatthewebsiteoftheAtomicMassDataCenter(AMDC)[16].
AnelectronicASCIIlefortheNUBASE2012tableisalsodistributedbytheAMDCweb-site.
Theseleswillnotbeupdated,toallowstablerefer-encedataforvariouscalculations.
Anyworkusingthoselesshouldmakereferencetothepresentpaperandnottotheelectronicles.
ThecontentsofNUBASE2012canbedisplayedbyastand-alonePC-programcalled"NUCLEUS"[17],whichcanalsobedownloadedfromtheAMDCwebsite.
ItwillbeupdatedonregularbasistoallowuserstocheckforthelatestavailableinformationinNUBASEdatabase.
5ConclusionsThe'horizontal'evaluateddatabase,NUBASE2012,whichcontainstherecommendedvaluesforthemainpropertiesofallknownnuclidesintheirgroundandex-citedisomericstates,wasdeveloped.
Thishasbeencom-pletedforthersttimebytheinclusionofallavail-ableIASdata.
Thesedataoriginatefromacompila-tionoftwoevaluateddatabases:ENSDF,followedbyacriticalassessmentofthevalidityandcompletenessofthosedata,includingnewupdatesfromtheliterature,andAME2012.
ThemainrequirementindevelopingNUBASE2012wastocoverascompletelyaspossiblealltheavailableexperimentaldataandtoprovideproperref-erencestothem,especiallyforcasesthatarenotalreadyincludedinENSDF.
Thistraceabilityallowsanyusertochecktherecommendeddataand,ifnecessary,tounder-takeare-evaluation.
Asaresultofthis'horizontal'work,betterhomogene-ityinhandlingandpresentationofalldatawasobtainedforallknownnuclides.
Furthermore,isomericassign-mentsandtheirexcitationenergieswerereconsideredonarmerbasisandtheirdataimproved.
ItisexpectedtofollowupthisthirdversionofNUBASEwithimprovedtreatmentsinthefuture.
Afore-seeableimplementationwouldbetoprovidethemainα,γ,conversionelectronsandX-raylinesaccompanyingparticulardecays,aswellastoincludeevenshorter-livedexcitednuclearisomers.
NUBASEcouldalsobeextendedtoothernuclearproperties,suchasenergiesoftherst2+statesineven-evennuclides,radii,moments,etc.
AnewfeaturethatwasimplementedinthepresentversionofNUBASEisthecompilationoftheyearofdis-coveryforeachnuclideinitsgroundorisomericstate.
Fortheformer,recentevaluationsperformedbyagroupatMichiganStateUniversity[18]wereadopted.
Simi-larcriteriawasusedwhenassigningtheyearofdiscoveryforisomericstates.
However,wewouldliketomaketheusersawarethatthisfeatureforexcitedisomersisnotfullycheckedandthattherearestillsomecasesmissing.
6AcknowledgmentsWewishtothankmanycolleagueswhoansweredourquestionsabouttheirexperimentsandthosewhosentuspreprintsoftheirpapers.
WeappreciatethehelpprovidedbyJ.
K.
Tuliinsolvingsomeofthepuzzlesweencoun-teredinENSDF.
Continuousinterest,discussions,sug-No.
12G.
Audietal:TheNUBASE2012evaluationofnuclearproperties1173gestionsandencouragementsfromK.
Blaum,D.
Lunney,G.
Savard,ZhangYuhu,ZhongzhouRen,andCh.
Schei-denbergerwerehighlyappreciated.
SpecialthankstoDar-ianJenkinsforhisinterestinourworkanddiscussionsaboutthe"YearofDiscovery"thatwenallyaddedtoNUBASE,andtoNicolasSavardforhelpinginitsimplen-tation.
ThisworkwasperformedintheframeandwiththehelpoftheFrench-ChinesecollaborationunderthePICSprogramme.
M.
W.
acknowledgessupportfromtheMax-PlanckSociety,fromtheInternationalAtomicEnergyAgency,IAEA-ViennaandfromtheNationalNaturalSci-enceFoundationofChinathroughGrantNo.
10925526,11035007.
TheworkatANLwassupportedbytheU.
S.
DepartmentofEnergy,OfceofNuclearPhysics,underContractNo.
DE-AC02-06CH1357.
Figure8:Simulatedasymmetricprobabilitydensityfunction(heavysolidline)andtheequivalentsymmetricone(dashedline).
AppendixASymmetrizationofasymmetricuncertaintiesExperimentaldataaresometimesgivenwithasymmet-ricuncertainties,X+ab.
Ifthesedataaretobeusedinsomepracticalapplications,theiruncertaintiesmayneedtobesymmetrized.
Asimplemethod(Method1)thatwasde-velopedearlier,usesthecentralvaluetobeinthemiddlebetweentheupperandlower1σ-equivalentlimitsX+(ab)/2,withtheuncertaintydenedtobetheaverageofthetwouncertainties(a+b)/2.
Analternativemethod(Method2)considerstheran-domvariablexassociatedwiththemeasuredquantity.
Forthisrandomvariable,oneassumesthattheprobabil-itydensityfunctionisanasymmetricnormaldistributionhavingamodal(mostprobable)valueofx=X,astandarddeviationbforxX(Fig.
8).
Thentheaveragevalueofthisdistributionisx=X+2/π(ab),withvarianceσ2=(12/π)(ab)2+ab.
(1)Themedianvaluemwhichdividesthedistributionintotwoequalareasisgiven,fora>b,byerfmX√2a=ab2a,(2)andbyasimilarexpressionforb>a.
Onecanthendenetheequivalentsymmetricnormaldistributionthathaveameanvalueequaltothemedianvaluemofthepreviousdistributionwithsamevarianceσ.
IftheshiftmXofthecentralvalueissmallcom-paredtoaorb,expression(2)canbewritten[19]:mXπ/8(ab)mX0.
6267(ab).
Inordertoallowforasmallnon-linearitythatappearsforhighervaluesofmX,therelationmX=0.
64(ab).
wasadoptedforMethod2.
TableAillustratestheresultsfrombothmethods.
InNUBASE2012,Method2isusedforthesymmetrizationofasymmetrichalf-livesanddecayintensities.
1174ChinesePhysicsC(HEP&NP)Vol.
36TableA.
Examplesoftwodifferenttreatmentsofasymmetrichalf-lifeuncertainties.
Method1istheclassicalmethod,usedpreviously,asintheAME1995.
Method2istheonedevelopedinNUBASE2003,describedinthisAppendix.
NuclideOriginalT1/2Method1Method254Zn3.
2+1.
8–0.
8ms3.
7±1.
33.
8±1.
380Cu170+110–50ms200±80208±8383Mo6+30–3ms20±1723±19100Kr7+11–3ms11±712±8115Mo51+79–19ms81±4989±53222U1.
0+1.
0–0.
4s1.
3±0.
71.
4±0.
7264Hs327+448–120s490±280540±300265Rf105+503–48s332±275400±320266Mt1.
01+0.
47–0.
24ms1.
1±0.
41.
2±0.
4267Db73+350–33m230±190280±220Referencesquotedinthetextas[1993Po.
A]or[2011Be53](NSRstyle)arelistedunder"ReferencesusedintheAME2012andtheNUBASE2012evaluations",p.
1863.
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1176ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012tableofnuclearanddecaypropertiesEXPLANATIONOFTABLEDataarepresentedingroupsorderedaccordingtoincreasingmassnumberA.
NuclideNuclidicname:massnumberA=N+Zandelementsymbol(forZ>109seeSection2).
Elementswithuppersufx'm','n','p','q','r'or'x'indicateassignmentstoexcitedisomericstates(denedashigherstateswithhalf-livesgreaterthan100ns).
Sufxes'p'and'q'alsoindicatenon-isomericlevels,butusedintheAME2012.
Sufx'r'alsoindicatesastatefromaprotonresonanceoccurringin(p,γ)reactions(e.
g.
28Sir).
Sufx'x'alsoappliestomixturesoflevels(withrelativeratioR,giveninthe'Half-life'column),e.
g.
occurringinspallationreactions(indicated'spmix'inthe'Jπ'column)orssion('fsmix').
MassexcessMassexcess[M(inu)A],inkeV,anditsonestandarddeviationuncertaintyasgiveninthe'AtomicMassEvaluation'(AME2012,inthesecondpartofthisvolume).
Rounding-offpolicy:incaseswherethefurthest-leftsignicantdigitintheerrorislargerthan3,valuesanderrorsarerounded-off,butnottomorethantensofkeV.
(Examples:2345.
67±2.
78→2345.
7±2.
8,2345.
67±4.
68→2346±5,but2346.
7±468.
2→2350±470).
#insteadofadecimalpoint:valueanduncertaintyarenotderivedonlyfromexperimentaldata,butatleastpartlywithestimatesfromTMS(seeAME2012).
ExcitationenergyForexcitedisomersonly:energydifference,inkeV,betweenlevelsadoptedashigherlevelisomerandgroundstateisomer,anditsonestandarddeviationuncertainty,asgiveninAME2012whenderivedfromtheAME,otherwiseasgivenbyENSDF.
Therounding-offpolicyisthesameasforthemassexcesses(seeabove).
#insteadofadecimalpoint:valueanduncertaintyderivedfromtrendsinneighboringnuclides.
Theexcitationenergyisfollowedbyitsorigincodewhenderivedfromamethodotherthanγ-rayspectrometry:MDmassdoubletRQreactionQ-valueADαenergydifferenceBDβenergydifferencep,2pone-,two-protondecayITcombinationofAMEandγ-raydataNmestimatedvaluederivedusingtheNilssonmodelWhentheexistenceofanisomerisquestionablethefollowingcodesareused:EUexistenceofisomerisunderdiscussion(e.
g.
73Znn).
Ifexistenceisstronglydoubted,noexcitationenergyandnomassaregiven.
Theyarereplacedbythemention"nonexistent"(e.
g.
138Pmn).
RNisomerhasbeenprovennottoexist(e.
g.
248Esm).
Excitationenergyandmassarereplacedbythemention"nonexistent".
Remark:codesEUandRNarealsousedwhenthediscoveryofanuclide(e.
g.
260Fmor289Lv)isquestioned.
Inthiscaseanestimatederivedfromtrendsinthemasssurfaceisalwaysgivenforthegroundstatemass.
Isomericassignment:iftheuncertaintyσontheexcitationenergyEisgreaterthanhalftheexcitationenergy(σ>E/2),thesequantitiesarefollowedbyanasterisk(e.
g.
130Inand130Inm).
&whentheorderingofthegroundstateisomerandtheexcitedisomerarereversedascomparedtoENSDF,anampersandsignisadded(e.
g.
102Yand102Ym).
No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1177Half-lifes=seconds;m=minutes;h=hours;d=days;y=years;1y=31556926sor365.
2422dadoptedvaluesforNUBASE(seetext)STABLE=stablenuclide,ornuclideforwhichnonitehalf-lifevaluehasbeenfound.
#valueestimatedfromtrendsinneighboringnuclideswiththesameZandNparities.
subunits:ms:103smillisecondky:103ykiloyears:106smicrosecondMy:106ymegayearns:109snanosecondGy:109ygigayearps:1012spicosecondTy:1012yterayearfs:1015sfemtosecondPy:1015ypetayearas:1018sattosecondEy:1018yexayearzs:1021szeptosecondZy:1021yzettayearys:1024syoctosecondYy:1024yyottayearR:Forisomericmixturesonly,itistheproductionratiooftheexcitedisomerstatetothegroundstateisomer.
JπSpinandparity:()uncertainspinand/orparity.
#valuesestimatedfromtrendsinneighboringnuclideswiththesameZandNparities.
highhighspin.
lowlowspin.
amsameJπasα-decayparentTIsopinmultipletforisobaricanalogstates(IAS).
Forisomericmixturesonly:mix(spmixandfsmixifobservedinspallationandssion,respec-tively).
EnsYearoftheENSDFlearchive(inordertoreducethewidthoftheTable,thetwocenturydigitsareomitted).
ReferenceReferencekeys:(inordertoreducethewidthoftheTable,thetwocenturydigitsareomitted.
However,attheendofthisvolumethefullreferencekey-numberisgiven,ie.
2010Cr02asopposedto10Cr02)10Cr02updatestoENSDFderivedfromaregularjournal.
ThesekeysaretakenfromNuclearDataSheets.
Wherenotyetavailable,thestyle12Ma.
1isprovisionallyadopted.
12Dr.
AupdatestoENSDFderivedfromanabstract,preprint,privatecommunication,confer-ence,thesisorannualreport.
AHW(orFGK,GAU,JBL,MMC,WGM),re-interpretationbyoneoftheevaluatorsofNUBASE.
Mirrordeducedfrommirrornuclideproperties.
ImmededucedfromIsobaricMultipletMassEquation.
Thereferencekey-numbersarefollowedbyone,twoorthreelettercodeswhichspeciestheaddedormodiedphysicalquantities:EfortheisomerexcitationenergyTforhalf-lifeJforspinand/orparityDfordecaymodeand/orintensityIforidenticationYearofforgroundstates[15]andforexcitedisomers(seetext).
discovery1178ChinesePhysicsC(HEP&NP)Vol.
36DecaymodesDecaymodesfollowedbytheirintensities(in%),andtheironestandarddeviationanduncertainties.
Thespecialnotation1.
8e–12standsfor1.
8*1012.
intensitiesTheuncertaintiesaregiven-onlyinthiseld-intheENSDF-style:α=25.
923standsforα=25.
9±2.
3%Theorderingisaccordingtodecreasingintensities.
αmeansαdecayisenergeticallyallowed.
α=meansαdecayhasbeenobservedbutnotyetquantied.
ααemissionp2pprotonemission2-protonemissionn2nneutronemission2-neutronemissionεelectroncapturee+positronemissionβ+β+decay(β+=ε+e+)ββdecay2βdoubleβdecay2β+doubleβ+decayβnβdelayedneutronemissionβ2nβdelayed2-neutronemissionβ+pβ+delayedprotonemissionβ+2pβ+delayed2-protonemissionβαβdelayedαemissionβ+αβ+delayedαemissionβdβdelayeddeuteronemissionITinternaltransitionSFspontaneousssionβ+SFβ+delayedssionβSFβdelayedssion24Neheavyclusteremission.
.
.
listiscontinuedinaremark,attheendoftheA-groupForlong-livednuclides:ISIsotopicabundance(from[2011Be53])AremarkonthecorrespondingnuclideisgivenbelowtheblockofdatacorrespondingtothesameA.
Remarks.
Fornuclidesmarkedwithanasteriskattheendoftheline,extracommentshavebeenadded.
TheyarecollectedingroupsattheendofeachblockofdatacorrespondingtothesameA.
Theystartwithalettercode,similartheonesfollowingthereferencekey-number,asgivenabove,indicatingtowhichquantitytheremarkapplies.
Theygive:i)Continuationforthelistofdecays.
Inthiscase,theremarkstartswiththreedots.
ii)Informationexplaininghowavaluehasbeenderived.
iii)Reasonsforchangingavalueoritsuncertaintyasgivenbytheauthors,orforrejectingit.
iv)Complementaryreferencestoupdateddata.
v)Separatevaluesusedintheadoptedaverage.
TNN:Trendsfromneighboringnuclides.
No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1179TableI.
TheNUBASE2012table(ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)1n8071.
31710.
0005613.
9s0.
61/2+061932β=1001H7288.
97050.
0001STABLE1/2+0611Be53D1920IS=99.
9885701nT:also12Ar05=611.
1(1.
5)meanlife=881.
6(2.
1)2H13135.
72170.
0001STABLE1+031932IS=0.
0115703H14949.
80610.
002212.
32y0.
021/2+001934β=1003He14931.
21550.
0023STABLE1/2+981934IS=0.
00013433Li28670#2000#p-unstable981969p3LiI:identicationin69Wi13notaccepted,seeENSDF'984H24620100139ys1029803Me11T1981n=1004He2424.
91560.
0001STABLE0+981908IS=99.
99986634Li2532021091ys929865Ce02T1965p=1004HT:width=3.
28(0.
23)MeV;also91Go19=4.
7(1.
0)outweighed,notused5H3289090>910ys(1/2+)0203Go11T19872n=1005He1123120700ys303/2021937n=1005Li1168050370ys303/2021941p=1005Be37140#2000#1/2+#02p5HT:fromwidth6.
3zs0+0012Ja11T19782p=603012BeD:from99Be53;also95Re.
A=0.
52(0.
09)%outweighed,notused12BiJ:08Ch28"suggeststhatthe12.
75-MeV,.
.
.
.
wasaT=1state,nottheIAS"12OT:fromwidth12Ja111as5/2+#9610Mu12TD1969p=10019Mg31830505ps31/2#9609Mu17TD20072p=10019BD:symmetrizedfrom71.
8(+8.
3–9.
1)%16.
0(+5.
6–4.
8)%19CT:average88Du09=49(4)95Re.
A=44(4)95Oz02=45.
5(4.
0)19CJ:from01Ma08,99Na27and95Ba2819NeT:also94Ko.
A=17.
296(0.
005)conicting,notused19NeT:92Ge08=18.
5(0.
6)forq=10+(bareion)19NeiJ:ifthisistheIASof19Oground-state5/2+;notyetconrmed19NaT:fromupperlimitof40keV,dominatedbyresolution:260ns)5/2+#0699Sa06I1999β;βn;β2n31Ne3082016203.
4ms0.
87/2#061996β=100;βn;β2n31Na122612317.
0ms0.
43/2(+#)0693Kl02J1969β=100;βn=375;.
.
.
31Mg31223232ms151/2+0708Ko05J1977β=100;βn=6.
22031Al1495520644ms255/2+0106Hi18J1971β=100;βn1.
5s)0+1202Le.
AI2002β;βn;β2n34Na31290#500#5.
5ms1.
01+12GAu03D1983β=100;β2n≈50;βn≈1534Mg83232920ms100+121979β=100;βn;β2n34Al30707056.
3ms0.
5(4)121977β=100;βn=12.
525;β2n34Alm2520#120#550#100#26ms1(1+)12Ro25TJ2012β≈100;βn;β2n34Si19957142.
77s0.
200+121971β=10034Sim15701144256.
10.
41.
5s)3/2+#1202Le.
AI2002β;βn;β2n37Mg28290#500#8ms47/2#121996β;βn;β2n37Al981012010.
7ms1.
33/2+#121979β=100;βn;β2n37Si65908090ms607/2#121979β=100;βn=1713;β2n37P19000402.
31s0.
131/2+#121971β=100;βn=0.
02#37S26896.
410.
205.
05m0.
027/2121945β=10037Cl31761.
520.
05STABLE3/2+121919IS=24.
241037Cli21539.
70.
310221.
80.
3RQ7/2T=5/2121984IT=10037Ar30947.
650.
2135.
011d0.
0193/2+121941ε=10037Ari25956649926RQ3/2+T=3/212197337K24800.
200.
091.
225s0.
0073/2+121958β+=10037Ki19749.
90.
85050.
30.
8RQ3/2+T=3/2121973IT=10037Ca13136.
10.
6181.
1ms1.
03/2+#121964β+=100;β+p=82.
1737Sc3480#300#7/2#p37CaTD:also07Do17=181.
7(3.
6)ms;72.
2(4.
3)%;alsoβ+p=74.
5(0.
7)%from95Tr0338Mg34070#500#1#ms(>260ns)0+082002β=100#;βn=76#;β2n=7.
4#38Al162102507.
6ms0.
6081989β=100;βn;β2n38Si41707090#ms(>1s)0+081979β=100#;βn38P1467090640ms140(0to4)081971β=100;βn=12538S268617170.
3m0.
70+081958β=10038Cl29798.
090.
1037.
24m0.
052081940β=10038Clm29126.
730.
10671.
3650.
008715ms35081954IT=10038Cli2159024820824RQ0+T=30838Ar34714.
820.
19STABLE0+081934IS=0.
0629738Ari24083.
90.
910630.
90.
9(2)T=20838Arj15940301878030RQ0+T=30838K28800.
750.
207.
636m0.
0183+T=0081937β+=10038Km28670.
610.
20130.
150.
04MD924.
46ms0.
140+T=10810Ba43T1953β+=10038Kn25342.
610.
263458.
140.
1721.
95s0.
11(7)+081971IT=10038Ca22058.
500.
19443.
77ms0.
360+0811Pa38T1966β+=10038Sc4550#200#170ns)0+072007β;βn;β2n40Al27970#500#10#ms(>260ns)042002β;βn;β2n40Si543023033.
0ms1.
00+0604Gr20TD1989β=100;βn;β2n40P8070110150ms8(2,3)041979β=100;;βn=15.
821;β2n40S2283848.
8s2.
20+041971β=10040Cl27560301.
35m0.
022041956β=10040Ar35039.
89460.
0022STABLE0+041920IS=99.
60352540K33535.
490.
061.
248Gy0.
0034041935IS=0.
01171;.
.
.
40Km31891.
850.
061643.
6390.
011336ns120+041968IT=10040Ki29151.
50.
34384.
00.
30+T=204IT=10040Ca34846.
3860.
021STABLE(>5.
9Zy)0+0499Be64T1922IS=96.
9416;2β+40Cai27188.
210.
057658.
180.
054T=104AHWEIT=10040Caj22858.
41.
01198810+T=204IT=10040Sc20523.
32.
8182.
3ms0.
74041955β+=100;.
.
.
40Sci16164643596RQ0+T=204IT=10040Ti885016052.
4ms0.
30+0407Do17TD1982β+=100;β+p=95.
81340V11890#400#2#p40KD:.
.
.
;β=89.
2813;β+=10.
721340CaiE:Original7658.
23(0.
05)recalibrated-0.
05keVfor27Al+presonances40ScD:.
.
.
;β+p=0.
447;β+α=0.
017541Al33890#600#2#ms(>260ns)3/2+#022002β;βn;β2n41Si1212037020.
0ms2.
57/2#0204Gr20TD1989β=100;βn;β2n41P498080100ms51/2+#071979β=100;βn=3010;β2n41S1900941.
99s0.
057/2#021979β=100;βn41Cl273107038.
4s0.
8(1/2+)071971β=10041Ar33067.
50.
3109.
61m0.
047/2021936β=10041K35559.
5430.
004STABLE3/2+021921IS=6.
73024441Ki2721015834915RQ7/2T=5/20275Me10J197541Ca35137.
890.
1499.
4ky1.
57/20212Jo04T1939ε=10041Cai29320.
70.
95817.
20.
9170ns)072007β;βn;β2n42Si16560#500#12.
5ms3.
50+061990β=100;βn;β2n42P101021048.
5ms1.
50104Gr20T1979β=100;βn=5020;β2n42S17637.
72.
81.
013s0.
0150+011979β=100;βn170ns)3/2+#072007β;βn;β2n43Si23100#600#15#ms(>260ns)3/2#0602No11I2002β;βn;β2n43P468037035.
8ms1.
31/2+#0604Gr20T1989β=100;βn=100;β2n43S121955265ms133/2#0104Gr20T1979β=100;βn=401043Sm118755320.
00.
5415ns5(7/2)0109Ga05TJE2000IT=10043Cl243201003.
13s0.
09(3/2+)0706Wi10J1976β=100;βn43Ar3201055.
37m0.
06(5/2)011969β=10043K36575.
40.
422.
3h0.
13/2+011949β=10043Km35837.
30.
4738.
10.
1200ns57/2011978IT=10043Ca38408.
820.
23STABLE7/2011934IS=0.
1351043Cai3041414799514RQ(3/2)+T=5/20143Sc36188.
11.
93.
891h0.
0127/2011935β+=10043Scm36036.
71.
9151.
40.
2438s53/2+0177Mi10T1964IT=10043Scn33064.
91.
93123.
20.
3472ns319/20108Fe02T1978IT=10043Sci31956342324RQ7/2T=3/201.
.
.
A-groupiscontinuedonnextpage.
.
.
1188ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%).
.
.
A-groupcontinued.
.
.
43Ti293217509ms57/2011948β+=10043Tim290087313.
01.
011.
9s0.
3(3/2+)0111Ho02T1978IT=10043Tin2625573066.
41.
0556ns5(19/2)0111Ho02T1978IT=10043Tii246059471667/2T=3/243V179204079.
3ms2.
47/2#0107Do17TD1987β+=100;β+p360ns)0+112007β;βn;β2n44P10440#500#18.
5ms2.
5111989β=100;βn=18#;β2n=7144S92045100ms10+111979β=100;βn=18344Sm783951365.
00.
82.
619s0.
0260+112005IT=10044Cl20610190560ms110(2)111979β=100;βn200ns)1/2+#081990β;βn;β2n45S399069068ms23/2#081989β=100;βn=54;β2n45Cl18360100413ms253/2+#081979β=100;βn=24445Ar29770.
80.
521.
48s0.
15(5/2,7/2)081974β=10045K36615.
60.
517.
8m0.
63/2+081964β=10045Ca40812.
20.
4162.
61d0.
097/2081940β=10045Sc41071.
20.
7STABLE7/2081923IS=100.
45Scm41058.
80.
712.
400.
05318ms73/2+081964IT=10045Sci34372156699157/2T=5/20845Ti39009.
10.
9184.
8m0.
57/2081941β+=10045Tim38972.
60.
936.
530.
153.
0s0.
23/2082006IT=10045Tii34290347193RQ7/2T=3/20845V318818547ms67/2081975β+=10045Vm31824856.
80.
6512ns13(3/2)0811Ho02T1980IT=10045Vi270909479112RQ7/2T=3/208p=10045Cr195104060.
9ms0.
47/2#081974β+=100;β+p=34.
4845Crm19400401071>80s(3/2)1111Ho02ETJ2011IT=10045Mn5130#400#200ns)0090Le03I1990β;βn;β2n46S40#500#50ms80+101989β=100;βn;β2n46Cl13810160232ms20004Gr20T1989β=100;βn=609;β2n46Ar29730408.
4s0.
60+001974β=10046K35413.
90.
7105s102()0082To02J1965β=10046Ca43138.
42.
3STABLE(>100Ey)0+0099Be64T1938IS=0.
0043;2β46Sc41760.
50.
783.
79d0.
044+001936β=10046Scm41708.
50.
752.
0110.
0019.
4s0.
86+001966IT=10046Scn41618.
00.
7142.
5280.
00718.
75s0.
041001948IT=10046Sci36747450144RQ0+T=30046Ti44127.
00.
3STABLE0+001934IS=8.
25346Tii34961791667RQ4+T=20046Tij299766141516RQ0+T=30046V37074.
60.
3422.
64ms0.
050+T=10012Pa07T1952β+=10046Vm36273.
10.
3801.
460.
101.
02ms0.
073+T=0001962IT=10046Cr2947420257ms550+1005On03T1972β+=10046Cri2032315915125RQ(4+)T=210p=46Mn12960#400#36.
2ms0.
4(4+)101987β+=100;β+p=57.
08;.
.
.
46Mnm12810#410#150#100#1#ms1#β+46Mni7470505480#400#pT=346Fe590#500#13.
0ms2.
00+1007Do17TD1992β+=100;β+p=78.
73846CaT:limitisfor0ν-ββdecay46VT:average12Pa07=422.
66(0.
06)97Ko65=422.
57(0.
13)46CrT:average05On03=240(140)72Zi02=260(60)46MnD:.
.
.
;β+2p≈18;β+α46MnT:others92Bo37=41(+7–6)01Gi01=34.
0(+4.
5–3.
5)46MnD:β+2p≈18%estimatedfromPp=β+p+2*β+2p=57(1)%46FeT:other01Gi01=9.
7(+3.
5–4.
3)D:other01Gi01=36(20)%47P29240#800#2#ms3/2+#β;βn;β2n47S7410#500#20#ms(>200ns)3/2#0789Gu03I1989β;βn;β2n47Cl10100#400#101ms53/2+#071989β=100;βn200ns)0+061990β;βn;β2n48Cl4060#500#100#ms(>200ns)0689Gu03I1989β;βn;β2n48Ar22440#300#475ms400+102004β=;βn48K32284.
50.
86.
8s0.
2(1)0611Bi.
AJ1972β=100;βn=1.
141548Ca44224.
760.
1253Ey170+0600Br63T1938IS=0.
18721;.
.
.
48Sc44503543.
67h0.
096+061937β=10048Ti48491.
70.
4STABLE0+061923IS=73.
72348Tii377666107266(6+)T=30648V44476.
81.
015.
9735d0.
00254+061937β+=10048Vi41457.
90.
43018.
90.
9RQ(0)+T=206IT=10048Cr42822721.
56h0.
030+061952β+=10048Cri3702975792.
770.
244+T=1061987IT=10048Crj3406215876017RQ0+frg.
T=20648Mn29320170158.
1ms2.
24+061987β+=100;β+p=0.
284;.
.
.
48Mni26259143060170p0+T=206MMC12Jp=10048Fe18420#400#45.
3ms0.
60+0607Do17TD1987β+=100;β+p=15.
9648Co870#800#6+#06p48Ni16480#510#2.
8ms0.
80+0611Po09TD20002p=7020;β+=3020;β+p48CaD:.
.
.
;2β=75+25-38;β48CaT:average00Br63=42(33-13)96Ba80=43(+24–11statistics+14systematics)48CaT:alsoT>36Eyfrom70Ba61.
Singleβdecay:T>6Ey(95%CL),from85Al1748CrjE:strongestfrg;other:10(15)keVlower48MnD:.
.
.
;β+α=6e–448NiT:average05Do20=2.
1(+2.
1–0.
7)11Po09=2.
1(+1.
4–0.
4)1190ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)49S21200#670#200ns)3/2+#0889Gu03I1989β;βn;β2n49Ar16860#400#170ms503/2#081989β=100;βn=6520;β2n49K29611.
50.
81.
26s0.
051/2()1111Bi.
AJ1972β=100;βn=86949Ca41299.
890.
218.
718m0.
0063/2081950β=10049Sc46561.
12.
757.
18m0.
137/2081940β=10049Ti48562.
80.
4STABLE7/2081934IS=5.
41249V47961.
00.
9330d157/2081940ε=10049Vi41529464324RQ7/2T=5/249Cr45332.
72.
442.
3m0.
15/2081942β+=10049Cri40569647645(7/2)T=3/20885Fu03E1969IT=10049Mn3763710382ms75/2081970β+=10049Mni3280418483320p(7/2)T=3/208p=10049Fe247512464.
7ms0.
3(7/2)0896Fa09J1970β+=100;β+p=56.
7449Co10330#700#620ns)1009Ta24I2009β;βn;β2n50Ar12920#500#85ms300+101989β=100;βn=3510;β2n50K257288472ms40()1011Bi.
AJ1972β=100;βn=293;β2n50Km255578171.
40.
4125ns40(2)10FGK127J1999IT=10050Ca39589.
21.
613.
9s0.
60+101964β=10050Sc4454815102.
5s0.
55+101959β=10050Scm4429115256.
8950.
010350ms40(2+,3+)101963IT>97.
5;β1.
3Ey)0+101930IS=4.
34513;2β+50Cri41835784277RQ6+T=21050Crj370386132246RQ0+T=31050Mn42627.
20.
9283.
19ms0.
100+T=1101952β+=10050Mnm42401.
90.
9225.
310.
07MD1.
75m0.
035+T=0101962β+=10050Fe3449060155ms110+101977β+=100;β+p≈050Fei2601614847060RQ(6+)T=21050Co17780#600#38.
8ms0.
2(6+)1096Fa09J1987β+=100;β+p=70.
57;β+2p50Coi127701705010#620#2p(0)+T=31007Do17Dp=10050Ni4900#800#18.
5ms1.
20+1007Do17TD1994β+=100;β+p=86.
739;β+2p50KmJ:E2toground-state50KmT:othersrecent12Ka.
B=138(+50–41)09Cr031.
3Ey85No03>0.
18Ey50FeT:from97Ko46=155(11)50NiT:other03Ma34=12(+3–2)D:other03Ma34=70(20)%51Cl14480#700#2#ms(>200ns)3/2+#061990β;βn;β2n51Ar5870#600#60#ms(>200ns)3/2#0689Gu03I1989β;βn;β2n51K2251613365ms5(3/2+)0606Pe16JD1983β=100;βn=656;β2n51Ca363392210.
0s0.
8(3/2)0606Pe16J1980β=100;βn51Sc432292012.
4s0.
1(7/2)061966β=100;βn51Ti49731.
90.
65.
76m0.
013/2061947β=10051V52203.
70.
9STABLE7/2061924IS=99.
750451Cr51451.
10.
927.
7010d0.
00117/2061940ε=10051Cri44838566135RQ7/2T=5/20651Mn48243.
50.
946.
2m0.
15/2061938β+=10051Mni43792.
11.
74451.
41.
5RQ7/2T=3/206IT=10051Fe402029305ms55/2061972β+=10051Co273405068.
8ms1.
97/2#0607Do17TD1987β+=100;β+p620ns)5/2#1109Ta24I2009β;βn;β2n53K11680#500#30ms5(3/2+)0906Pe16JD1983β=100;βn=6411;β2n≈10553Ca28460#400#461ms903/2#0910Cr02T1983β=100;βn>3053Sc381102702.
4s0.
6(7/2)0910Cr02TJ1980β=100;βn53Ti4683010032.
7s0.
9(3/2)091977β=10053V5185031.
543m0.
0147/2091960β=10053Cr55285.
90.
6STABLE3/2091930IS=9.
5011753Mn54689.
00.
63.
7My0.
47/20971Ho24T1955ε=10053Mni47715469744RQ3/2T=5/209197653Fe50946.
71.
78.
51m0.
027/2091938β+=10053Fem47906.
31.
73040.
40.
32.
54m0.
0219/2091967IT=10053Fei466973425037/2T=3/20953Co42658.
61.
8242ms87/2#0902Lo13T1970β+=10053Com39484.
41.
93174.
30.
9MD247ms12(19/2)091970β+≈98.
5;p≈1.
553Coi3826418439518p(7/2)T=3/2091976p=10053Ni296312555.
2ms0.
77/2#0907Do17TD1976β+=100;β+p=23.
41053Cu14350#800#620ns)3/2+#0909Ta24I2009β;βn;β2n55Ca18350#500#22ms25/2#091997β=100;βn;β2n55Sc2998046096ms2(7/2)0810Cr02TJD1990β=100;βn=177;β2n55Ti416701601.
3s0.
1(1/2)101980β=100;βn55V491401006.
54s0.
157/2#081977β=10055Cr55108.
60.
63.
497m0.
0033/2081952β=10055Mn57711.
70.
4STABLE5/2081923IS=100.
55Fe57480.
60.
52.
744y0.
0093/2091939ε=10055Fei49847676336RQ5/2T=5/20955Co54029.
30.
517.
53h0.
037/2091938β+=10055Coi49307.
90.
54721.
440.
103/2frg.
T=3/2091981IT=10055Ni45335.
20.
8204.
7ms1.
77/20802Lo13T1972β+=10055Cu3164016027ms83/2#0807Do17TD1987β+=100;β+p=15.
04355Zn14920#700#19.
8ms1.
35/2#0807Do17TD2001β+=100;β+p=91.
05155ScT:others04Li75=115(15)02Sh43=103(7)98So03=120(40)55CoiE:strongestfrg(spectr.
factor0.
45);other26.
69(0.
15)higher(sf=0.
37)55NiT:average02Lo13=196(5)99Re06=204(3)87Ha.
A=212.
1(3.
8)84Ay01=208(5)55NiT:and77Ho25=189(5)76Ed.
A=219(6);97Wo06=204(3)supersededby99Re0656K7930#800#1#ms(>620ns)2#1109Ta24I2009β;βn;β2n56Ca13900#600#11ms20+111997β=100;βn;β2n56Sc24730#400#26ms6(1+)1110Sc02J1997β=100;βn=;β2n56Scm24730#410#0#100#75ms6(6+,5+)1110Sc02J2004β=100;βn>142;β2n56Scn23960#400#774.
90.
3290ns30(4+)112004IT=10056Ti39210140200ms50+1198Am04D1980β=100;βn56V46120180216ms4(1+)1198Am04D1980β=100;βn56Cr55281.
21.
95.
94m0.
100+1160Dr03D1960β=10056Mn56910.
80.
52.
5789h0.
00013+111934β=10056Fe60606.
40.
5STABLE0+111923IS=91.
7543656Fei49102.
70.
611503.
70.
33+T=31156Co56039.
80.
677.
236d0.
0264+111941β+=10056Coi52447935939RQ(0+)frg.
T=21156Ni53906.
90.
56.
075d0.
0100+111952β+=10056Nii47475.
00.
96431.
90.
74+T=11156Nij43963499444RQ0+frg.
T=256Cu38240#200#93ms3(4+)1101Bo54TJD1987β+=100;β+p=0.
401256Cui35120303120#200#pT=207Do17D2007p=10056Zn25580#500#30.
0ms1.
70+1107Do17TD2001β+=100;β+p=86.
04956Zni21720#710#3860#510#3+#T=3p56Ga4320#600#3+#p56ScnT:other12Ka.
B=350(+260–120)56CoiE:strongestfrg(crosssection115);other70(9)keVlower(xs=55)56NijE:strongestfrg;others68(6)and98(6)keVhigher56ZnT:other95Wa.
A=36(10)msderivedfromexperimental(p,n)crosssections57Ca6870#600#5#ms(>620ns)5/2#1009Ta24I2009β;βn=22#;β2n=2#57Sc20710#500#22ms27/2#1010Sc02T1997β=100;βn=33#;β2n=1#57Ti3387025095ms85/2#1099So20T1985β=100;βn=0.
3#57V44230230350ms10(3/2)1003Ma02TJ1980β=100;βn=0.
4#57Cr52524.
11.
921.
1s1.
0(3/2)101978β=10057Mn57486.
11.
585.
4s1.
85/2981954β=10057Fe60181.
20.
5STABLE1/2981935IS=2.
1191057Co59344.
90.
6271.
74d0.
067/2981941ε=10057Coi52091.
60.
67253.
40.
6RQ1/2T=5/2MMC12J57Ni56083.
20.
735.
60h0.
063/2981938β+=10057Nii50844.
41.
05238.
80.
77/2frg.
T=3/29857Cu47308.
30.
6196.
3ms0.
73/2981976β+=10057Cui4200925529925p7/2T=3/257Zn32550#210#38ms47/2#9802Lo13T1976β+=100;β+p≈6557Ga15650#300#1/2#p57ScT:other03So21=13(4)57TiT:average05Li53=98(5)99So20=67(25)96Do23=56(20)57TiT:98Am04=180(30)conicting,notused57NiiE:strongestfrg;79Ik04others98(7)keVlower(5.
5%)128(7)keVhigher(10.
0%)57NiiE:strongestfrg;78Na11others104(5)keVlower,129(5)keVhigher57ZnT:average02Lo13=37(5)76Vi02=40(10)58Ca1920#700#3#ms(>620ns)0+102009β;βn;β2n58Sc14880#600#12ms53+#101997β=100;βn;β2n58Ti31110#400#55ms60+1011Da08T1992β=100;βn58V40320130191ms10(1+)101980β=100;βn=0.
8#58Cr518302007.
0s0.
30+101980β=100.
.
.
A-groupiscontinuedonnextpage.
.
.
No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1193TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%).
.
.
A-groupcontinued.
.
.
58Mn55827.
62.
73.
0s0.
11+101961β=10058Mnm55755.
82.
771.
770.
0565.
4s0.
54+101961β=;IT=20#58Fe62154.
50.
5STABLE0+101935IS=0.
282458Co59846.
61.
270.
86d0.
062+101941β+=10058Com59821.
71.
224.
950.
069.
10h0.
095+101950IT=10058Con59793.
51.
253.
150.
0710.
5s0.
34+101964IT=10058Coi54094857538RQ0+frg.
T=31058Ni60228.
20.
5STABLE(>700Ey)0+101921IS=68.
07719;2β+58Nii5140040883040RQ2+T=21058Nij456897145397RQ0+T=310MMC12J58Cu51667.
10.
73.
204s0.
0071+T=0101952β+=10058Cui51464.
10.
7202.
990.
240+T=11058Zn423005086ms80+101986β+=100;β+p400Eyto2+levelof58Fe,>700Eytoground-state59Sc10300#600#10#ms(>620ns)7/2#0909Ta24I2009β;βn;β2n59Ti25640#400#28.
5ms1.
95/2#0211Da08T1997β=100;βn;β2n59Tim25530#400#109.
00.
5590ns50(1/2)12Ka.
BETJ2012IT=10059V3783016095ms6(5/2)0205Li53TJ1985β=100;βn59Cr478902401050ms90(1/2)0205Li53TJ1980β=10059Crm47390240503.
01.
796s20(9/2+)021998IT=10059Mn55525.
32.
34.
59s0.
05(5/2)021976β=10059Fe60664.
20.
544.
495d0.
0093/2021938β=10059Co62229.
10.
5STABLE7/2021923IS=100.
59Ni61156.
10.
5101ky133/20294Ru19T1951β+=10059Nii53814.
22.
27341.
92.
1RQ7/2frg.
T=5/259Cu56357.
70.
681.
5s0.
53/2021947β+=10059Cui52472.
22.
23885.
52.
13/2frg.
T=3/202IT=10059Zn47215.
00.
8182.
0ms1.
83/2031981β+=100;β+p=0.
10359Ga33970#170#620ns)3+#0909Ta24I2009β;βn;β2n60Ti22330#500#22.
2ms1.
60+0311Da08T1997β=100;βn;β2n60V33240220&122ms183+#031985β=100;βn;β2n60Vm33240#270#0#150#&40ms151+#031999β=;IT;βn;β2n60Vn33040220203.
70.
7230ns24(4+)0312Ka.
BET1999IT=10060Cr46500210490ms100+031980β=100;βn60Mn52967.
92.
3280ms201+031978β=10060Mnm52696.
02.
3271.
900.
101.
77s0.
024+031978β=88.
58;IT=11.
5860Fe6141232.
62My0.
040+9309Ru08T1957β=10060Co61649.
70.
55.
2712y0.
00045+031941β=10060Com61591.
10.
558.
590.
0110.
467m0.
0062+031963IT≈100;β=0.
24360Ni64472.
50.
5STABLE0+031921IS=26.
2231560Nii533464111264RQ5+T=360Cu58344.
61.
623.
7m0.
42+031947β+=10060Cui55803525415RQ(0+)T=203IT=10060Zn54173.
70.
62.
38m0.
050+031955β+=10060Zni49321.
50.
94852.
20.
7(2+)T=103IT=10060Znj4680624736724RQ0+T=20360Ga39780#200#70ms10(2+)0301Ma96TJ1995β+=100;β+p=1.
67;β+α110ns)0+092005β+;β+p60As5700#400#5+#p60Asm5640#400#60#20#2+#p60TiT:average11Da08=22.
4(2.
5)03So21=22(2)60VnT:symmetrizedfrom12Ka.
B=229(+25–23);others10Da06=320(90)99Da.
A=320(90)60MnmI:alsoanisomerT=1.
0(+0.
3–0.
2)sdecayby114keVγ-raystoground-stateor60Mnm60GaT:average02Lo13=70(13)01Ma96=70(15)1194ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)61Sc930#800#2#ms(>620ns)7/2#0909Ta24I2009β;βn;β2n61Ti16350#600#15ms41/2#0911Da08T1997β=100;βn=0.
8#;β2n=0.
7#61V3051089047.
0ms1.
23/2#091992β=100;βn>6;β2n61Cr42460130243ms9(5/2)0909Cr02T1985β=100;βn61Mn51742.
12.
3670ms40(5/2)0999Ha05D1980β=100;βn=61Fe58920.
52.
65.
98m0.
063/29908Ho05J1957β=10061Fem58058.
72.
6861.
800.
15241.
2ns4.
59/2+9908Ho05EJ1998IT=10061Co62897.
60.
91.
650h0.
0057/2991947β=10061Ni64221.
30.
5STABLE3/2991934IS=1.
13991361Cu61983.
81.
03.
333h0.
0053/2991937β+=10061Cui55610763747RQ3/2frg.
T=5/261Zn563491689.
1s0.
23/2991955β+=10061Znm562611688.
40.
15861As17590#300#3/2#p61CrT:average09Cr02=233(11)99So20=251(22)98Am04=270(20)61MnD:delayedneutronsobservedin99Ha0561FemT:average04Ma80=239(5)98Gr14=250(10)61FemE:derivedfromleast-squaresttoγ-rayenergiesEgusing08Ho05levelscheme61CuiE:strongestfrg(xs=55);other18(7)keVhigher(xs=35)62Ti12570#700#10#ms(>620ns)0+122009β;βn;β2n62V25480#300#33.
6ms2.
33+#121997β=100;βn;β2n62Cr40890150206ms120+121985β=100;βn=1#62Mn48480#150#92ms13(1+)1299So20JD1983β=100;βn≈062Mnm48181.
02.
6300#150#671ms5(3+)1299Ha05D1983β=100;βn=;IT62Fe58878.
02.
868s20+121975β=10062Co61424191.
54m0.
10(2)+121949β=10062Com614022022513.
86m0.
09(5)+121957β>99;IT620ns)1/2#0909Ta24I2009β;βn;β2n63V21990#400#18.
3ms1.
97/2#0911Da08T1997β=100;βn>35;β2n63Cr35720460129ms21/2#091992β=100;βn63Mn468874275ms45/2#091985β=100;βn=63Fe5563646.
1s0.
6(5/2)091980β=10063Co618511926.
9s0.
47/20994It.
AT1960β=10063Ni65512.
30.
5101.
2y1.
51/2091951β=10063Nim65425.
20.
587.
150.
111.
67s0.
035/2091978IT=10063Cu65579.
30.
5STABLE3/2091923IS=69.
151563Zn62213.
11.
638.
47m0.
053/2091937β+=10063Zni56723654906RQ3/2T=5/20963Ga56547.
11.
332.
4s0.
5(3/2)091965β+=10063Ge4692040142ms83/2#0902Lo13TD1991β+=100;β+p63As33630#200#8.
9Ey)0+071922IS=49.
1775;2β+64Ga58832.
81.
42.
627m0.
0120(+#)071953β+=10064Gam58790.
01.
442.
850.
0821.
9s0.
7(2+)071999IT=10064Gai56925.
72.
51907.
12.
2RQ(0+)T=20764Ge54315463.
7s2.
50+071972β+=10064As39650#300#40ms300+#071995β+=100;β+p64Se26930#500#30#ms(>180ns)0+072005β+;β+p64CrT:otherrecent11Li50=44(3)ms,outweighed,notused64MnT:average11Da08=90(9)02So.
A=91(4)99So20=85(5)99Ha05=89(4)64MnmT:average11Li50=400(40)05Ga.
B=500(50)64CuiE:strongestfragment(xs=100);other16keVlower(xs=37)64AsT:symmetrizedfrom18(+43–7)65V11640#500#10#ms(>620ns)5/2#1009Ta24I2009β;βn;β2n65Cr27980#300#27.
5ms2.
11/2#1011Da08T1997β=100;βn;β2n65Mn40967492ms15/2#101985β=100;βn=65Fe512217810ms50(1/2)1009Pa16J1980β=100;βn65Fem508247396.
80.
5420ns135/2#1010Da06ET1998IT=10065Fen50819840210MD1.
12s0.
15(9/2+)102008β65Co59185.
22.
11.
16s0.
03(7/2)101978β=10065Ni65125.
20.
62.
5175h0.
00055/2101946β=10065Nim65061.
80.
663.
370.
0569s31/2101978IT=10065Cu67263.
50.
7STABLE3/2101923IS=30.
851565Zn65911.
80.
7243.
93d0.
095/2101939β+=10065Znm65857.
90.
753.
9280.
0101.
6s0.
6(1/2)10IT=10065Ga62657.
30.
815.
2m0.
23/2101938β+=10065Ge56478.
22.
230.
9s0.
53/2101972β+=100;β+p=0.
011365As4694080170ms303/2#1002Lo13T1991β+=100;β+p65Asi4345117349090p(3/2)T=3/21011Ro47J1993p=10065Se33160#600#33ms43/2#1011Ro47T1993β+=100;β+p=65CrT:average11Da08=28(3)03So21=27(3)65MnT:otherrecent11Da08=84(8),outweighed,notused65FemE:uncertaintynotgiven,estimatedbyevaluator65FemJ:98Gr14=(5/2)assumingM2,E2directtoground-state;10De06showsitisacascade65AsT:average02Lo13=126(16)95Mo26=190(11)withBirgeratioB=3.
365AsiJ:IASstudiedin93Ba12and11Ro4766V5610#600#5#ms(>620ns)1009Ta24I2009β;βn;β2n66Cr24540#500#23.
8ms1.
80+1011Li50T1997β=100;βn;β2n66Mn367501164.
2ms0.
8(1+)1011Pa.
ATD1992β=100;βn=8.
49;β2n66Mnm3628611464.
50.
4780s40(5)11Li50ETJ2005IT≈100;β66Fe500684351ms60+1012Li02T1985β=100;βn66Co5640914194ms17(1+)1012Li02J1985β=100;βn66Com5623414175.
10.
31.
21s0.
01(3+)1012Li02EJ1998IT=10066Con55767156425>100s(8)1098Gr14ETJ1998IT=10066Ni66006.
31.
454.
6h0.
30+101948β=10066Cu66258.
10.
75.
120m0.
0141+101937β=10066Cum65103.
91.
61154.
21.
4600ns17(6)1011Lo01T1972IT=10066Zn68899.
10.
9STABLE0+101922IS=27.
739866Ga6372439.
304h0.
0080+1010Se16T1937β+=10066Gai59874638507RQ0+T=366Ge61607.
02.
42.
26h0.
050+101950β+=10066As52025695.
77ms0.
23(0+)1098Gr12J1978β+=10066Asm5066861356.
630.
171.
1s0.
1(5+)101995IT=10066Asn4900163023.
80.
38.
2s0.
5(9+)101998IT=10066Asi51230200800200(1+)T=198Gr.
AJ66Se41370#300#33ms120+1002Lo13TD1993β+=100;β+p66CrT:average11Li50=24(2)11Da08=23(4);other05Ga01=10(6)outweighed66MnJ:11Li50=(1+)duetolargeground-statefeedingfrom66Cr66MnmE:other05Ga.
B=294+170keVT:other05Ga.
B=750(250)66CumT:average11Lo01=601(30)72Bl16=600(20)66GaT:other12Gy01=9.
312(0.
032)notused;ENSDF=9.
49(0.
03)1196ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)67Cr18480#500#10#ms(>300ns)1/2#0597Be70I1997β;βn;β2n67Mn33310#400#46.
7ms2.
35/2#0511Da08TD1997β=100;βn=105;β2n67Fe46070220394ms9(1/2)0502So.
ATD1985β=100;βn67Fem45670220402964s17(5/2+,7/2+)0511Da08EJ1998IT=10067Fen45620#240#450#100#75s21(9/2+)08Bl05TJ2008IT67Co553226329ms28(7/2)0508Pa33TJ1985β=100;βn67Com548306491.
61.
0496ms33(1/2)09Pa16E2008IT>80;β67Ni63742.
72.
921s11/20500Ri14J1978β=10067Nim6273631007.
21.
013.
3s0.
2(9/2+)051998IT=10067Cu67318.
81.
261.
83h0.
123/2051948β=10067Zn67880.
10.
9STABLE5/2051928IS=4.
041667Znm67786.
80.
993.
3120.
0059.
07s0.
041/2051972IT=10067Znn67275.
60.
9604.
480.
05333ns149/2+051973IT=10067Ga66878.
91.
23.
2617d0.
00053/2051938ε=10067Ge62658518.
9m0.
31/2051950β+=10067Gem62640518.
200.
0513.
7s0.
95/2051978IT=10067Gen619065751.
700.
06109.
1ns3.
89/2+0500Ch07T1973IT=10067As56587.
20.
442.
5s1.
2(5/2)051980β+=10067Se4658070133ms115/2#0595Bl23T1991β+=100;β+p=0.
5167Br32930#500#1/2#p67MnT:average11Da08=51(4)03So21=47(4)99Ha05=42(4)67FeT:othersrecent11Da08=304(81)08Pa33=416(29),outweighed,notused67FemT:average03Sa02=75(21)98Gr14=43(30),sameauthors,differentexperiment67FemE:lessthan30keVabove387.
7level67ComE:09Pa16=491.
55(0.
11)γray;08Pa33=491.
6(1.
0)D:from08Pa3367GenT:average00Ch07=101(3)79Al04=110.
9(1.
4);BirgeratioB=2.
9967SeT:average02Lo13=136(12)94Ba50=107(35)67SeT:valuesfrom95Bl23for67Se=60(+17–11)and71Krquestionedin97Oi0168Cr14880#700#5#ms(>620ns)0+1209Ta24I2009β;βn=15#;β2n68Mn28300#500#28.
4ms2.
71211Da08T1995β=100;βn=;β2n68Fe43830370188ms40+121985β=100;βn>068Co51920150200ms20(7)121985β=100;βn68Com51770#210#150#150#1.
6s0.
3(1+)121998β=10068Con51730#210#195#150#101ns10(0,1)1210Da06T2010IT=10068Ni63463.
83.
029s20+121977β=10068Nim6169431770.
01.
0270ns50+121984IT=10068Nin612623nonexistentRN230ns600+12Di03TJDIT=10068Nip6061532849.
10.
3860s505121995IT=10068Cu65567.
01.
630.
9s0.
61+121953β=10068Cum64845.
71.
6721.
260.
083.
75m0.
056121969IT=862;β=14268Zn70006.
80.
9STABLE0+121922IS=18.
456368Ga67085.
71.
567.
71m0.
081+121937β+=10068Ge66978.
81.
9270.
93d0.
130+121948ε=10068As58894.
51.
8151.
6s0.
83+121971β+=10068Asm58469.
41.
8425.
10.
2111ns201+121994IT=10068Se54189.
40.
535.
5s0.
70+121990β+=10068Br38440#310#620ns)0909Ta24I2009β;βn;β2n70Fe36310#500#77ms90+0411Da08T1997β=100;βn70Co46920300112.
7ms4.
5(6)0411Da08T1985β=100;βn;β2n70Com46720#360#200#200#500ms1803+#041998β≈100;IT;βn70Ni59213.
92.
16.
0s0.
30+041987β=10070Nim56353.
92.
928602232ns1(8+)041997IT=10070Cu62976.
41.
144.
5s0.
260410Vi07J1971β=10070Cum62875.
31.
1101.
10.
333s230410Vi07J2002β=529;IT=48970Cun62733.
81.
2242.
60.
56.
6s0.
21+041971β=93.
29;IT=6.
8970Zn69564.
71.
9STABLE0+041922IS=0.
6110;2β70Ga68910.
11.
221.
14m0.
031+041937β≈100;ε=0.
41670Ge70561.
80.
8STABLE0+041923IS=20.
572770As643405052.
6m0.
34(+#)041950β+=10070Asm643105032.
0080.
00296s32(+#)041979IT=10070Se61929.
91.
641.
1m0.
30+041950β+=10070Br514261579.
1ms0.
80+T=1041978β+=100;β+p70Brm49134152292.
30.
82.
2s0.
29+041981β+=;IT;β+p70Kr40950#200#52ms170+041995β+=100;β+p13PyinENSDFisfor0ν-ββdecay71Mn15200#700#5#ms(>400ns)5/2#1010Oh02I2010β;βn;β2n71Fe31000#600#28ms57/2+#1011Da08T1997β=100;βn;β2n71Co4437047080ms37/2#1005Ma95D1992β=100;βn>3171Ni55406.
22.
22.
56s0.
03(9/2+)101987β=10071Nim55406.
02.
349952.
3s0.
3(1/2)102009β=10071Cu62711.
11.
519.
4s1.
43/21010Vi07J1983β=10071Cum59955.
41.
62755.
70.
6271ns13(19/2)1098Gr14TJ1998IT=10071Zn67328.
82.
72.
45m0.
101/2101955β=10071Znm67171.
12.
4157.
71.
3MD4.
125h0.
0079/2+1012Re05T1958β≈100;IT≤0.
0571Ga70139.
10.
8STABLE3/2101923IS=39.
892971Ge69906.
50.
811.
43d0.
031/2101941ε=10071Gem69708.
10.
8198.
3540.
01420.
41ms0.
189/2+101959IT=10071As67893465.
30h0.
075/2101939β+=10071Se63146.
52.
84.
74m0.
05(5/2)101957β+=10071Sem63097.
72.
848.
790.
055.
6s0.
7(1/2)101982IT=10071Sen62886.
02.
8260.
480.
1019.
0s0.
5(9/2+)101982IT=10071Br56502521.
4s0.
6(5/2)101981β+=10071Kr46330130100ms3(5/2)101981β+=100;β+p=2.
1771Rb32300#500#5/2#p71Rbm32250#510#50#100#1/2#71Rbn32040#510#260#100#9/2+#71CuT:average99Pr10=19(3)83Ru06=19.
5(1.
6)71CumT:average98Is11=250(30)98Gr14=275(14)1198ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)72Fe28100#700#10#ms(>300ns)0+1097Be70I1997β;βn;β2n72Co39780#400#59.
9ms1.
76#1005Ma95D1992β=100;βn>62;β2n72Ni54226.
12.
21.
57s0.
050+101987β=100;βn72Cu59783.
01.
46.
63s0.
0321010Fl02J1983β=10072Cum59512.
71.
7270.
31.
01.
76s0.
03(6)101998IT=10072Zn68145.
52.
146.
5h0.
10+101951β=10072Ga68588.
30.
814.
10h0.
023101939β=10072Gam68468.
60.
8119.
660.
0539.
68ms0.
13(0+)T=1101968IT=10072Ge72585.
900.
08STABLE0+101923IS=27.
453272Gem71894.
470.
09691.
430.
04444.
2ns0.
80+101984IT=10072As68230426.
0h0.
12101939β+=10072Se67868.
22.
08.
40d0.
080+101948ε=10072Br59067778.
6s2.
41+101970β+=10072Brm589667100.
760.
1510.
6s0.
3(3)101980IT≈100;β+=72Kr53941817.
16s0.
180+1003Pi03T1973β+=10072Rb38120#500#400ns)7/2+#1010Oh02I2010β;βn;β2n73Co36900#500#41ms37/2#0411Da08T1995β=100;βn>94;β2n73Ni50108.
22.
4840ms30(9/2+)041987β=100;βn73Cu58987.
41.
94.
2s0.
33/20410Vi07J1983β=100;βn73Zn65593.
41.
923.
5s1.
0(1/2)041972β=10073Znm65397.
91.
9195.
50.
213.
0ms0.
2(5/2+)041985IT=10073Znn65355.
82.
8237.
62.
0EU5.
8s0.
8(9/2+)041998IT=;β=73Ga69699.
31.
74.
86h0.
031/20411Ch16J1949β=10073Ge71297.
520.
06STABLE9/2+041933IS=7.
751273Gem71284.
240.
0613.
28450.
00152.
92s0.
035/2+041975IT=10073Gen71230.
790.
0666.
7260.
009499ms111/2041957IT=10073As70953480.
30d0.
063/2041948ε=10073Asm705254427.
9060.
0215.
7s0.
29/2+041956IT=10073Se6822777.
15h0.
089/2+041948β+=10073Sem68201725.
710.
0439.
8m1.
33/2041960IT=72.
63;β+=27.
4373Br6364873.
4m0.
21/2041970β+=10073Kr56552727.
3s1.
03/2041972β+=100;β+p=0.
25373Krm561187433.
660.
12107ns10(9/2+)041993IT=10073Rb46080#100#25ms1/2#041993β+=100;β+p=73CoT:average11Da08(=04Sa59)=41(4)10Ho12=41(6)73CoD:βn>9(4)%isfrom05Ma95;howeverβn400ns)0+1010Oh02I2010β;βn;β2n74Co32460#600#30ms30605Ma95D1995β=100;βn>269;β2n74Ni48460#400#680ms1200+0698Fr15T1987β=100;βn74Cu5600661.
63s0.
0520610Fl02J1987β=100;βn=74Zn65756.
72.
595.
6s1.
20+061972β=10074Ga68049.
63.
08.
12m0.
1230611Ma45J1956β=10074Gam67990359.
5710.
0149.
5s1.
0(0)(+#)061974IT=7525;β74Ge73422.
4420.
013STABLE0+061923IS=36.
502074As70860.
11.
717.
77d0.
022061938β+=662;β=34274Se72213.
2020.
015STABLE0+061922IS=0.
894;2β+74Br65288625.
4m0.
3(0)061952β+=10074Brm65274613.
580.
2146m24(+#)061953β+=10074Kr62331.
82.
011.
50m0.
110+061960β+=10074Kri61790305403098Gr.
AE1998IT=10074Rb51916364.
776ms0.
0300+061977β+=100;β+p74Sr40830#100#50#ms(>1.
5s)0+061995β+;β+p74CoT:othersrecent11Da08=19(7)10Ho12=34(+6–9)D:βn=18(15)%in10Ho1274NiT:average98Fr15=900(200)98Am04=540(160)74KriE:E(g)400ns)1010Oh02I2010β;βn;β2n76Ni41610#500#236ms170+0710Ho12D1995β=100;βn=143.
676Nim39190#500#2418.
71.
0410ns50(8+)0712Ka.
BET2005IT=10076Cu509767637.
7ms5.
5(3,4)9509Wi03D1987β=100;βn=7.
2576Cum50980#200#0#200#1.
27s0.
30(1,3)9590Wi12J1990β=10076Zn62303.
01.
55.
7s0.
30+951974β=10076Ga66296.
62.
032.
6s0.
629511Ma45J1961β=10076Ge73212.
8890.
0181.
58Zy0.
170+9501Kl11T1933IS=7.
7312;2β=10076As72291.
40.
91.
0778d0.
00202951934β≈100;ε99.
4;β+200ns)1#0701Ki13I2001β+;p;β+p76NiT:symmetrizedfrom238(+15–18)76CuT:average10Ho12=599(18)05Va19=653(24)91Kr15=641(6)76CuJ:from05Va19and90Wi1276GeT:from01Kl11=1.
55(+0.
19–0.
15);otherresultsfromsamegroup:76GeT:97Gu13=1.
77(+0.
13–0.
11)94Ba15=1.
42(0.
13)76GeT:othergroups93Br22=0.
84(+0.
10–0.
08)(2σ)90Va18=0.
90(0.
10)76GeT:and90Mi23=1.
1(+0.
6–0.
3)(2σ)76GeTD:claimfor0ν-ββ01Kl13=15Yy04Kl03=11.
2Yynottrusted.
Seealso76GeTD:02Aa.
Aand02Zd0276YI:also00We.
A>170nssamegroup77Ni36750#500#124ms309/2+#1210Ho12D1995β=100;βn=3024;β2n77Cu48510#150#467.
9ms2.
15/2121987β=100;βn=30.
32077Zn58789.
22.
02.
08s0.
05(7/2+)121977β=10077Znm58016.
82.
0772.
4400.
0151.
05s0.
10(1/2)1209Pa35J1986β=667;IT=34777Ga65992.
32.
413.
2s0.
23/2()121968β=10077Ge71212.
860.
0511.
211h0.
0037/2+121939β=10077Gem71053.
150.
08159.
710.
0653.
7s0.
61/2121947β=812;IT=19277As73916.
31.
738.
79h0.
053/2121951β=10077Asm73440.
81.
7475.
480.
04114.
0s2.
59/2+121957IT=10077Se74599.
480.
06STABLE1/2121922IS=7.
631677Sem74437.
560.
06161.
92230.
001017.
36s0.
057/2+121947IT=10077Br73234.
82.
857.
04h0.
123/2121948β+=10077Brm73128.
92.
8105.
860.
084.
28m0.
109/2+121961IT=10077Kr70169.
42.
074.
4m0.
65/2+121948β+=10077Krm70102.
92.
066.
500.
05118ns123/2121975IT=10077Rb64830.
51.
33.
78m0.
043/2121972β+=10077Sr5780389.
0s0.
25/2(+)121976β+=100;β+p=0.
08377Y46780#60#63ms175/2+#1200We.
AD1999β+=;β+p;p110Ey)0+0994Sa31T1920IS=0.
3553;2β+78Rb66935317.
66m0.
030(+)091968β+=10078Rbm66888346.
840.
14910ns40(1)091996IT=10078Rbn668243111.
190.
225.
74m0.
034()091968β+=912;IT=9278Rbx66861127412R=2.
00.
5spmix78Sr631747156.
1s2.
70+0911Pe29T1982β+=10078Y52530#400#54ms5(0+)0901Ga24TJ1992β+=100;β+p78Ym52530#640#0#500#5.
8s0.
6(5+)091998β+=100;β+p78Zr41300#500#50#ms(>200ns)0+0901Ki13I2001β+;β+p78NiT:symmetrizedfrom05Ho08=110(+100–60)78CuD:βnother10Ho12=44.
0(5.
4)%78ZnmT:average12Ka.
B=321(9)00Da07=319(9)78GamE:thisislevel559.
6(0.
7)170nssamegroup79Ni27710#800#100#ms(>400ns)5/2+#1010Oh02I2010β;βn;β2n79Cu41900#400#220ms195/2#0210Ho12TD1991β=100;βn=6610;β2n79Zn53432.
32.
2995ms19(9/2+)021981β=100;βn=1.
3479Ga62547.
71.
92.
847s0.
0033/20211Ch16J1974β=100;βn=0.
0891979Ge695304018.
98s0.
03(1/2)021970β=10079Gem6934040185.
950.
0439.
0s1.
07/2+#021970β=961;IT=4179As7363659.
01m0.
153/2021950β=10079Asm728635772.
810.
061.
21s0.
01(9/2)+0298Gr14T1998IT=10079Se75917.
420.
23335ky187/2+0210Jo09T1950β=10079Sem75821.
650.
2395.
770.
033.
92m0.
011/2021950IT≈100;β=0.
0561179Br76068.
11.
3STABLE3/2021920IS=50.
69779Brm75860.
51.
3207.
610.
094.
86s0.
049/2+0209Mu15J1954IT=10079Kr74442435.
04h0.
101/2021948β+=10079Krm743124129.
770.
0550s37/2+021940IT=10079Rb70803.
02.
122.
9m0.
55/2+021957β+=10079Sr6547782.
25m0.
103/2()021972β+=10079Y5836045014.
8s0.
65/2+#021992β+=10079Zr47060#400#56ms305/2+#021999β+=100;β+p79CuT:average10Ho12=257(+29–26)91Kr15=188(25)79CuD:βnaverage10Ho12=72(12)%91Kr15=55(17)%79ZnT:other10Ho12=746(42)notusedD:βn10Ho12=2.
2(1.
4)%notused79AsmT:11Ru.
A=1.
18(0.
03)98Ho15=0.
87(0.
06)outweighed,notused79SeT:average10Jo09=327(8)07Bi01=377(19)79BrmJ:207.
2keVE3γrayto3/280Cu36430#600#210ms800510Ho12T1995β;βn;β2n80Zn51648.
62.
6550ms110+0510Ho12T1981β=100;βn=1.
0580Ga59223.
72.
92.
03s0.
09(6)0511Ve.
BTJ1974β=100;βn=0.
86780Gam59220#100#0#100#1.
4s0.
1(3)11Ve.
BTJ2011β;βn80Ge69535.
32.
129.
5s0.
40+051972β=10080As72214315.
2s0.
21+051954β=10080Se77759.
51.
2STABLE0+051922IS=49.
6141;2β80Br75889.
01.
317.
68m0.
021+051937β=91.
72;β+=8.
3280Brm75803.
21.
385.
8430.
0044.
4205h0.
00085051937IT=10080Kr77893.
30.
7STABLE0+051920IS=2.
2861080Rb72175.
51.
933.
4s0.
71+0593Al03T1961β+=10080Rbm71681.
62.
0493.
90.
51.
63s0.
04(6+)0592Do10E1980IT=10080Sr703113106.
3m1.
50+051961β+=10080Y61147630.
1s0.
54051981β+=10080Ym609196228.
50.
14.
8s0.
310501No07J1998IT=812;β+=19280Yn608346312.
60.
94.
7s0.
3(2+)051997IT=10080Zr5552014904.
6s0.
60+0501Ki13T1987β+=10080CuT:symmetrizedfrom10Ho12=170(+110–50)80ZnT:average10Ho12=578(21)91Kr15=540(30)86Gi07=550(20)86Ek01=530(20)80ZnD:βnother10Ho12400ns)5/2#1010Oh02I2010β;βn;β2n81Zn462005304ms13(5/2+)0810Pa33T1991β=100;βn=9.
124;β2n81Ga5762831.
217s0.
0055/20811Ch16J1976β=100;βn=11.
9781Ge66291.
72.
18s29/2+#081972β=10081Gem65612.
62.
1679.
140.
048s2(1/2+)081981β≈100;IT400ns)1010Oh02I2010β;βn;β2n82Zn42610#300#228ms100+0312Ma37TD1997β=100;βn=;β2n82Ga52930.
72.
4599ms2(1,2,3)0393Ru01D1976β=100;βn=21.
313;β2n82Gam52789.
72.
5141.
00.
599ns102#12Ka.
BETJ2009IT=10082Ge65415.
12.
24.
56s0.
260+111972β=10082As70103419.
1s0.
5(1+)031968β=10082Asm6997541286BD13.
6s0.
4(5)031970β=10082Se77593.
91.
497Ey50+0399Pi08T1922IS=8.
7322;2β=10082Br77497.
31.
335.
282h0.
0075031937β=10082Brm77451.
41.
345.
94920.
00106.
13m0.
052031965IT=97.
63;β=2.
4382Kr80590.
30.
9STABLE0+031920IS=11.
5933182Rb7618831.
273m0.
0021+031949β+=10082Rbm76118.
82.
669.
01.
56.
472h0.
0065031957β+≈100;IT18keV83MoT:symmetrizedfrom6(+30–3)84Zn32410#600#50#ms(>400ns)0+1010Oh02I2010β;βn;β2n84Ga44280#400#85ms100#0910Wi03D1991β=100;βn=7210;β2n84Ge581483954ms140+0993Ru01TD1972β=100;βn=10.
7684As6585434.
02s0.
03(3)(+#)0993Ru01TD1968β=100;βn=0.
28484Asm65850#100#0#100#650ms150091974β=10084Se75947.
72.
03.
26m0.
100+091960β=10084Br777832631.
76m0.
082091943β=10084Brm77470100310100BD6.
0m0.
2(6)091957β=10084Brn7737526408.
20.
4400ns)5/2+#10Oh02I2010β;βn;β2n85Ga40060#300#93ms73/2#9712Ma37TD1997β=100;βn=;β2n85Ge531234540ms505/2+#971991β=100;βn=143;β2n85As6318932.
021s0.
0103/2#971967β=100;βn=59.
42485Se72413.
62.
631.
7s0.
95/2+#971960β=10085Br7857532.
90m0.
063/2911943β=10085Kr81480.
32.
010.
776y0.
0039/2+9102Un02T1940β=10085Krm81175.
42.
0304.
8710.
0204.
480h0.
0081/2911937β=78.
64;IT=21.
4485Krn79488.
52.
41991.
81.
31.
82s0.
05(17/2+)9111Ru.
AT1989IT=10085Rb82167.
3300.
005STABLE5/2911921IS=72.
17285Rbm81653.
3220.
005514.
00830.
00191.
015s0.
0019/2+911964IT=10085Sr81103.
32.
864.
853d0.
0089/2+9102Un02T1940ε=10085Srm80864.
62.
8238.
660.
0667.
63m0.
041/2911940IT=86.
64;β+=13.
4485Y77842192.
68h0.
05(1/2)941952β+=10085Ym778221919.
80.
54.
86h0.
139/2+941952β+≈100;IT885Nb66280420.
9s0.
7(9/2+)911988β+=10085Nbm66130#80#150#80#3.
3s0.
9(1/2)9105Ka39TJ1988β+=10085Mo57510163.
2s0.
2(1/2)9797Hu15TD1992β+=100;β+p=85Tc46030#400#69keV85NbmET:759.
0(1.
0)12(5)sinNUBASE2003ismis-interpretationof98Oi0285MoJ:from05Xu0485TcI:also99Ja02300ns)1197Be70I1997β;βn;β2n86Ge49760#300#219ms400+1112Ma.
ATD1994β=100;βn86As589623945ms8111973β=100;βn=267;β2n86Se70503.
22.
514.
3s0.
30+111973β=100;βn86Br75632355.
1s0.
4(1)111962β=10086Kr83265.
6650.
004STABLE0+011920IS=17.
27941;2β86Rb82747.
010.
2018.
642d0.
0182011941β≈100;ε=0.
0052586Rbm82190.
960.
27556.
050.
181.
017m0.
0036011951IT≈100;β400ns)3/2#1010Oh02I2010β;βn;β2n87Ge44080#400#150#ms(>300ns)5/2+#0297Be70I1997β;βn;β2n87As55617.
93.
0610ms1203/2#0293Ru01T1970β=100;βn=15.
422;β2n87Se66426.
12.
25.
50s0.
125/2+#021968β=100;βn=0.
20487Br73892355.
65s0.
13(5/2)0206Po09J1943β=100;βn=2.
60487Kr80709.
520.
2576.
3m0.
55/2+021940β=10087Rb84597.
7900.
00649.
23Gy0.
223/20282Mi14T1921IS=27.
832;β=10087Sr84880.
01.
1STABLE9/2+021931IS=7.
00187Srm84491.
51.
1388.
5330.
0032.
815h0.
0121/2021940IT≈100;ε=0.
30887Y83018.
31.
679.
8h0.
31/2021940β+=10087Ym82637.
51.
6380.
820.
0713.
37h0.
039/2+021940IT=98.
4310;β+=1.
571087Zr7934741.
68h0.
01(9/2)+021948β+=10087Zrm790114335.
840.
1914.
0s0.
2(1/2)021972IT=10087Nb7387373.
75m0.
09(1/2)021971β+=10087Nbm7386973.
840.
142.
6m0.
19/2+#021972β+=10087Mo66884.
82.
914.
05s0.
237/2+#0297Hu07TD1977β+=100;β+p=15587Tc5769042.
18s0.
169/2+#0200We.
ATD1991β+=100;β+p87Tcm576834712#s1/2#09Ga40Eβ+;IT87Tcn576194711647ns247/2+#09Ga40ETJ2009IT=10087Ru45930#400#50#ms(>1.
5s)1/2#0295Ry03I1995β+;β+p87AsT:unweighedaverage93Ru01=485(40)78Cr03=730(60)(BirgeratioB=3.
4)87AsT:other12Qu01=1450(550)(+3900–1100)87RbT:average82Mi14=49.
44(0.
28)74Ne14=48.
8(0.
8)77Da22=48.
9(0.
4)obtainedby87RbT:threemethods,respectively:geochronology,decaycounting,chemical87RbT:77Da22supersedes66Mc12=47.
2(0.
4)usingthesamematerial87MoT:average97Hu07=13.
6(1.
1)91Mi15=14.
5(0.
3)83Ha06=13.
3(0.
4)87MoD:average97Hu07=15(6)%(through3levels)83Ha06=15(8)%rst2+state87TcmE:observed64keVγrayinparallelto71keVonedepopulating87Tcn87TcnE:observed71keVγray;trendof7/2+inTc:89Tc=17991Tc=39588Ge40140#500#100#ms(>300ns)0+0597Be70I1997β;βn;β2n88As50720#200#270ms1501212Qu01TD1994β=100;βn;β2n88Se6388431.
53s0.
060+081970β=100;βn=0.
673088Br70716316.
29s0.
06(2)051948β=100;βn=6.
581888Brm704463270.
11.
15.
51s0.
04(4,5)0511Ru.
AT1970IT=10088Kr79691.
32.
62.
84h0.
030+051939β=10088Rb82608.
990.
1617.
773m0.
0112051939β=10088Rbm81235.
80.
61373.
20.
6123ns137+0909Po10ETJ2000IT=10088Sr87921.
41.
1STABLE0+051923IS=82.
58188Y84298.
81.
9106.
626d0.
0214051948β+=10088Ym83905.
91.
9392.
860.
09301s31+051955IT=10088Yn83624.
31.
9674.
550.
0413.
97ms0.
188+0507Ch07J1962IT=10088Zr83628583.
4d0.
30+051951ε=10088Zrm8074052887.
790.
061.
320s0.
025(8+)051978IT=10088Nb761806014.
55m0.
06(8+)051964β+=10088Nbm76040100140120BD7.
78m0.
05(4)051971β+=10088Mo7268748.
0m0.
20+061971β+=100.
.
.
A-groupiscontinuedonnextpage.
.
.
1204ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%).
.
.
A-groupcontinued.
.
.
88Tc616801506.
4s0.
8(6+)051991β+=100;β+p88Tcm61680#340#0#300#5.
8s0.
2(3+)051993β+=100;β+p88Tcn61580#160#100#50#146ns12(4+)0909Ga40TJD2009IT=10088Ru54400#300#1.
3s0.
30+051994β+=100;β+p88AsT:symmetrizedfrom12Qu01=200(5)(+200–90)88SeT:other12Qu01=650(35)(+175–140)ms88TcmJ:09Ga40suggestthisstatetobe2+,plusexistenceofanisomer95keV88TcmJ:abovethis2+,thatdecaysbyE2,withhalf-life=146(12)ns88RuT:symmetrizedfrom01Ki13=1.
2(+0.
3–0.
2)89Ge33730#600#50#ms(>300ns)3/2+#9897Be70I1997β;βn;β2n89As46800#300#200#ms(>150ns)3/2#9894Be24I1994β;βn;β2n89Se589924410ms405/2+#981971β=100;βn=7.
82589Br6827434.
40s0.
03(3/2,5/2)981959β=100;βn=13.
8489Kr76535.
82.
13.
15m0.
043/2(+)9895Ke04J1940β=10089Rb81712515.
15m0.
123/2981940β=10089Sr86208.
71.
150.
53d0.
075/2+981937β=10089Y87709.
22.
2STABLE1/2981923IS=100.
89Ym86800.
22.
2908.
970.
0315.
663s0.
0059/2+9894It.
AT1951IT=10089Zr84876378.
41h0.
129/2+981948β+=10089Zrm842883587.
820.
104.
161m0.
0171/2981953IT=93.
7712;β+=6.
231289Nb80625242.
03h0.
07(9/2+)981954β+=10089Nbm80630#40#0#30#1.
10h0.
03(1/2)981954β+=10089Mo7501542.
11m0.
10(9/2+)981980β+=10089Mom746284387.
50.
2190ms15(1/2)981980IT=10089Tc67395412.
8s0.
9(9/2+)041991β+=10089Tcm67332462.
60.
512.
9s0.
8(1/2)041991β+≈100;IT1.
5s)7/2+#041995β+;β+p89SeT:others12Qu01=345(20)(+95–75)82Re08=560(80)89BrT:ENSDFaverages8values.
Also93Ru01=4.
348(0.
022)89KrJ:positiveparity,sincenoβtransitionto89Rbground-state89RuD:β+psymmetrizedfrom3.
0(+1.
9–1.
7)%T:otherrecent12Lo08=2.
2(1.
2)90Ge29220#700#50#ms(>400ns)0+1010Oh02I2010β;βn;β2n90As41330#600#80#ms(>300ns)0997Be70I1997β;βn;β2n90Asm41210#600#124.
50.
5220ns10012Ka.
BET2012IT=10090Se55800330210ms800+1212Qu01TD1994β=100;βn90Br6400031.
910s0.
0109893Ru01T1959β=100;βn=25.
2990Kr74959.
21.
932.
32s0.
090+981951β=10090Rb793657158s50981951β=10090Rbm792587106.
900.
03258s43981967β=97.
44;IT=2.
6490Rbx79294147112R=21fsmix90Sr85948.
92.
628.
79y0.
060+981948β=10090Y86494.
92.
264.
00h0.
212981937β=10090Ym85813.
22.
2681.
670.
103.
19h0.
067+981961IT≈100;β=0.
0018290Zr88773.
61.
8STABLE0+981924IS=51.
454090Zrm86454.
61.
82319.
0000.
010809.
2ms2.
05981972IT=10090Zrn85184.
21.
83589.
4190.
016131ns48+981977IT=10090Nb82662414.
60h0.
058+981951β+=10090Nbm825404122.
3700.
02263s26+981967IT=10090Nbn825374124.
670.
2518.
81s0.
064981969IT=10090Nbp824914171.
100.
10300ns)3/2#9997Be70I1997β;βn;β2n91Se50340#500#270ms501/2+#991975β=100;βn=2110;β2n91Br611074541ms55/2#991974β=100;βn=20391Kr70974.
02.
28.
57s0.
045/2(+)011951β=100;βn91Rb77745858.
4s0.
43/2()991951β=100;βn91Sr8365269.
63h0.
055/2+011943β=10091Y86351.
92.
658.
51d0.
061/2991943β=10091Ym85796.
32.
6555.
580.
0549.
71m0.
049/2+991953IT>98.
5;β99;IT1.
5s)7/2+#9995Ry03I1995β+;β+p91BrT:other12Qu01=615(35)(+60–50)ms91NbmD:.
.
.
;e+=0.
0028291RhT:average04De40=1.
7(0.
2)01Ki13=1.
47(0.
22);00We.
A(samegroup)=1.
74(0.
14)92As30980#700#30#ms(>300ns)0197Be70I1997β;βn;β2n92Se46720#600#100#ms(>300ns)0+0197Be70I1997β;βn;β2n92Sem44780#600#19405012s412Ka.
BET2012IT=10092Br562337343ms15(2)011974β=100;βn=33.
125;β2n92Brm555717662188ns812Ka.
BET2012IT=10092Brn5509571138185ns1012Ka.
BET2012IT=10092Kr68769.
32.
71.
840s0.
0080+041951β=100;βn=0.
03322592Rb7477364.
492s0.
0200011960β=100;βn=0.
0107592Sr8286732.
66h0.
040+031956β=10092Y8481793.
54h0.
012011940β=10092Ym8401050807503.
7s0.
511Ru.
AET2009IT=10092Zr88459.
61.
8STABLE0+011924IS=17.
15892Nb86453.
72.
434.
7My2.
4(7)+011938β+≈100;β190Ey)0+0197Ba35T1930IS=14.
5330;2β+92Mom84047.
30.
82760.
460.
16190ns38+011964IT=10092Tc7892634.
25m0.
15(8)+011964β+=10092Tcm786563270.
150.
111.
03s0.
07(4+)011976IT=10092Tcn783973529.
470.
15190Ey(2σ)92RhT:other12Lo08=5.
7(0.
1)01Ki13=5.
6(0.
5);01Xu05=3.
0(0.
8)forgs+mmixture92RhD:from12Lo0892RhmI:thisstateisnotobservedin12Lo0892PdT:symmetrizedfrom1.
0(+0.
3–0.
2)1206ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)93Se40720#800#50#ms(>300ns)1/2+#1197Be70I1997β;βn;β2n93Sem40040#800#678.
20.
7420ns10012Ka.
BET2012IT=10093Br52970450102ms105/2#111981β=100;βn=687;β2n93Kr64136.
02.
51.
286s0.
0101/2+111951β=100;βn=1.
951193Rb7262085.
84s0.
025/2111960β=100;βn=1.
39793Rbm723678253.
390.
0357s153/211FGK126J1970IT=10093Rbn6819784423.
11.
5111ns11(27/2)112010IT=10093Sr8008687.
43m0.
035/2+111959β=10093Y842281110.
18h0.
081/2111948β=10093Ym8346911758.
7190.
021820ms409/2+1107Ch07J1974IT=10093Zr87122.
71.
81.
61My0.
055/2+111950β=10093Nb87213.
01.
8STABLE9/2+111932IS=100.
93Nbm87182.
21.
830.
770.
0216.
12y0.
121/2111965IT=10093Nbn79753177460171.
5s0.
5112007IT93Mo86806.
30.
84.
0ky0.
85/2+111946ε=10093Mom84381.
40.
82424.
950.
046.
85h0.
0721/2+111950IT≈100;β+=0.
12193Mon77111179695171.
8s1.
0(39/2)112005IT93Tc83605.
41.
32.
75h0.
059/2+111948β+=10093Tcm83213.
61.
3391.
840.
0843.
5m1.
01/2111939IT=77.
46;β+=22.
6693Tcn81420.
21.
32185.
160.
1510.
2s0.
3(17/2)111973IT=10093Ru77216.
72.
159.
7s0.
6(9/2)+111972β+=10093Rum76482.
32.
1734.
400.
1010.
8s0.
3(1/2)111983β+=78.
023;.
.
.
93Run75134.
22.
32082.
50.
92.
49s0.
15(21/2)+111983IT=10093Rh69011.
82.
613.
9s1.
69/2+#111994β+=10093Pd59140#400#1.
15s0.
05(9/2+)1112Lo08TD1994β+=100;β+p=7.
5593Ag46270#500#5#ms(>1.
5s)9/2+#1195Ry03I1994p;β+;β+p93SemT:symmetrizedfrom393(+120–84)93RbmJ:253.
4keVM1(andE2)γrayto5/2;βfeedingfrom1/2+93Kr93RbmJ:lowlogftvalueisinconsistentwith5/2;inENSDFJ=(3/2,5/2)93NbnE:ENSDF2011:xkeVabove7435.
3(2.
1)37/2level;NUBASEassumesx0.
2s93AgT:estimatedhalf-lifeisforβ+decay;p-decaywouldbemuchshorter94Se36800#800#20#ms(>300ns)0+0697Be70I1997β;βn;β2n94Br47600#400#70ms20061981β=100;βn=6816;β2n94Brm47310#400#294.
50.
7530ns1512Ka.
BET2012IT=10094Kr6134812212ms50+111972β=100;βn=1.
11794Rb68562.
82.
02.
702s0.
0053()111961β=100;βn=10.
5494Rbm66487.
92.
42074.
91.
4107ns16(10)112008IT=10094Sr78845.
71.
775.
3s0.
20+111959β=10094Y82353618.
7m0.
12061948β=10094Ym8115161202.
31.
01.
295s0.
005(5+)0611Ru.
AT1999IT=10094Zr87270.
91.
9STABLE(>110Py)0+0699Ar25T1924IS=17.
3828;2β94Nb86369.
21.
820.
3ky1.
66+061938β=10094Nbm86328.
31.
840.
8920.
0126.
263m0.
0043+061962IT=99.
506;β=0.
50694Mo88412.
80.
4STABLE0+061930IS=9.
15994Tc841574293m17+061948β+=10094Tcm84081576352.
0m1.
0(2)+061948β+≈100;IT400ns)3/2+#1210Oh02I2010β;βn;β2n95Br43770#200#50#ms(>300ns)5/2#1097Be70I1997β;βn=34#;β2n95Brm43230#200#537.
90.
56.
8s1.
012Ka.
BET2012IT=10095Kr5615919114ms31/2(+)101994β=100;βn=2.
8718;β2n95Krm5596419195.
50.
31.
582s0.
022(7/2+)1012Ka.
BT2006IT=10095Rb6589420377.
7ms0.
85/2101967β=100;βn=8.
7395Rbm6505920835.
00.
6300ns)0897Be70I1997β;βn=27.
6#;β2n96Brm37850#300#311.
50.
53.
0s0.
912Ka.
BET2012IT=10096Kr530802080ms80+121994β=100;βn=3.
7496Rb613543201ms120893Ru01T1967β=100;βn=13.
37;β2n96Rbm61350#200#0#200#200#ms(>1ms)1(+#)81Bo30JI1981β;IT;βn;β2n96Rbn6021931134.
61.
11.
80s0.
04(10)0812Ka.
BT1999IT=10096Sr7293091.
07s0.
010+081971β=100;βn96Y7834265.
34s0.
050081975β=10096Ym76802715409MD9.
6s0.
28+0807Ch07J1974β=10096Zr85444.
62.
020Ey40+081934IS=2.
809;2β=10096Nb85607323.
35h0.
056+081949β=10096Mo88793.
60.
4STABLE0+081930IS=16.
671596Tc8582054.
28d0.
077+081947β+=10096Tcm85786534.
230.
0451.
5m1.
04+081950IT=98.
05;β+=2.
0596Ru86079.
10.
5STABLE(>67Py)0+0885No03T1931IS=5.
5414;2β+96Rh79686109.
90m0.
106+081967β+=10096Rhm796341051.
980.
091.
51m0.
023+081966IT=605;β+=40596Pd761824122s20+081980β+=10096Pdm7365142530.
570.
231.
81s0.
018+#0898Gr.
BTD1983IT=10096Ag64510904.
44s0.
04(8)+0812Lo08TD1982β+=100;β+p=6.
9796Agm64510#100#0#50#6.
9s0.
5(2+)0812Lo08TD2003β+=100;β+p=15.
12696Agn62050902461.
40.
3100s10(13)11Bo23TJD2011IT=10096Agp6183090268071.
543s0.
028(15+)0811Bo23ETJ2011IT=10096Agq575709069457160ns30(19+)11Bo23ETJ2011IT=10096Cd55570#400#880ms900+1012Lo08D2008β+=100;β+p=5.
54096Cdm50270#400#5300#2000#300ms11016+1011Na34TJD2011β+=100;β+p96BrmT:symmetrizedfrom2.
74(+1.
10–0.
72)96RbJ:measuredmagneticmomentconsistentwith296RbmI:non-observationin81Th04isnotincontradictionwith81Bo30experiment96RbnT:average12Ka.
B=1.
73(0.
15)11Ru.
A=1.
77(0.
05)05Pi13=2.
0(0.
1)99Ge01=1.
65(0.
15)96RuT:β+ε>67Pyandβ+β+>31Pytheorysaysmostprobableisεε96PdmT:supersedes97Gr02=1.
7(0.
1);others09Ga40=1.
76(0.
05)07My02=2.
10(0.
21)96PdmT:83Gr01=2.
2(0.
3)J:from03Ba3996AgT:average12Lo08=4.
40(0.
09)03Ba39=4.
40(0.
06)97Sc30=4.
50(0.
06)96AgD:β+paverage12Lo08=6.
5(0.
8)03Ba39=8.
5(1.
5)96AgmT:average12Lo08=6.
8(1.
0)03Ba39=6.
9(0.
6)D:average12Lo08=14(3)03Ba39=18(5)96AgnE:fromleast-squaresttoγ-rayenergiesusing11Bo23levelscheme96AgnT:other11Be34=8.
6(6.
3)susingacollectiontimeof12s96AgpE:25-50keVabovethe264313+level96AgpT:average11Bo23=1.
56(0.
03)11Be34=1.
45(0.
07)96AgqE:4265abovethe96Agp96CdT:average11Na34=670(150)10St.
A=990(130)08Ba53=1030(+240–210)96CdmT:symmetrizedfrom11Na34=290(+110–100)1208ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)97Br34060#400#10#ms(>300ns)5/2#101997β;βn;β2n97Kr4742013062.
2ms3.
23/2+#1011Ni01T1997β=100;βn=6.
76;β2n97Rb58519.
11.
9169.
1ms0.
63/2+101969β=100;βn=25.
59;β2n97Rbm58442.
02.
077.
10.
56.
3ms0.
4(5/2)12Ka.
BETJ2012IT=10097Sr685823429ms51/2+101978β=100;βn99.
3;IT400ns)1010Oh02I2010β;βn;β2n98Kr44310#300#42.
8ms3.
60+0311Ni01T1997β=100;βn=7.
010;β2n98Rb543183114ms5(0)(#)0381Th04J1971β=100;βn=13.
86;.
.
.
98Rbm53720120600120BD96ms3(3,4)(+#)031980β=100;βn;β2n98Rbn541403178.
30.
4358ns70912Ka.
BET2009IT=10098Sr664264653ms20+031971β=100;βn=0.
25598Y723018548ms2(0)031970β=100;βn=0.
3312498Ym720602824129BD2.
0s0.
2(5+,4)031977β=;IT=10#;βn=3.
41098Yn721308170.
740.
06610ns9(2)0311Ru.
AT1972IT=10098Yp718058496.
190.
156.
87s0.
05(4)0311Ru.
AT1970IT=10098Yq7112081181.
10.
4806ns21(10)0311Ru.
AT1972IT=10098Zr81293930.
7s0.
40+031967β=10098Zrm7468996603.
70.
31.
9s0.
2(17)06Si36EJT2005IT=10098Nb8353052.
86s0.
061+031960β=10098Nbm83446684451.
3m0.
4(5+)031948β≈100;IT=0.
1#98Mo88114.
80.
5STABLE(>100Ty)0+0352Fr23T1930IS=24.
3937;2β98Tc8643134.
2My0.
3(6)+031955β=100;β+=098Tcm86340390.
760.
1614.
7s0.
3(2)031976IT=10098Ru882256STABLE0+031944IS=1.
87398Rh83175128.
72m0.
12(2)+031955β+=10098Rhm83120#50#60#50#3.
6m0.
2(5+)031966IT=895;β+=11598Pd81321517.
7m0.
30+031955β+=10098Ag730703047.
5s0.
3(5+)03GAu03J1978β+=100;β+p=0.
0012598Agm7290030167.
830.
15220ns20(3+)0398Gr.
BETD1998IT=10098Cd67640509.
2s0.
30+031978β+=100;β+p0.
2s)9/2+#10St.
AI2011β+;β+p99Snm47540#510#400#100#1/2#99KrT:also11Ni01=13(+34–6)99RbT:ENSDFisweightedaverageof6scatteredresults;also11Ni01=54.
2(1.
3)99ZrmJ:130.
2γray,E2to3/2+and121.
7keV,γray,M1to1/2+99CdD:.
.
.
;β+α400ns)1010Oh02I2010β;βn;β2n101Rb42810#220#31.
8ms3.
33/2+#0611Ni01T1992β=100;βn=284;β2n101Sr5556080113.
8ms1.
7(5/2)0611Ni01T1983β=100;βn=2.
3714101Y650677426ms205/2+0607Ch07J1983β=100;βn=1.
9418101Ym647367331.
50.
7190ns4012Ka.
BETD2012IT=100101Yn6386071207.
01.
6870ns9009Fo05ETD2009IT=100101Zr7317182.
3s0.
13/2+0602Ca37J1972β=100101Nb7888847.
1s0.
3(5/2#)+061970β=100101Mo83516.
41.
114.
61m0.
031/2+061941β=100101Mom83502.
91.
113.
4970.
009226ns73/2+061977IT=100101Mon83459.
41.
157.
0150.
011133ns705/2+061977IT=100101Tc863412414.
22m0.
019/2+061941β=100101Tcm8613324207.
5260.
020636s81/2061964IT=100101Ru87954.
61.
1STABLE5/2+061931IS=17.
062101Rum87427.
01.
1527.
560.
1017.
5s0.
411/2061974IT=100101Rh8741163.
3y0.
31/2061948ε=100101Rhm872546157.
320.
034.
34d0.
019/2+061944ε=92.
8025;IT=7.
2025101Pd8543158.
47h0.
065/2+061948β+=100101Ag81334511.
1m0.
39/2+061966β+=100101Agm810605274.
10.
33.
10s0.
10(1/2)061975IT=100101Cd75836.
51.
51.
36m0.
055/2+#061969β+=100101In68610#300#15.
1s1.
19/2+#0697Sz04T1988β+=100;β+p=101Inm68060#320#550#100#10#s1/2#β+=95#;IT=5#101Sn603103001.
97s0.
16(7/2+)0712Lo08TD1994β+=100;β+p=21.
07101RbT:average11Ni01=31(+5–4)95Lh04=32(5)101SrT:average11Ni01=113(2)86Wa17=114(4)83Wo10=121(6)101YT:average96Me09=400(20)86Wa17=440(20)83Wo10=500(50)101YT:93Ru01=279(9)conicting,notused101YmT:symmetrizedfrom187(+49–38)101YnT:symmetrizedfrom860(+90–80)101YnE:fromaleast-squaresttoEgusing09Fo05levelscheme101NbJ:+duetoM1+E2γfroma+exc.
level101AgmJ:fromENSDF:E3γto(7/2)+level101InT:average97Sz04=14.
9(1.
2)88Hu07=16(3)101SnT:average12Lo08=2.
1(0.
2)07Se04=1.
3(0.
5)07Ka15=1.
9(0.
3)101SnD:β+paverage12Lo08=22(1)10St.
A=20(1)J:from10Da17102Rb37710#300#37ms3091995β=100;βn=188;β2n102Sr523607069ms60+091986β=100;βn=5.
515102Y611734&298ms9(2)0911Ha48J1983β=100;βn=4.
912102Ym60970#200#200#200#&360ms40(>5)0911Ha48J1980β=100;βn=4.
912102Zr7159492.
9s0.
20+091970β=100102Nb7631134.
3s0.
4(4+)091972β=100102Nbm762168947MD1.
3s0.
21+091976β=100102Mo83570811.
3m0.
20+091954β=100102Tc8457195.
28s0.
151+091954β=100102Tcm845511320104.
35m0.
07(4,5)091954β=982;IT=22102Ru89102.
91.
1STABLE0+091931IS=31.
5514102Rh867805207.
0d1.
5(1,2)0998Sh21T1941β+=785;β=225102Rhm866395140.
730.
093.
742y0.
0106+0999Gi14J1962β+≈100;IT=0.
23324102Pd87931.
02.
6STABLE0+091935IS=1.
021;2β+102Ag82247812.
9m0.
35(+)091960β+=100102Agm8223889.
400.
077.
7m0.
52+091967β+=515;IT=495102Cd79659.
51.
75.
5m0.
50+091969β+=100102In70694523.
3s0.
1(6+)0995Sz01J1981β+=100;β+p=0.
009313102Sn649301003.
8s0.
20+091994β+=100102Snm6291010020172367ns8(6+)0998Li50E1996IT=100102RbT:also11Ni01=35(+15–8)102SrT:also11Ni01=85(15)102YJ:in11Ha48,combining07Ch07=(2,3)withspectrocopydatafrom91Hill102RhT:average98Sh21=207.
3(1.
7)61Hi06=206(3)102SnT:95Fa.
A=4.
6(1.
4)supersedes95Sc28=4.
5(0.
7),preliminaryfromsamegroup102SnmT:from11Hi.
ANo.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1211TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)103Rb33610#400#20#ms(>400ns)3/2+#1010Oh02I2010β;βn;β2n103Sr47420#200#90ms405/2+#0911Ni01TD1997β=100;βn;β2n103Y5845811239ms125/2+#0911Ni01T1994β=100;βn=8.
017103Zr6782191.
38s0.
075/2#0909Pe06TD1987β=100;βn1.
5s104Sr44110#300#44ms80+0711Ni01TD1997β=100;βn;β2n104Y54060#400#197ms40711Ni01T1994β=100;βn=3410;β2n104Zr6573010920ms280+0709Pe06TD1990β=100;βn400ns)0+1010Oh02I2010β;βn;β2n106Y46050#500#72ms200811Ni01TD1997β=100;βn;β2n106Zr58910#200#187ms110+1109Pe06TD1994β=100;βn410Ey)0+0802Tr04T1935IS=1.
256;2β+106In80608126.
2m0.
17+081962β+=100106Inm805791228.
60.
35.
2m0.
1(2)+081966β+=100106Sn7735451.
92m0.
080+081975β+=100106Sb664737600ms200(2+)081981β+=100106Sbm663707103.
50.
3226ns14(4+)0899So08T1998IT=100106Te5822010080s130+0805Ja03T1981α=100106YT:symmetrizedfrom11Ni01=62(+25–14)106ZrT:symmetrizedfrom11Ni01=186(+11–10);othernotused09Pe06=260(+40–36)106NbT:unweighedaverage09Pe06=1240(20)96Me09=900(20)83Sh06=1020(50)106NbmT:symmetrizedfrom12Ka.
B=661(+110–97);other99Ge01=840(40)106SbmT:average99So08=232(21)98Li50=220(20)106TeT:average05Ja03=85(+25–15)94Pa11=60(+40–20)81Sc17=60(+30–10)107Sr28900#700#10#ms(>400ns)1010Oh02I2010β;βn;β2n107Y42360#500#45ms125/2+#0811Ni01TD1997β=100;βn;β2n107Zr54270#300#138ms40811Ni01T1994β=100;βn10s1/2081986IT=100107Pd88372.
51.
26.
5My0.
35/2+081958β=100107Pdm88256.
81.
2115.
740.
12850ns1001/2+081969IT=100107Pdn88157.
91.
2214.
60.
321.
3s0.
511/2081952IT=100107Ag88406.
62.
4STABLE1/2081924IS=51.
8398107Agm88313.
52.
493.
1250.
01944.
3s0.
27/2+081940IT=100107Cd86990.
21.
76.
50h0.
025/2+081946β+=100107In835641132.
4m0.
39/2+081949β+=100107Inm8288611678.
50.
350.
4s0.
61/2081973IT=100107Sn7851252.
90m0.
05(5/2+)081976β+=100107Sb7065344.
0s0.
25/2+#081994β+=100107Te60540703.
1ms0.
15/2+#081979α=7030;β+;β+p107I49570#300#20#s5/2+#α107YT:symmetrizedfrom11Ni01=41(+15–9)107ZrD:from09Pe06107NbT:average09Pe06=290(11)96Me09=300(30)91Hi02=300(10)107NbD:average09Pe06=8(1)%96Me09=6.
0(1.
5)%No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1213TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)108Y37300#600#60ms401011Ni01TD2010β=100;βn;β2n108Zr51350#400#73ms40+1111Ni01TD1997β=100;βn108Zrm49280#400#2074.
50.
5540ns30(6+)1112Ka.
BEJT2011IT≈100108Nb595468210ms5(2+)0809Pe06T1994β=100;βn=6.
25;β2n108Nbm593808166.
50.
7109ns2(4,5)12Ka.
BETJ2012IT=100108Mo7076291.
105s0.
0100+0809Pe06TD1972β=100;βn410Py)0+0895Ge14T1935IS=0.
893;2β+108In84120958.
0m1.
27+081949β+=100108Inm84090929.
750.
0539.
6m0.
72+081955β+=100108Sn82070510.
30m0.
080+081968β+=100108Sb7244557.
4s0.
3(4+)081976β+=100108Te6578252.
1s0.
10+0885Ti02D1974β+=514;α=494;.
.
.
108I5265013036ms61+#0894Pa12D1991α=;β+=9#;p400ns)5/2+#1010Oh02I2010β;βn;β2n109Zr46190#500#80ms300611Ni01TD1997β=100;βn;β2n109Nb56620530101ms95/2+#0611Ni01T1994β=100;βn=315109Nbm56310530312.
20.
5115ns812Ka.
BET2011IT=100109Mo6667211700ms145/2+#0609Pe06TD1992β=100;βn=1.
36109Mom666021169.
70.
5210ns60(1/2+)12Ka.
BET2012IT=100109Tc74281101.
14s0.
033/2#0609Pe06T1976β=100;βn=0.
082109Ru80736934.
5s1.
05/2+#061967β=100109Rum80640996.
20.
3680ns30(5/2)061976IT=100109Rh85000480s27/2+061972β=100109Rhm847744225.
9740.
0211.
66s0.
043/2+06FGK127J1987IT=100109Pd87606.
61.
113.
7012h0.
00245/2+061937β=100109Pdm87493.
21.
1113.
4000.
010380ns50.
1/2+061978IT=100109Pdn87417.
61.
1188.
9900.
0104.
696m0.
00311/2061957IT=100109Ag88719.
91.
3STABLE1/2061924IS=48.
1618109Agm88631.
91.
388.
03410.
001139.
6s0.
27/2+061967IT=100109Cd88504.
41.
5461.
4d1.
25/2+061950ε=100109Cdm88444.
91.
559.
490.
1112s21/2+061956IT=100109Cdn88040.
91.
5463.
50.
310.
9s0.
511/2061964IT=100109In8648844.
167h0.
0189/2+061948β+=100109Inm858384650.
10.
31.
34m0.
071/2061966IT=100109Inn8438642101.
80.
2209ms6(19/2+)061963IT=100109Sn82631818.
0m0.
25/2(+#)061966β+=100109Sb76251517.
0s0.
75/2+#061976β+=100109Te6771544.
6s0.
3(5/2+)061967β+=96.
113;α=3.
913;.
.
.
109I576736103s51/2+0607Ma35D1984p=100;α=0.
0144109Xe4617030013ms27/2+#06Li41TDJ2006α≈100;β+;β+p109ZrT:symmetrizedfrom11Ni01=63(+38–17)109NbT:symmetrizedfrom11Ni01=100(+9–8);others09Pe06=130(20)96Me09=190(30)109NbD:09Pe06βn600Py)0+1252Wi26T1935IS=11.
729;2β110Ag87457.
81.
324.
56s0.
111+121937β≈100;ε=0.
306110Agm87456.
71.
31.
1120.
016660ns402121975IT=100110Agn87340.
21.
3117.
590.
05249.
83d0.
046+121938β=98.
678;IT=1.
338110Cd90348.
80.
6STABLE0+121925IS=12.
4918.
.
.
A-groupiscontinuedonnextpage.
.
.
1214ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%).
.
.
A-groupcontinued.
.
.
110In86471124.
92h0.
087+121939β+=100110Inm864091262.
080.
0469.
1m0.
52+121962β+=100110Sn85842144.
154h0.
0040+121965ε=100110Sb77450623.
6s0.
3(3+)121972β+=100110Te72230718.
6s0.
80+121977β+≈100;α=0.
003#110I6046050664ms24(1+)121977β+=834;α=174;.
.
.
110Xe5192010093ms30+121981α=6435;β+;β+p110ZrT:symmetrizedfrom11Ni01=37(+17–9)110ID:.
.
.
;β+p=113;β+α=1.
13111Zr37560#700#30#ms(>400ns)1010Oh02I2010β;βn;β2n111Nb48880#300#52ms65/2+#0911Ni01TD1997β=100;βn;β2n111Mo5993813186ms91/2+#0911Ku16T1994β=100;βn400ns)0+1010Oh02I2010β;βn;β2n112Nb44270#300#35ms82+#9711Ni01TD1997β=100;βn;β2n112Mo57460#200#121ms120+9711Ni01TD1994β=100;βn112Tc652556290ms112+#9709Pe06TD1990β=100;βn=1.
52112Tcm649036352.
30.
7150ns179710Br15T2010IT=100112Ru75629101.
75s0.
070+971970β=100112Rh79730403.
4s0.
41+9799Lh01T1972β=100112Rhm793906034070BD6.
73s0.
15>39799Lh01T1987β=100112Pd86322721.
03h0.
050+971951β=100112Ag86583.
72.
43.
130h0.
0092()971938β=100112Cd90575.
80.
6STABLE0+971925IS=24.
1321112In87991414.
97m0.
101+971947β+=563;β=443112Inm878344156.
590.
0520.
56m0.
064+971953IT=100112Inn876404350.
760.
09690ns507+971976IT=100112Inp873774613.
690.
142.
81s0.
0389787Eb02J1976IT=100112Sn88656.
00.
6STABLE0+971927IS=0.
971;2β+112Sb815991851.
4s1.
03+971959β+=100112Sbm8080318796.
40.
3560ns1208#971976IT=100112Te7756882.
0m0.
20+971976β+=100112I67063103.
42s0.
111+#9778Ro19D1977β+≈100;α=0.
0012;.
.
.
112Xe6002682.
7s0.
80+9794Pa11D1978β+≈100;α=0.
98;β+p112Cs4629090490s351+#0212Ca03TD1994p≈100;α1.
3Zyforneutrinolessεεtransitionto0+3statein112Cd112ID:.
.
.
;β+p=0.
8810;β+α=0.
10412112ID:β+pandβ+αarederivedfromβ+p/α=735(80)β+p/β+α=8.
5(2),in85Ti02112XeD:αintensityisestimatedfrom94Pa11=0.
8(+1.
1–0.
5)%and78Ro19=0.
84%112CsT:average12Ca03=506(55)12Wa10=470(50)94Pa12=500(100)No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1215TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)113Nb40510#400#20#ms(>300ns)5/2+#1097Be70I1997β;βn;β2n113Mo52770#300#79ms63/2+#1011Ni01TD1994β=100;βn113Tc628123169ms185/2+#1009Pe06T1992β=100;βn=2.
13113Tcm626983114.
40.
5527ns16(5/2)12Ka.
BET2010IT=100113Ru7187040800ms50(1/2+)101988β=100113Rum717404013018510ms30(7/2)1098Ku17E1998IT=;β=113Rh7876872.
80s0.
12(7/2+)1093Pe11J1971β=100113Pd83591793s5(5/2+)101954β=100113Pdm83510781.
10.
3300ms100(9/2)101993IT=100113Ag87027175.
37h0.
051/2101949β=100113Agm869841743.
500.
1068.
7s1.
67/2+101958IT=647;β=367113Cd89043.
30.
48.
04Py0.
051/2+101925IS=12.
2212;β=100113Cdm88779.
80.
4263.
540.
0313.
89y0.
1111/21011Ko01TD1965β=99.
903619;IT=0.
096419113In89365.
80.
9STABLE9/2+101934IS=4.
295113Inm88974.
10.
9391.
6990.
0031.
6579h0.
00041/2101939IT=100113Sn88328.
21.
6115.
09d0.
031/2+101939β+=100113Snm88250.
81.
677.
3890.
01921.
4m0.
47/2+101961IT=91.
123;β+=8.
923113Sb84417176.
67m0.
075/2+101958β+=100113Te78347281.
7m0.
2(7/2+)101974β+=100113I7112086.
6s0.
25/2+#101977β+=100;α=3.
310e–7;.
.
.
113Xe6220472.
74s0.
085/2+#101973β+≈100;α≈0.
011;.
.
.
113Cs51764916.
7s0.
7(3/2+)101984p=100113MoT:symmetrizedfrom11Ni01=78(+6–5)113TcT:average09Pe06=160(+50–40)99Wa09=170(20)J:07Ku23>5/2113TcmT:otherrecent10Br15=500(100)E:other10Br15=114(1)113RumE:abovethe99keVlevelandbelow160keV113CdT:from07Be61=8.
037(0.
005)(0.
05systematics);113CdT:other09Da03=8.
00(0.
11)(syt0.
24)outweighed113CdmT:average11Ko01=13.
97(0.
13)72Wa11=14.
6(0.
5)65Fl02=13.
6(0.
2)113InmT:99.
476m23113ID:.
.
.
;β+α113XeD:.
.
.
;β+p=74;β+α≈0.
0074113XeD:α=0.
0024-0.
0204%fromestimatedlimitforthereducedwidth,see85Ti02113XeD:β+pandβ+αderivedfromβ+p/α=605(35)andβ+p/β+α=500-1500in85Ti02114Nb35390#500#15#ms(>400ns)0+122010β;βn=52.
5#;β2n=6.
2#114Mo49810#300#63ms110+121997β=100;βn114Tc58770#100#&90ms20(1+)1211Ri01TJ1994β=100;βn=114Tcm5843813330#100#&100ms20(4,5)1211Ri01TJ2011β;βn114Ru702224540ms300+1206Mo07T1991β=100;βn;β2n114Rh75710701.
85s0.
051+121988β=100114Rhm75510#170#200#150#1.
85s0.
05(7)121987β=100114Pd8349172.
42m0.
060+121958β=100114Ag8493154.
6s0.
11+121958β=100114Agm84732719951.
50ms0.
05(92Py)0+1295Ge14T1925IS=28.
7342;2β114In88568.
40.
971.
9s0.
11+121937β=99.
5015;β+=0.
5015114Inm88378.
10.
9190.
26820.
000849.
51d0.
015+121939IT=96.
7524;β+=3.
2524114Inn88066.
50.
9501.
9480.
00343.
1ms0.
68121958IT=100114Inp87926.
70.
9641.
7450.
0034.
3s0.
47+121975IT=100114Sn90557.
31.
0STABLE0+121927IS=0.
661114Snm87469.
91.
03087.
370.
07733ns147121980IT=100114Sb84496223.
49m0.
033+121959β+=100114Sbm8400122495.
50.
7219s12(8)121973IT=100114Te818892815.
2m0.
70+121968β+=100114I72800#300#2.
1s0.
21+121977β+=100;β+p114Im72530#300#265.
90.
56.
2s0.
5(7)12JBl96D1995β+=912;IT=92114Xe670861110.
0s0.
40+121977β+=100114Cs5468070570ms20(1+)121978β+≈100;α=0.
0186;.
.
.
114Ba45960110530ms2300+121995β+≈100;β+p=2010;.
.
.
114MoT:symmetrizedfrom11Ni01=60(+13–9)114TcT:others,mightbemixtureofground-stateandm:06Mo07=91(+62–35)99Wa09=150(30)114RuT:average06Mo07=510(+69–65)92Jo05=530(60)91Le09=570(50)114InpT:typoinENSDF2012:4.
3ns114ImD:evaluatedforNUBASEbyJ.
Blachot,basedon114IITdecay114CsD:.
.
.
;β+p=8.
713;β+α=0.
193114BaD:.
.
.
;α=0.
93;12C400ns)5/2+#1010Oh02I2010β;βn;β2n115Mo44750#400#90ms501011Ni01TD2010β=100;βn;β2n115Tc55910#200#85ms143/2#0711Ni01T1994β=100;βn=17#115Ru6630070322ms19(3/2+)0511Ri07J1992β=100;βn115Rum66050#120#250#100#76ms6(7/2)10Ku25TJ2010IT=100115Rh742297990ms50(7/2+)0711Ri07J1988β=100;βn115Pd804271425s2(1/2+)0510Ku19J1958β=100115Pdm803381489.
180.
2550s3(7/2)0510Ku19J1987β=92.
020;IT=8.
020115Ag849831820.
0m0.
51/2051949β=100115Agm849421841.
160.
1018.
0s0.
77/2+051958β=79.
03;IT=21.
03115Cd88084.
40.
753.
46h0.
051/2+051939β=100115Cdm87903.
40.
9181.
00.
544.
56d0.
2411/205FGK127J1959β≈100;IT15115MoT:symmetrizedfrom11Ni01=51(+79–19)115TcT:average11Ni01=83(+20–13)06Mo07=73(+32–22)115RuT:average10Ku25=318(19)06Mo07=405(+96–80);other92Ay02=740(80)115RuJ:suggestedin11Ri07fromβdecaystudy115PdJ:previously04Ur04=(3/2+)115PdmJ:E3transitiontoground-state,previously04Ur04=(9/2)115CdmJ:measuredmagneticmomentandL(d,p)=5115TemE:lessthan20keV,fromENSDF115XeD:.
.
.
;α=0.
00031116Mo41500#500#20#ms(>400ns)0+1010Oh02I2010β;βn;β2n116Tc51460#300#59ms132+#1011Ni01TD1997β=100;βn;β2n116Ru640694210ms300+101994β=100;βn116Rh7074070685ms391+1006Mo07TD1970β=100;βn400ns)1210Oh02I2010β;βn;β2n117Tc48380#400#130ms703/2#1111Ni01TD1997β=100;βn;β2n117Ru59520590143ms183/2+#1106Mo07TD1994β=100;βn=117Rum59340590184.
60.
52.
49s0.
612Ka.
BETD2012IT=100117Rh688989421ms307/2+#1106Mo07TD1991β=100;βn300ns)2+#0695Cz.
AI2010β;βn;β2n118Ru57260#300#130ms400+061994β=100;βn118Rh6488824281ms17(410)(+#)0606Mo07T1994β=100;βn=3.
114118Pd75388.
92.
51.
9s0.
10+061969β=100118Ag79553.
82.
53.
76s0.
1519593Ja03J1967β=100118Agm79508.
02.
545.
790.
090.
1s0()to2()951989IT=100118Agn79426.
22.
5127.
630.
102.
0s0.
24(+)951971β=59;IT=41118Agp79274.
42.
5279.
370.
200.
1s(2+,3+)951989IT=100118Cd867022050.
3m0.
20+951961β=100118In8722885.
0s0.
51+951949β=100118Inm87130#50#100#50#4.
364m0.
0075+9594It.
AT1964β=100118Inn86990#50#240#50#8.
5s0.
38951969IT=98.
63;β=1.
43118Sn91652.
90.
5STABLE0+951924IS=24.
229118Snm89078.
00.
52574.
910.
04230ns107951961IT=100118Snn88544.
80.
53108.
060.
222.
52s0.
06(10+)9511Fo15J1973IT=100118Sb8799633.
6m0.
11+951947β+=100118Sbm87945350.
8140.
02120.
6s0.
6(3)+951975IT=100118Sbn8774652506BD5.
00h0.
028951947β+=100118Te87697186.
00d0.
020+951948ε=100118I809712013.
7m0.
52951957β+=100118Im8078220188.
80.
78.
5m0.
5(7)9503Mo36E1968β+≈100;IT=118Xe78079103.
8m0.
90+951965β+=100118Cs684091314s22951969β+=100;β+p=0.
02114;.
.
.
118Csm68310#60#100#60#17s3(7)9593Be46J1972β+=100;β+p=0.
02114;.
.
.
118Csx684041254R400ns)3/2#1010Oh02I2010β;βn;β2n119Ru52560#300#170#ms(>300ns)0997Be70I1997β;βn;β2n119Rum52330#300#227.
10.
7384ns2212Ka.
BETD2012IT=100119Rh628239171ms187/2+#091994β=100;βn=6.
416119Pd714088920ms803/2+#0906Mo07TD1991β=100;βn=119Pdm71110#150#300#150#3#ms11/2#IT;β119Ag7864615&6.
0s0.
51/2#091975β=100119Agm78626#25#20#20#&2.
1s0.
17/2+#091975β=100119Cd83980402.
69m0.
021/2+0912Yo.
AJ1961β=100119Cdm8383040146.
540.
112.
20m0.
0211/20912Yo.
AJ1974β=100119In8770072.
4m0.
19/2+091949β=100119Inm873897311.
370.
0318.
0m0.
31/2091973β=95.
6;IT=4.
4119Inn870467654.
270.
07130ns15(3/2)+091974IT=100119Inp8504372656.
91.
8240ns25(25/2+)092002IT=100119Sn90065.
10.
7STABLE1/2+091925IS=8.
594119Snm89975.
60.
789.
5310.
013293.
1d0.
711/2091950IT=100119Snn87938.
11.
22127.
01.
09.
6s1.
2(19/2+)091992IT=100119Sb89474838.
19h0.
225/2+091947ε=100119Sbm8692082553.
60.
3130ns319/20991Io02J1991IT=100119Sbn866221128527850ms9027/2+#091979IT=100119Te87181816.
05h0.
051/2+091948ε=97.
945;e+=2.
065119Tem869208260.
960.
054.
70d0.
0411/2091960ε=99.
594;e+=0.
414;IT400ns)0+1010Oh02I2010β;βn;β2n120Ru50010#400#80#ms(>300ns)0+0295Cz.
AI2010β;βn120Rum49850#400#157.
20.
7295ns1612Ka.
BETD2012IT=100120Rh58820#200#126ms80606Mo07TD1994β=100;βn400ns)1010Oh02I2010β;βn;β2n121Rh56430#300#160ms607/2+#1006Mo07TD1994β=100;βn=121Pd661823285ms243/2+#101994β=100;βn400ns)0+1010Oh02I2010β;βn;β2n122Rum42140#500#271.
00.
7830ns12012Ka.
BETD2012IT=100122Rh52170#300#80#ms(>300ns)071997β;βn;β2n122Pd6461620175ms160+071994β=100;βn1s(3)+071987IT=100122Csn78005914030MD3.
70m0.
118071969β+=100122Csp7801030127.
070.
16360ms20(5)071969IT=100122Csx7813030147R=0.
1.
05spmix122Ba74609281.
95m0.
150+071974β+=100122La64540#300#8.
6s0.
5071984β+=100;β+p=122Ce57870#400#2#s0+072005β+;β+p122Pr44950#500#500#msβ+;β+p122RumT:symmetrizedfrom12Ka.
B=820(+130–110)122CsD:β+αintensityupperlimitisfrom75Ho091220ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)123Ru37360#500#20#ms(>400ns)1010Oh02I2010β;βn;β2n123Rh49510#400#60#ms(>400ns)7/2+#1010Oh02I2010β;βn;β2n123Pd60420#200#180ms403/2+#0406Mo07TD1994β=100;βn=123Ag6955030300ms57/2+#0406Mo07D1976β=100;βn=1.
05123Agm69530#40#20#20#100#ms1/2#β;IT123Agn6807060148150396ns37(17/2)0909St28TJ2009IT=100123Cd77414.
22.
72.
10s0.
02(3/2+)041983β=100123Cdm7727131434MD1.
82s0.
0311/2#041986β=;IT123In83430206.
17s0.
05(9/2)+041960β=100123Inm8310320327.
210.
0447.
4s0.
4(1/2)041960β=100123Inn81352202078.
10.
61.
4s0.
2(17/2)04Sc42ETJ2004IT=100123Inp81300502128.
150.
0>100s(21/2)1010Re01EJT2010IT=100123Sn87816.
42.
4129.
2d0.
411/2041948β=100123Snm87791.
82.
424.
60.
440.
06m0.
013/2+041948β=100123Snn85871.
42.
61945.
01.
07.
4s2.
6(19/2+)041992IT=100123Snp85663.
42.
72153.
01.
26s(23/2+)041994IT=100123Snq85103.
42.
82713.
01.
434s(27/2)041994IT=100123Sb89224.
82.
1STABLE7/2+041922IS=42.
795123Sbm86987.
02.
12237.
80.
3214ns319/209Wa02ETJ2005IT=100123Sbn86611.
42.
12613.
40.
465s123/2+09Wa02ETJ2007IT=100123Te89172.
11.
5STABLE(>2Py)1/2+0403Al02T1932IS=0.
893;ε=100123Tem88924.
61.
5247.
470.
04119.
2d0.
111/2041951IT=100123I87944413.
2235h0.
00195/2+041949β+=100123Xe85249102.
08h0.
021/2+0490Ne.
AJ1952β+=100123Xem8506410185.
180.
115.
49s0.
267/2()041981IT=100123Cs81044125.
88m0.
031/2+041954β+=100123Csm8088812156.
270.
051.
64s0.
12(11/2)041972IT=100123Csn807922325220114ns5(9/2+)04GAu127E2000IT=100123Csx810371374R400ns)0+1010Oh02I2010β;βn;β2n124Rh45170#400#40#ms(>400ns)1010Oh02I2010β;βn;β2n124Pd58550#300#50ms300+081997β=100;βn124Pdm58490#300#62.
21.
6>50s12Ka.
BET2012IT=100;β124Ag66200250172ms53+#081984β=100;βn=1.
39124Agm66200#270#0#100#171ms10(9)(#)0811Ba.
ATJ1995β;IT124Agn65970250231.
10.
71.
7s0.
312Ka.
BET2012IT=100124Cd76701.
73.
01.
25s0.
020+081974β=100124In80870303.
12s0.
09(1)+081964β=100124Inm80890502060BD3.
7s0.
2(8)(#)081974β≈100;IT124Sn88234.
21.
0STABLE(>100Py)0+0852Ka41T1922IS=5.
795;2β124Snm86029.
61.
02204.
6200.
023270ns60508FGK127J1979IT=100124Snn85909.
21.
02325.
010.
043.
1s0.
5708FGK127J1979IT=100124Snp85577.
61.
12656.
60.
545s510+08FGK127J1992IT=100124Snq83682.
81.
24551.
40.
7260ns251512As05EJT2012IT=100124Sb87621.
02.
160.
20d0.
033081939β=100124Sbm87610.
12.
110.
86270.
000893s55+081947IT=755;β=255124Sbn87584.
22.
136.
84400.
001420.
2m0.
2(8)081947IT=100124Sbp87580.
22.
140.
80380.
00073.
2s0.
3(3+,4+)081989IT=100124Te90525.
31.
5STABLE0+081932IS=4.
7414124I87365.
72.
44.
1760d0.
00032081938β+=100.
.
.
A-groupiscontinuedonnextpage.
.
.
No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1221TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%).
.
.
A-groupcontinued.
.
.
124Xe87661.
11.
8STABLE(>200Ty)0+081922IS=0.
09523;2β+124Cs81731830.
9s0.
41+081969β+=100124Csm812688462.
630.
146.
3s0.
2(7)+081983IT=100124Csx81701223020R=spmix124Ba790901211.
0m0.
50+081967β+=100124La7026060&29.
21s0.
17(7,8)0892Id01J1978β+=100124Lam70160#120#100#100#&21s4low(+#)0892Id01J1992β+=100124Ce64920#300#9.
1s1.
20+0897As05T1978β+=100124Pr53150#400#1.
2s0.
2081986β+=100;β+p=124Nd44530#500#500#ms0+β+;β+p124PdT:symmetrizedfrom38(+38–19)124AgmT:average11Ba.
A=172(12)and167(19)124AgmJ:feedingto8+and10+levelsin11Ba.
AwouldbeconsistentwithJ=9124AgnT:symmetrizedfrom1.
62(+0.
29–0.
24)124SnmJ:E1to4+;L(p,p)=5for124Snm;E2to5for124Snn;E2to8+for124Snp124CeT:average97As05=10.
8(1.
5)78Bo32=6(2)125Rh42210#500#20#ms(>400ns)7/2+#1110Oh02I2010β;βn;β2n125Pd54220#400#80#ms(>400ns)3/2+#1108Oh06I2008β;βn=6.
2#125Ag64230600166ms77/2+#111994β=100;βn=125Agm64210#600#20#20#50#ms1/2#β;IT125Agn62780600145350499ns21(17/2)1112Ka.
BETJ2009IT=100125Cd73348.
12.
9680ms403/2+#111986β=100125Cdm7316231864MD480ms3011/2#111986β=100125Cdn718407015127019s3(19/2+)11Si32EJT2011IT=100125In80477272.
36s0.
049/2+111967β=100125Inm8011727360.
120.
0912.
2s0.
21/2()111974β=100125Inn78468272009.
40.
79.
4s0.
6(19/2+)111998IT=100125Inp78316272161.
20.
95.
0ms1.
5(23/2)111998IT=100125Sn85896.
41.
09.
64d0.
0311/2111939β=100125Snm85868.
91.
027.
500.
149.
52m0.
053/2+111939β=100125Snn84003.
61.
01892.
80.
36.
2s0.
219/2+1108Lo07J2000IT=100125Snp83836.
91.
12059.
50.
4600ns20023/2+11FGK128J2008IT=100125Snq83272.
91.
12623.
50.
5230ns17(27/2)1108Lo07T2000IT=100125Sb88256.
32.
62.
7586y0.
00037/2+111951β=100125Sbm86285.
12.
61971.
250.
204.
1s0.
215/2112007IT=100125Sbn86144.
22.
62112.
10.
328.
0s0.
719/211FGK128J2007IT=100125Sbq85785.
32.
62471.
00.
4272ns16(23/2)+112007IT=100125Te89023.
01.
5STABLE1/2+111931IS=7.
0715125Tem88878.
21.
5144.
7750.
00857.
40d0.
1511/2111949IT=100125I88837.
21.
559.
407d0.
0105/2+111947ε=100125Xe87193.
01.
816.
9h0.
21/2(+)111950β+=100125Xem86940.
41.
8252.
610.
1456.
9s0.
99/2()111954IT=100125Xen86897.
11.
8295.
890.
15140ns307/2(+)111979IT=100125Cs84088846.
7m0.
11/2(+)111954β+=100125Csm838228266.
11.
1900s30(11/2)1198Su16J1998IT=100125Ba79669113.
3m0.
31/2(+#)111968β+=100125Bam7955923110202.
76s0.
14(7/2)11FGK128J1989IT=100125La737592664.
8s1.
211/2#111973β+=100125Lam7365226107.
000.
10390ms40(3/2+)1199Ca21J1998IT=100125Ce66660#200#9.
7s0.
3(7/2)1102Pe15J1978β+=100;β+p=125Cem66570#200#93.
60.
413s10(1/2+)1107Su07ETJ2007IT=100125Pr58030#300#3.
3s0.
73/2+#112002β+=100;β+p125Nd47600#400#650ms150(5/2)(+#)111999β+=100;β+p>0125PdI:08Oh06>400ns(BigRips)08Be33>300ns(Frs)125AgnT:otherrecent09St28=470(110)125CdnE:11Si32=1461.
8(0.
5)keVabovethe11/2isomer125SnpJ:E2to19/2+for125Snp;E2to23/2for125Snq125SbT:roundedfrom2.
75856(0.
00025)125SbnJ:E2to15/2T:othersrecent10Re01=25(4)07Ju06=25(4)125CsmT:waserroneously900(30)msinNUBASE2003125BamE:67.
7(0.
4)above5/2+#levelatestimated30#20J:E1to5/2+125LamJ:3/2+#fromtrendsinLaisotopes;lowspinandeven-parityfrom99Ca21125CemT:symmetrizedfrom134(+641–61)sforfullyionizedion;icc=38.
1fora125CemT:93.
6(0.
4)keV,E3transition;ENSDFquotes3.
4(2.
7)s1222ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)126Rh37760#500#10#ms(>400ns)1010Oh02I2010β;βn;β2n126Pd52020#500#60#ms(>400ns)0+1008Oh06I2008β;βn126Ag60780#200#55ms102+#0311Ba.
AT1994β=100;βn=126Agm60680#220#100#100#98ms98#11Ba.
AT1995β=100;IT;βn126Agn60530#200#254.
80.
5>20s12Ka.
BET2012IT=100126Cd72256.
82.
5515ms170+031978β=100126In77773271.
53s0.
013(+#)031974β=100126Inm77710507060BD1.
64s0.
058(#)0379Fo10J1970β=100126Inn7753027243.
30.
222s21()04Sc42ETJ2003IT=100126Sn8601510230ky140+031962β=100126Snm83796102218.
990.
085.
8s0.
770312As05T1979IT=100126Snn83451102564.
50.
57.
6s0.
310+0312As05TJ2000IT=100126Snp81669104345.
70.
8160ns201512As05EJT2012IT=100126Sb863903012.
35d0.
06(8)031956β=100126Sbm863703017.
70.
319.
15m0.
08(5+)031956β=864;IT=144126Sbn863503040.
40.
311s(3)031976IT=100126Sbp8629030104.
60.
3553ns5(3+)031976IT=100126Te90065.
31.
5STABLE0+031924IS=18.
8425126I87911412.
93d0.
052031938β+=52.
75;β=47.
35126Im878004111.
000.
23128ns3+12Mo.
AEJT2012IT=100126Xe891464STABLE0+031922IS=0.
08902;2β+126Cs84350101.
64m0.
021+031954β+=100126Csm8407710273.
00.
7>1s031993IT=100126Csn8375410596.
11.
1171s14031993IT=100126Ba8267012100m20+031954β+=100126La749709054s2(5)(+#)031961β+=100126Lam74760400210410BD20s20(0,1,2)031997β+=100126Ce708212851.
0s0.
30+031978β+=100126Pr60320#200#3.
12s0.
18(4,5,6)0388Ba42T1983β+=100;β+p=126Nd52990#300#1#s(>200ns)0+0300So11I2000β+;β+p126Pm39200#500#500#msβ+;β+p126SnmT:average12As05=6.
6(1.
4)10Tl01=5.
6(0.
8)126SnnT:average12As05=7.
7(0.
5)10Tl01=7.
5(0.
3)126LamT:97As05:"byfarshorterthan50s"126PrT:average95Os03=3.
14(0.
22)88Ba42=3.
0(0.
4)83Ni05=3.
2(0.
6)127Pd47440#500#40#ms(>400ns)3/2+#1210Oh02I2010β;βn;β2n127Ag58580#200#79ms37/2+#1196Wo.
ATD1995β=100;βn=127Agm58560#200#20#20#20#ms1/2#β;IT127Cd6849113370ms703/2+#111986β=100;βn127Cdm68490#100#0#100#200#ms11/2#β;IT127Cdn66930#100#1560#100#17.
5s0.
3(19/2+)10Na17ETJ2010IT=100127In76898211.
09s0.
019/2(+)1187Eb02J1975β=100;βn10s(7/2)111995IT=100127Pr64540#200#4.
2s0.
33/2+#111995β+=100127Prm63940#280#600#200#50#ms11/21198Mo30J1998β+;IT127Nd55540#300#1.
8s0.
45/2+#111983β+=100;β+p=127Pm44790#400#1#s5/2+#β+;p127AgT:supersedes95Fe12=109(25)fromsamegroup127CdnE:1560.
1(0.
5)keVabove127CdmT:other12Ka.
B=11.
0(+9.
2–3.
5)127InpE:derivedbyNUBASEfromleast-squaresttoγ-rayenergies127SbnT:also05Po03=165(20)conicting,notusedNo.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1223TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)128Pd44870#600#20#ms(>400ns)0+1010Oh02I2010β;βn128Ag54900#300#58ms5012000β=100;βn=;β2n128Cd672427280ms400+011986β=100;βn128Cdm6537271870.
50.
4270ns7(5)09Ca02ETJ2009IT=100128Cdn6452772714.
60.
53.
56s0.
06(10+)09Ca02ETJ2009IT=100128In74150150840ms60(3)+0193Ru01D1975β=100;βn=0.
0383128Inm740603080160BD720ms100(8)011986β=100128Inn73900150247.
870.
1023s2(1)0104Sc42ETJ1988IT=100128Sn833621859.
07m0.
140+011956β=100128Snm81271182091.
500.
116.
5s0.
5(7)011979IT=100128Snn80870182491.
910.
172.
69s0.
12(10+)011981IT=100128Snp792641840981220ns30(15)11Pi05ETJ2011IT=100128Sb84630199.
01h0.
048011956β=100128Sbm846201810710.
4m0.
25+011955β=96.
410;IT=3.
610128Te88993.
70.
92.
2Yy0.
30+0196Ta04T1924IS=31.
748;2β=100128Tem86203.
01.
02790.
70.
4363ns2710+0104Va03T1998IT=100128I87739424.
99m0.
021+011934β=93.
18;β+=6.
98128Im876014137.
8500.
004845ns204011982IT=100128In875724167.
3670.
005175ns15(6)011991IT=100128Xe89860.
31.
1STABLE0+011922IS=1.
91028128Cs8593253.
640m0.
0141+0193Al03T1951β+=100128Ba8537952.
43d0.
050+011950ε=100128La78630505.
18m0.
14(5+)011961β+=100128Lam78530#110#100#100#4.
0Zy)0+0196Ba24T1936IS=0.
1061;2β+130Bam84786.
62.
62475.
120.
189.
54ms0.
1480102Mo31T1969IT=100130La81627268.
7m0.
13(+)011961β+=100130Ce794232822.
9m0.
50+011965β+=100130Cem76969282453.
60.
3100ns8(7)011999IT=100130Pr711806040.
0s0.
4(6,7)(+#)0188Ba42J1977β+=100130Prm71080#120#100#100#10#s2+#0188Ba42J1988β+130Nd665962821s30+0101Gi17T1977β+=100130Pm55400#200#2.
6s0.
2(5+,6+,4+)0199Xi03J1985β+=100;β+p=130Sm47510#400#1#s0+011999β+130Eu33820#500#1.
0ms0.
4(1+)082004p≈100;β+=1#;β+p130CdmT:average12Ka.
B=248(+21–19)07Ju05=220(30)130InpT:symmetrizedfrom12Ka.
B=5.
25(+0.
40–0.
35);other04Sc42=3.
1(0.
3)130TeT:seealsonumerous(notused)resultsin95Tr07130TeT:treatedinENSDF'01asalowerlimit(notacceptedbyNUBASE)130TemT:otherconictingdata:72Ke28=115(11)J:E1to6+,E2to4+130TenE:other:lessthan25keVabove2648.
57(0.
22)(8+)level,seeENSDF'01130TenT:otherconictingdata,notused:98Zh09=4.
2(0.
9)s130BamT:others66Br14=8.
8(0.
2)69Wa.
A=13.
5(1.
0)notused130PrmJ:88Ba42:thereisalsoalow-spincomponentin130Practivity130PrmJ:seealsothediscussionin01Gi17onthreeisomericstatesin130Pr130NdT:other00Xu08=13(3)77Bo02=28(3)conicting,notused130EuT:symmetrizedfrom0.
90(+0.
49–0.
29)D:estimfromβ+half-live=49#msNo.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1225TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)131Cd55330#200#68ms37/2#0600Ha55TD2000β=100;βn=3.
510;β2n131In68025.
62.
7280ms30(9/2+)0693Ru01D1976β=100;βn=2.
23131Inm6766073668MD350ms50(1/2)061984β≈100;.
.
.
131Inn6429090374090BD320ms60(21/2+)061984β>99;.
.
.
131Inp64242.
02.
73783.
60.
5669ns34(17/2+)09Go40TJ2009IT=100131Sn77272656.
0s0.
53/2+0605Le34J1963β=100131Snm77207665.
10.
358.
4s0.
511/20604Fo06E1977β=100;IT300Ey)0+0596Ba24T1936IS=0.
1011;2β+132La83720404.
8h0.
22051951β+=100132Lam8353040188.
200.
1124.
3m0.
56051969IT=76;β+=24132Ce82471203.
51h0.
110+051960β+=100132Cem80130202341.
150.
219.
4ms0.
380509Pe31J1969IT=100132Pr75210601.
49m0.
11(2+)0594Bu18TJ1974β+=100132Prm75210#120#0#100#20#s(5+)0590Ko25J1990β+132Nd71426241.
56m0.
100+0595Bu11T1977β+=100132Pm61630#150#6.
2s0.
6(3+)051977β+=100;β+p≈5e–5132Sm55080#300#4.
0s0.
30+051989β+=100;β+p132Eu42230#400#100#ms0593Li40Dβ+;β+p;p=0132SnmT:average12Ka.
B=2.
088(0.
017)94Fo14=2.
03(4);other82Ka25=1.
7(2)132TenJ:E1to6+132PrT:average94Bu18=1.
47(0.
12)74Ar27=1.
6(0.
3)132NdT:average95Bu11=1.
47(0.
12)77Bo02=1.
75(0.
17)1226ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)133Cd43920#300#57ms107/2#112010β=100;βn=0.
47#;β2n=98.
6#133In57460#200#165ms3(9/2+)1196Ho16J1996β=100;βn=8510;β2n133Inm57130#200#330#40#180#ms(1/2)1196Ho16J1996IT;β133Sn70874.
22.
41.
46s0.
03(7/2)111973β=100;βn=0.
029424133Sb7892332.
34m0.
057/2+#111966β=100133Sbm74360100456010016.
54s0.
19(21/2+)111978IT=100133Te82932412.
5m0.
33/2+#111940β=100133Tem825984334.
260.
0455.
4m0.
4(11/2)111957β=83.
520;IT=16.
520133Ten8132241610.
40.
5100ns5(19/2)112001IT=100133I85887520.
83h0.
087/2+111940β=100133Im8425351634.
1480.
0109s2(19/2)111970IT=100133In8415851729.
1370.
010170ns(15/2)111984IT=100133Ip8345252435.
000.
23780ns1606(19/2+)112004IT=100133Iq8339352493.
70.
4469ns15(23/2+)112009IT=100133Xe87643.
62.
45.
2475d0.
00053/2+1102Un02T1940β=100133Xem87410.
42.
4233.
2210.
0152.
198d0.
01311/2111951IT=100133Cs88070.
9310.
008STABLE7/2+111921IS=100.
133Ba87553.
61.
010.
551y0.
0111/2+111941ε=100133Bam87265.
31.
0288.
2520.
00938.
90h0.
0611/21112Da04T1941IT≈100;ε=0.
01045133La85494283.
912h0.
0085/2+111950β+=100133Ce824181697m41/2+111951β+=100133Cem823811637.
20.
75.
1h0.
39/2111951β+=100133Pr77938126.
5m0.
3(3/2+)111970β+=100133Prm7774612192.
120.
141.
1s0.
2(11/2)111995IT=100133Nd723305070s10(7/2+)111977β+=100133Ndm7220050127.
970.
1270s(1/2)+1195Br24D1993β+≈100;IT=133Ndn7215050176.
100.
10301ns18(9/2)111993IT=100133Pm654105013.
5s2.
1(3/2+)111977β+=100133Pmm6528050129.
70.
78#s(11/2)111996β+;IT133Sm57230#300#2.
89s0.
16(5/2+)111977β+=100;β+p=133Smm57110#310#120#60#3.
5s0.
4(1/2)111993β+;IT;β+p133Eu47240#300#200#ms11/2#β+;β+p133Gd36020#500#10#ms5/2+#β+;β+p133CdD:delayedneutronswereobservedin05Kr20133InD:βnintensityisfrom93Ru01;delayedneutronswerealsoseenin02Di12133BamT:average12Da04=38.
88(0.
08)11Gr01=38.
92(0.
09)134In51660#300#140ms4high0495Jo.
AD1996β=100;βn=65;β2n11Py)0+0489Ba22T1920IS=10.
435721;2β134Xem86158.
80.
91965.
50.
5290ms17(7)041968IT=100134Xen85099.
11.
73025.
21.
55s1(10+)042001IT=100134Cs86891.
1540.
0162.
0652y0.
00044+041940β=100;ε=0.
00031134Csm86752.
4100.
016138.
74410.
00262.
912h0.
0028041975IT=100134Ba88950.
050.
28STABLE0+041936IS=2.
41718134Bam85992.
90.
62957.
20.
52.
63s0.
14(10+)041982IT=100134La85219206.
45m0.
161+041951β+=100134Lam84780#100#440#100#29s4041985IT=100134Ce84833203.
16d0.
040+041951ε=100134Cem81624203208.
60.
4308ns510+041980IT=100134Pr785282017m22041967β+=100134Prm784602068111m(6)0411Ti10E1973β+=100;IT≈0134Nd75646128.
5m1.
50+041970β+=100134Ndm73353122293.
00.
4410s30(8)041969IT=100134Pm6674060&22s1(5+)041977β+=100134Pmm66740#120#0#100#&5s(2+)041988β+=100134Pmn66620#80#120#50#20s1(7)09Cu02TJ2009IT=100134Sm61380#200#9.
5s0.
80+041977β+=100134Eu49930#300#500ms200041989β+=100;β+p=134Gd41300#400#400#ms0+04β+;β+p134InD:β2nintensitylimitsisfrom95Jo.
A134XeD:and>58Zyand>26Zyfor0ν-ββ0+→0+and0+→2+respectively134LamE:100#100keVabove336.
44(17)level134PmmE:70.
7(0.
2)keVabovea6+statethatdecaysviaalow-energyγto5+No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1227TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)135In46530#400#92ms109/2+#082002β;βn=95#;β2n135Sn606323530ms207/2#081994β=100;βn=213;β2n135Sb69689.
62.
91.
679s0.
015(7/2+)081964β=100;βn=223135Te77727.
92.
719.
0s0.
2(7/2)081969β=100135Tem76173.
02.
71554.
890.
16511ns20(19/2)081980IT=100135I8378956.
58h0.
037/2+081940β=100135Xe8641749.
14h0.
023/2+081940β=100135Xem858904526.
5510.
01315.
29m0.
0511/2081960IT≈100;β=0.
3017135Cs87581.
81.
02.
3My0.
37/2+081949β=100135Csm85948.
91.
81632.
91.
553m219/2081962IT=100135Ba87850.
710.
27STABLE3/2+081932IS=6.
59212135Bam87582.
490.
27268.
2180.
02028.
11h0.
0211/20812Da04T1948IT=100135La86644919.
5h0.
25/2+081948β+=100135Ce846161017.
7h0.
31/2(+)081948β+=100135Cem8417010445.
810.
2120s1(11/2)081963IT=100135Pr809361224m13/2(+)081954β+=100135Prm8057812358.
060.
06105s10(11/2)081973IT=100135Nd762141912.
4m0.
69/2()081970β+=100135Ndm761491964.
950.
245.
5m0.
5(1/2+)081970β+>99.
97;IT82)145Pm:794.
6(0.
4)147Pm:649.
3(0.
4)149Pm:240.
215(0.
007)135PmmE:ENSDF2008:68.
7+y135SmmI:existenceof135SmmandspinsofbothstatesarediscussedinENSDF135TbT:symmetrizedfrom940(+330–220)s136Sn55900#400#290ms130+0211Ar18TD1994β=100;βn=283;β2n136Sb645106923ms141#021976β=100;βn=16.
332;β2n=0.
28#136Sbm642336277.
00.
7570ns5(6)0212Ka.
BET2001IT=100136Te74425.
82.
417.
63s0.
080+021974β=100;βn=1.
315136I795451483.
4s1.
0(1)021949β=100136Im79339520615BD46.
9s1.
0(6)021959β=100;IT=0136Xe86429.
1520.
010STABLE(>10Zy)0+0202Be74T1920IS=8.
857344;2β136Xem84537.
4490.
0171891.
7030.
0142.
95s0.
096+021969IT=100136Cs86338.
91.
913.
16d0.
035+021951β=100136Csm85821.
01.
9517.
90.
117.
5s0.
280211Wi09ET1981IT=;β136Ba88887.
140.
27STABLE0+021932IS=7.
85424136Bam86856.
670.
272030.
4660.
018308.
4ms1.
97021965IT=100136Ban85529.
70.
53357.
40.
491ns2(10+)04Va03TD2004IT=100136La86040509.
87m0.
031+021950β+=100136Lam8578050259.
30.
4114ms3(7)(#)0205Bh06EJ1966IT=100136Ce86508.
60.
4STABLE(>38Py)0+0201Da22T1936IS=0.
1852;2β+136Cem83413.
10.
63095.
50.
42.
2s0.
210+021991IT=100136Pr813401113.
1m0.
12+021968β+=100136Nd791991250.
7m0.
30+021968β+=100136Pm7118070&107s6(5)(+#)02FGK12aJ1982β+=100136Pmm7107090110120BD&47s2(2)02FGK12aI1988β+=100136Pmn711107068251.
5s0.
18+#0208Ri05ET1987IT=100136Sm668111247s20+021982β+=100136Smm64546122264.
71.
115s1(8)021994IT=100136Eu56240#200#3.
3s0.
3(7+)0289Vi04D1987β+=100;β+p=0.
093136Eum56240#540#0#500#3.
8s0.
3(3+)0289Vi04D1987β+=100;β+p=0.
093136Gd49090#300#1#s(>200ns)0+0200So11I2000β+;β+p136Tb36060#500#200#ms02β+;β+p136SnT:average11Ar18=300(15)02Sh08=250(30)136SnD:βnaverage11Ar18=27(4)%02Sh08=30(5)%136SbmT:others07Si27=480(100)01Mi22=570(50)136CsmE:also83We07=518(5)136BanT:other04Sh15=94(10)outweighed136CeT:also11Be02>18Py;bothfor2ν-ββand1σ136PmJ:expected5+n9/2[514]+p1/2[550];supportedbyobserveddirectfeeding136PmJ:toI=4,5,6levelsfollowing136Pmβ+decay136PmmI:theexistenceofthislevelisuncertain136PmnE:08Ri05=42.
7(0.
2)keVabovealonγ-livedstatethatcouldbeeitherthe136PmnE:ground-stateoranexcitedlevellocated400ns)0+1010Oh02I2010β;βn;β2n138Sb54540#300#350ms152#0311Ar18TD1994β=100;βn=728;β2n138Te6569641.
4s0.
40+031975β=100;βn=6.
321138I7198066.
23s0.
03(1)0393Ru01D1949β=100;βn=5.
4618138Im71912667.
90.
51.
26s0.
16(3)0307Rz01EJT2007IT=100138Xe79972.
22.
814.
08m0.
080+031943β=100138Cs82887933.
41m0.
183031943β=100138Csm82807979.
90.
32.
91m0.
086031971IT=812;β=192138Csx82847254023R=fsmix138Ba88261.
860.
29STABLE0+031925IS=71.
69842138Bam86171.
320.
302090.
540.
06800ns1006+031971IT=100138La865223102Gy15+031947IS=0.
0888171;.
.
.
138Lam86449372.
570.
03116ns5(3)+031975IT=100138Ce8756910STABLE(>57Py)0+0311Be02T1936IS=0.
2512;2β+138Cem85440102129.
170.
128.
65ms0.
207031960IT=100138Pr83132141.
45m0.
051+031951β+=100138Prm827811835119BD2.
12h0.
047031958β+=100138Nd82018125.
04h0.
090+031965β+=100138Ndm78843123174.
90.
4410ns5010+031975IT=100138Pm749402810s21+#031981β+=100138Pmm74911133030BD3.
24m0.
055#031973β+=100138PmnnonexistentEU3.
24m0.
05(3+)81De38Iβ+=100138Sm71498123.
1m0.
20+031982β+=100138Eu617502812.
1s0.
6(6)031982β+=100138Gd55660#200#4.
7s0.
90+031985β+=100138Gdm53430#200#2233.
10.
56.
2s0.
2(8)0311Pr02T1997IT=100138Tb43670#300#800#ms(>200ns)0300So11I1993β+;β+p;p=0138Dy34930#400#200#ms0+β+;β+p138IJ:from07Rz01138ImE:unc.
assignedbyevaluatorJ:67.
9E2γray(delayed)to(1)138LaD:.
.
.
;β+=65.
65;β=34.
45138CeT:also01Da22>150Ty;bothfor2ν-ββand1σ138PmnD:argumentsforasecondisomerofintermediatespinarenotconvincing138GdmE:forleast-squaresttoγ-rayenergiesin11Pr02138TbD:from93Li40No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1229TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)139Sb49790#400#93ms137/2+#0111Ar18TD1994β=100;βn=9010;β2n139Te602054500#ms(>150ns)5/2#0194Be24I1994β;βn139I68459292.
282s0.
0107/2+#0193Ru01T1949β=100;βn=10.
03139Xe75644.
62.
139.
68s0.
143/2011951β=100139Cs8070139.
27m0.
057/2+011939β=100139Ba84913.
970.
2983.
25m0.
08(7/2)0112Da04T1937β=100139La87228.
62.
3STABLE7/2+011924IS=99.
9111971139Lam85428.
72.
41799.
90.
5315ns35(17/2+)12As06T2012IT=100139Ce869507137.
641d0.
0203/2+011948ε=100139Cem861967754.
240.
0856.
54s0.
1311/20194It.
AT1967IT=100139Pr8482184.
41h0.
045/2+011951β+=100139Nd820152829.
7m0.
53/2+011951β+=100139Ndm8178428231.
150.
055.
50h0.
2011/2011951β+=88.
24;IT=11.
84139Ndn79400#60#2620#50#272ns40108Fe02T1980IT=100139Pm77501144.
15m0.
05(5/2)+011967β+=100139Pmm7731214188.
70.
3180ms20(11/2)011975IT≈100;β+=0.
16#139Sm72380112.
57m0.
101/2+011971β+=100139Smm7192311457.
400.
2210.
7s0.
611/2011973IT=93.
75;β+=6.
35139Eu653981317.
9s0.
6(11/2)011975β+=100139Eum6525013148.
20.
210s2(7/2+)11Cu01ETJ2011IT=100139Gd57630#200#5.
7s0.
39/2#0199Xi04T1983β+=100;β+p=139Gdm57380#250#250#150#4.
8s0.
91/2+#011983β+=100;β+p=139Tb48130#300#1.
6s0.
211/2#011999β+=100;β+p139Dy37640#500#600ms200(7/2+)011999β+=100;β+p139IT:average93Ru01=2.
280(0.
011)80Al15=2.
29(0.
02)139BaT:average12Da04=83.
25(0.
08)72Em01=82.
71(0.
18)62Fr04=82.
9(0.
2)139BaT:othernotused80Ge04=83.
06(0.
28)139NdnT:80Mu10>141nsE:50#50keVabove2570.
9(0.
6)level139GdT:average99Xi04=5.
8(0.
9)88Be.
A=5.
8(0.
4);other83Ni05=4.
9(1.
0)notused139GdT:sinceitcorrespondstoamixtureofground-stateandisomer139GdmD:assumingthatthedelayedprotonsreportedin83Ni05arefrombothstates140Sb43940#600#100#ms(>400ns)2#1010Oh02I2010β;βn=50#;β2n=16#140Te5635728300#ms(>300ns)0+071994β;βn140I63600180860ms40(4)071972β=100;βn=9.
310;β2n140Xe72986.
52.
313.
60s0.
100+071951β=100140Cs77050863.
7s0.
31071950β=100140Csm77036813.
9310.
021471ns51(2)071974IT=100140Ba83270812.
7527d0.
00230+071939β=100140La84318.
22.
340.
285h0.
0033071935β=100140Ce88079.
22.
2STABLE0+071925IS=88.
45051140Cem85971.
32.
22107.
860.
037.
3s1.
56+071966IT=100140Pr8469163.
39m0.
011+071938e+=51.
318;ε=48.
718140Prm845636127.
80.
3350ns205+071964IT=100140Prn839276763.
70.
53.
05s0.
20(7)071964IT=100140Nd84254263.
37d0.
020+071949ε=100140Ndm82033262221.
40.
1600s507071962IT=100140Ndn76824267429.
60.
71.
23s0.
0720+08Fe02ETJ2008IT=100140Pm78210409.
2s0.
21+071966β+=100140Pmm777821343040BD5.
95m0.
058071966β+=100140Sm754561214.
82m0.
120+071967β+=100140Eu66990501.
51s0.
021+071982β+=100140Eum667805021015125ms2(5)071988IT≈100;β+150ns)5/2#0194Be24I1994β;βn;β2n141I59900#200#430ms207/2+#011974β=100;βn=213141Xe68197.
32.
91.
73s0.
015/2(#)011951β=100;βn=0.
0445141Cs74477924.
84s0.
167/2+011962β=100;βn=0.
0353141Ba79733518.
27m0.
073/2011945β=100141La8293543.
92h0.
03(7/2+)011951β=100141Ce85436.
02.
232.
508d0.
0137/2011948β=100141Pr86016.
42.
1STABLE5/2+011924IS=100.
141Nd8419342.
49h0.
033/2+011949β+=100141Ndm834364756.
510.
0562.
0s0.
811/20170Ab05D1960IT≈100;β+=0.
0328141Pm805231420.
90m0.
055/2+011952β+=100141Pmm7989514628.
400.
10630ns2011/2011970IT=100141Pmn77992142530.
90.
5>2s011985IT=100141Sm75934910.
2m0.
21/2+011967β+=100141Smm757589176.
00.
322.
6m0.
211/2011967β+≈100;IT=0.
313141Eu699261340.
7s0.
75/2+011977β+=100141Eum698301396.
450.
072.
7s0.
311/2011973IT=863;β+=143141Gd632242014s4(1/2+)011986β+=100;β+p=0.
031141Gdm6284620377.
80.
224.
5s0.
5(11/2)011986β+=892;IT=112141Tb545401103.
5s0.
2(5/2)011986β+=100141Tbm54540#230#0#200#EU7.
9s0.
611/2#0188Be.
AI1988β+=100141Dy45380#300#900ms140(9/2)0106Xu03T1984β+=100;β+p=141Ho34360#500#4.
1ms0.
3(7/2)021998p=;β+=1#;β+p141Hom34290#500#6627.
28s0.
28(1/2+)0201Se03ET1998p=100141ID:roundedfrom21.
230;80Al15=21.
2(3.
0)includedin93Ru01=22(3)141EumD:symmetrizedfromIT=87(+2–4)%andβ+=13(+4–2)%141GdJ:weakargumentsinENSDF'2001forJpiassignment;samefor141Gdm141TbmI:existencediscussedin88Be.
A.
Provisionallyaccepted141DyT:average06Xu03=900(200)86Wi15=900(200)141HoD:fromestimatedβ+half-life200#ms141HomT:average08Ka16=7.
4(0.
3)01Se03=6.
5(+0.
9–0.
7);othernotused99Ry04=8(3)142Te46370#500#100#ms(>150ns)0+1194Be24I1994β;βn;β2n142I54770370222ms122#111975β=100;βn=25#;β2n142Xe65229.
62.
71.
23s0.
020+111960β=100;βn=0.
216142Cs7051871.
684s0.
0140111962β=100;βn=0.
0904142Ba77843610.
6m0.
20+111959β=100142La80024691.
1m0.
52111953β=100142Lam798786145.
820.
08870ns170(4)111983IT=100142Ce84532.
72.
7STABLE(>50Py)0+111925IS=11.
11451;α;2β142Pr83788.
32.
119.
12h0.
042111935β≈100;ε=0.
01648142Prm83784.
62.
13.
6940.
00314.
6m0.
55111967IT=100142Nd85949.
91.
8STABLE0+111924IS=27.
15240142Pm811422440.
5s0.
51+111959e+=77.
127;ε=22.
927142Pmm8025924883.
170.
162.
0ms0.
2(8)111971IT=100142Pmn78313242828.
70.
667s5(13)111974IT=100142Sm78987372.
49m0.
050+111959β+=100142Smm7661532372.
10.
4170ns27111975IT=100142Smn7532533662.
20.
7480ns6010+111979IT=100142Eu71310302.
36s0.
101+1191Fi03T1966β+=100142Eum708561246030BD1.
223m0.
0088111966β+=100142Gd669602870.
2s0.
60+111986ε=525,e+=485142Tb56560700597ms171+111991β+=100;β+p=0.
002211142Tbm56280700279.
70.
4303ms175111986IT=100142Tbn55910700652.
10.
626s18+111989IT=100142Dy50120#730#2.
3s0.
30+111986β+=100;β+p=0.
063142Ho37250#500#400ms100(7,8+)112001β+≈100;β+p=;p≈0142Er27850#500#10#s0+p142XeD:03Be05=0.
21(6)75As04=0.
406(0.
034)T03Be05=1.
250(0.
025)142BaD:βn=0.
091(0.
003)%inENSDF'00contradictsQ(βn)=–2979(7)keV142CeT:lowerlimitisforαdecay;forββdecay11Be02>300Py01Da22>260Py142PmT:other:09Wi09=56(3)forq=61+(bareion)39.
2(0.
7)forq=60+142PmT:(H-likeion)and39.
6(1.
4)forq=59+(He–likeion)142PmD:e+=71.
0(1.
3)%;ε=29.
0(1.
3)%forq=60+(H-likeion)and142PmD:e+=79.
8(1.
0)%;ε=20.
2(1.
0)%forq=59+(He–likeion)142EuT:average91Fi03=2.
34(0.
12)75Ke08=2.
4(0.
2)142HoD:p=0from93Li40No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1231TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)143Te40280#500#100#ms(>400ns)7/2+#122010β;βn;β2n143I50630#300#130ms457/2+#121994β;βn=40#;β2n143Xe602035511ms65/21203Be05D1951β=100;βn=1.
0015143Cs67674221.
791s0.
0073/2+121962β=100;βn=1.
647143Ba73937714.
5s0.
35/2121962β=100143La78171714.
2m0.
1(7/2)+121951β=100143Ce81606.
22.
733.
039h0.
0063/2121948β=100143Pr83068.
02.
213.
57d0.
027/2+121948β=100143Nd84002.
11.
8STABLE7/2121933IS=12.
17426143Pm829603265d75/2+121952ε=100;e+200ns)11/2#1200So11I2000β+;β+p143Er31090#400#200#ms9/2#12β+;β+p143SmnJ:E3to17/2+143GdD:78Fi02:β+pand/orβ+αfor143Gd+143Gdm=0.
001%,39particlesdetected143GdmJ:from05Ba64143DyT:03Xu04=5.
6(1.
0);84Ni03=3.
2(0.
6)83Ni05=4.
1(0.
3)indiff.
experiments143DynE:95.
6(0.
5)above11/2isomer144I45280#400#100#ms(>150ns)1#0194Be24I1994β;βn=40#;β2n144Xe568725388ms70+0103Be05TD2003β=100;βn=3.
03144Cs6327125994ms61()101967β=100;βn=3.
0313144Csm631792592.
20.
51.
1s0.
1(4)102009IT=100144Csn62970#200#300#200#3)101978β=;IT144Ba71767711.
5s0.
20+011967β=100144La748501340.
8s0.
4(3)011967β=100144Ce804323284.
91d0.
050+011945β=100144Pr80750317.
28m0.
050011951β=100144Prm80691359.
030.
037.
2m0.
33011970IT≈100;β=0.
07144Nd83747.
91.
82.
29Py0.
160+011924IS=23.
79819;α=100144Pm814163363d1450194Hi05D1952ε=100;e+200ns)0+062003β+144Tm22090#400#2.
3s0.
9(10+)082005p=;β+=0#144BaD:βn=3.
6(0.
7)%inENSDF'01belongsinfactto144Cs;βnnotallowed144EumJ:E2to6144TbmT:other03Li42=12(2)sforq=65+(bareion)144TmT:symmetrizedfrom1.
9(+1.
2–0.
5)s1232ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)145I40940#500#100#ms(>400ns)7/2+#1010Oh02I2010β;βn;β2n145Xe5149311188ms43/2#092003β=100;βn=5.
06;β2n145Cs6005611582ms63/2+0993Ru01T1971β=100;βn=14.
79145Ba6751684.
31s0.
165/2091974β=100145La728351224.
8s2.
0(5/2+)091974β=100145Ce77070303.
01m0.
065/2#091954β=100145Pr7962675.
984h0.
0107/2+091954β=100145Nd81431.
81.
8STABLE7/2091933IS=8.
29312145Pm81267317.
7y0.
45/2+091951ε=100;α=2.
8e–7145Sm80651.
22.
0340d37/2091947ε=100145Smm71865.
02.
18786.
20.
7990ns170(49/2+)091993IT=100145Eu7799235.
93d0.
045/2+091951β+=100145Eum772763716.
00.
3490ns3011/2091975IT=100145Gd729242023.
0m0.
41/2+091959β+=100145Gdm7217520749.
10.
285s311/2091969IT=94.
35;β+=5.
75145Tb66300100&30.
9s0.
6(11/2)091981β+=100145Tbm65540200760220BD&(3/2+)091993β+145Dy5824379.
5s1.
0(1/2+)0993Al03T1982β+=100;β+p=145Dym581257118.
20.
214.
1s0.
7(11/2)091982β+=100;β+p≈50145Ho4912072.
4s0.
111/2#091987β+=100145Hom49020#100#100#100#100#ms5/2+#β+;IT145Er39080#200#900ms3001/2+#091989β+=100;β+p=145Erm38870#200#2054p1.
0s0.
311/2#10Ma20T2010β+145Tm27580#200#3.
17s0.
20(11/2)091998p=100145CsT:average93Ru01=579(6)82Ra13=594(13)145SmmT:symmetrizedfrom960(+190–150)145DyT:average93Al03=10.
5(1.
5)93To04=6(2)84Sc.
C=10(1)145ErT:89Vi02=900(300)formixturegs+isomer;similarly900(200)from10Ma20146Xe4795524146ms60+9703Be05TD1989β=100;βn=6.
915146Cs5557040323ms619793Ru01T1971β=100;βn=14.
25;β2n146Ba64940202.
22s0.
070+9793Ru01D1970β=100146La69050306.
27s0.
1029793Ru01D1970β=100146Lam6892013013013010.
0s0.
1(6)9779Ke02E1969β=100146Ce756351613.
52m0.
130+971953β=100146Pr766803024.
15m0.
18(2)971953β=100146Nd80925.
81.
8STABLE0+971924IS=17.
18932;2β;α146Pm7945445.
53y0.
053991960ε=66.
013;β=34.
013146Sm80996368My70+9712Ki16T1953α=100146Eu7711764.
61d0.
034971957β+=100146Eum764516666.
370.
16235s39+971962IT=100146Gd76086448.
27d0.
100+011957ε=100146Tb67760408s41+971974β+=100146Tbm67610#110#150#100#24.
1s0.
559793Al03T1974β+=100146Tbn66830#110#930#100#1.
18ms0.
02(10+)971989IT=100146Dy62555733.
2s0.
70+9793Al03T1981β+=100146Dym5961972935.
70.
6150ms20(10+)97FGK128J1982IT=100146Ho5123872.
8s0.
5(6)9710Ma37TJ1982β+=100;β+p=146Er4432271.
7s0.
60+9793To05D1993β+=100;β+p=146Tm30890#200#155ms20(1+)05Ro40TJD1993p≈100;β+;β+p146Tmm30590#200#3046p75ms7(5)0206Ta08TJ1993p≈100;β+;β+p146Tmn30460#200#4377p200ms3(10+)0206Ta08TJ1993p=;β+=16#;β+p146CsT:average93Ru01=321(2)76Lu02=343(7)146BaD:93Ru01βn400ns)0+1010Oh02I2010β;βn;β2n148Cs47300580146ms6001978β=100;βn=25.
125;β2n148Ba5759060612ms170+001979β=100;βn=0.
43148La62709191.
26s0.
08(2)001982β=100;βn=0.
153148Ce703981156s10+001964β=100148Pr72535152.
29m0.
021001964β=100148Prm72490#30#50#30#2.
01m0.
07(4)00GAuE1964β=100148Nd77407.
82.
4STABLE(>3.
0Ey)0+0082Be20T1937IS=5.
75621;2β;α148Pm7686565.
368d0.
0021001947β=100148Pmm767276137.
90.
341.
29d0.
115,6001951β=95.
86;IT=4.
26148Sm79336.
11.
87Py30+001933IS=11.
2410;α=100148Eu762991054.
5d0.
55001951β+=100;α=9.
4e–728148Eum7557910720.
40.
3162ns89+001980IT=100148Gd76269.
31.
970.
9y1.
00+0003Fu10T1953α=100;2β+148Tb705311360m12001960β+=100148Tbm704411390.
10.
32.
20m0.
05(9)+001973β+=100148Tbn61912138618.
61.
01.
310s0.
007(27+)001980IT=100148Dy6785393.
3m0.
20+001974β+=100148Dym6493492919.
11.
0471ns2010+001978IT=100148Ho57990802.
2s1.
1(1+)111979β+=100148Hom57740#130#250#100#9.
49s0.
125#()1193Al03T1979β+=100;β+p=0.
081148Hon57050#130#940#100#2.
36ms0.
06(10)+111984IT=100148Er51479104.
6s0.
20+111982β+=100;β+p≈0.
15148Erm48566102913.
20.
413s3(10+)111982IT=100148Tm3876510700ms200(10+)111982β+=100;β+p148Yb30200#600#250#ms0+β+;β+p148PrmE:derivedfromENSDFestimateE50ms)3/2+#041979β;βn;β2n149Ba53020#200#344ms73/2#041993β=100;βn=0.
4312149La602202001.
05s0.
03(3/2)071979β=100;βn=1.
4328149Ce66670105.
3s0.
23/2#041974β=100149Pr71039102.
26m0.
07(5/2+)041964β=100149Nd74375.
32.
41.
728h0.
0015/2041938β=100149Pm76063.
72.
553.
08h0.
057/2+041947β=100149Pmm75823.
52.
5240.
2140.
00735s311/2041966IT=100149Sm77135.
11.
7STABLE(>2Py)7/2041933IS=13.
827;α149Eu76440493.
1d0.
45/2+041959ε=100149Eum759444496.
3860.
0022.
45s0.
0511/2041961IT=100149Gd7512749.
28d0.
107/2041951β+=100;α=4.
3e–410149Tb7148944.
118h0.
0251/2+041950β+=83.
317;α=16.
717149Tbm71453435.
780.
134.
16m0.
0411/2041962β+≈100;α=0.
0223149Dy6769994.
20m0.
147/2()0488Ah02J1958β+=100149Dym6503892661.
10.
4490ms15(27/2)041976IT=99.
33;β+=0.
73149Ho616621421.
1s0.
2(11/2)041979β+=100149Hom616131448.
800.
2056s3(1/2+)041988β+=100149Er53742284s2(1/2+)041984β+=100;β+p=72149Erm5300028741.
80.
28.
9s0.
2(11/2)041984β+=96.
57;IT=3.
57;.
.
.
149Ern51131282611.
10.
3610ns80(19/2+)041987IT=100149Erp50470303272204.
8s0.
1(27/2)041987IT=100149Tm43880#300#900ms200(11/2)041987β+=100;β+p=0.
2615149Yb33200#500#700ms200(1/2+)0405Xu04J2001β+=100;β+p≈100149DymT:other03Li42=11(1)sforq=66+(bareion)149ErmD:.
.
.
;β+p=0.
187149ErpE:3242.
7+30(20)keV149TmD:symmetrizedfromβ+p=0.
2(+0.
2–0.
1)%149YbJ:(1/2+,3/2+)inENSDF2004and1/2in05Xu04;06Xu07=(1/2)however,149YbJ:no1/2ground-stateorisomerfore–ointhisregion150Cs38820#300#100#ms(>50ms)9787Ra12I1979β;βn;β2n150Ba50250#300#300ms0+951994β=100;βn150La56380#200#510ms30(3+)9795Ok02TJ1993β=100;βn=2.
73150Ce64847124.
0s0.
60+951970β=100150Pr6830096.
19s0.
16(1)961970β=100150Nd73679.
11.
76.
7Ey0.
70+9697De40TD1937IS=5.
63828;2β=100150Pm73596202.
68h0.
02(1)951952β=100150Sm77050.
51.
7STABLE0+961934IS=7.
381150Eu74792636.
9y0.
95()951950β+=100150Eum74750642.
10.
512.
8h0.
10951953β=892;β+=112;.
.
.
150Gd7576461.
79My0.
080+961953α=100;2β+150Tb7110673.
48h0.
16(2)961959β+≈100;α200ns)0+9700So11I2000β+150Lu24640#500#46ms6(5,6)0200Gi01J1993p=;β+=30#150Lum24620#500#225p40s7(1+,2+)0200Gi01J1998p=100150NdT:from6.
75(+0.
37–0.
68statistics+0.
68systematics)150EumD:.
.
.
;IT≤5e–8150HoT:average93Al03=78(2)82No08=72(4)150HonE:7912.
4(2.
1)keVabovethe(9)+isomerfromttoγ-rayenergies150TmmT:average96Ga24=2.
22(0.
07)88Ni02=2.
15(0.
10)87To05=2.
2(0.
2)150TmmT:82No08=3.
5(0.
6)conicting,notusedD:from88Ni02150TmnE:671.
6keVabove150Tmm,fromENSDF150LumT:symmetrizedfrom39(+8–6)No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1235TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)151Cs34860#400#60#ms(>50ms)3/2+#091979β;βn=85.
9#;β2n=0.
4#151Ba45390#300#200#ms(>300ns)3/2#091994β;βn151La53730#200#300#ms(>300ns)5/2+#091994β;βn=5.
8#151Ce61225181.
76s0.
06(3/2)0910Si03J1997β=100151Pr667791218.
90s0.
07(3/2)091990β=100151Prm667441235.
100.
1050s8(7/2+)0912Ma03T2006IT=100151Nd70942.
31.
712.
44m0.
073/2+091938β=100151Pm73385528.
40h0.
045/2+091952β=100151Sm74575.
61.
790y85/2091947β=100151Smm74314.
51.
7261.
130.
041.
4s0.
1(11/2)091973IT=100151Eu74652.
01.
7STABLE(>1.
7Ey)5/2+091933IS=47.
816;α151Eum74455.
81.
7196.
2450.
01058.
9s0.
511/2091958IT=100151Gd741883123.
9d1.
07/2091950ε=100;α=1.
0e–66151Tb71623417.
609h0.
0011/2(+)091953β+≈100;α=0.
009515151Tbm71523499.
530.
0525s3(11/2)091978IT=93.
420;β+=6.
620151Dy68752317.
9m0.
37/2()091959β+=;α=5.
64151Ho63623835.
2s0.
111/2()0987Ne.
AJ1963β+=;α=223151Hom63582841.
00.
247.
2s1.
31/2(+)0987Ne.
AJ1963α=7718;β+151Er582661623.
5s2.
0(7/2)091970β+=100151Erm55680162586.
00.
5580ms20(27/2)091980IT=95.
33;β+=4.
73151Ern479791610286.
61.
0420ns50(65/2,61/2+)0909Fu05J1990IT=100151Tm50778204.
17s0.
11(11/2)091982β+=100151Tmm5068420946AD6.
6s2.
0(1/2+)091987β+=100151Tmn48122202655.
670.
22451ns34(27/2)091982IT=100151Yb415403001.
6s0.
5(1/2+)0986To12T1985β+=100;β+p=151Ybm40790#320#750#100#1.
6s0.
5(11/2)0986To12T1986β+≈100;β+p=;IT=0.
4#151Ybn39000#580#2540#500#2.
6s0.
719/2#091993IT=100151Ybp39090#580#2450#500#20s127/2#091987IT=100151Lu30110#400#80.
6ms2.
011/2#091982p=;β+=37#151Lum30030#400#775p16s13/2+#091998p=100151CeI:isomerwithT=1.
02(0.
06)suggestedinENSDF2009nottrustedbyNUBASE151GdD:symmetrizedfromα=0.
8(+0.
8–0.
4)e–6%151HomD:symmetrizedfromα=80(+15–20)%151ErmT:other03Li42=19(3)sforq=68+(bareion)151YbT:derivedfrom1.
6(0.
1),formixtureofground-stateandisomerwithalmostsamehalf-life151YbmE:740#estimatedin90Ak01(seeENSDF'09)151YbnE:abovethe1791.
2keVlevelabove151Ybm(seeENSDF'09)151YbpE:2448keVabove151Ybm(seeENSDF'97)151LuD:p=63.
4(0.
9)%inENSDF'09,basedonpredictedβ+decayhalf-life≈220ms152Ba42090#400#100#ms(>400ns)0+1010Oh02I2010β;βn152La49540#300#200#ms(>150ns)9794Be24I1994β;βn152Ce59060#200#1.
1s0.
30+9790Ta07T1990β=100152Pr63758193.
63s0.
124+9799To04J1983β=100152Nd701492511.
4m0.
20+971969β=100152Pm71254264.
12m0.
081+971958β=100152Pmm711108014090BD7.
52m0.
084971971β=100152Pmn71000#150#250#150#13.
8m0.
2(8)971971β≈100;IT=152Sm74762.
01.
6STABLE0+971933IS=26.
7516152Eu72887.
41.
713.
537y0.
0063971938β+=72.
13;β=27.
93152Eum72841.
81.
745.
59980.
00049.
3116h0.
00130971958β=724;β+=284152Eun72822.
11.
765.
29690.
0004940ns801971978IT=100152Eup72809.
21.
778.
23310.
0004165ns101+971978IT=100152Euq72797.
61.
789.
84960.
0004384ns104+971970IT=100152Eur72739.
51.
7147.
860.
1096m18971963IT=100152Gd74706.
31.
6108Ty80+971938IS=0.
201;α=100;2β+152Tb707204017.
5h0.
12981959β+=100;α150ns)5/2+#0694Be24I1994β;βn153Ce55020#200#500#ms(>150ns)3/2#0694Be24I1994β;βn153Pr61568124.
28s0.
115/2#061987β=100;βn153Nd67330.
32.
731.
6s1.
0(3/2)061987β=100153Ndm67138.
62.
9191.
71.
01.
10s0.
04(5/2+)0610Si03TJ1996IT=100153Pm7064895.
25m0.
025/2061962β=100153Sm72559.
11.
646.
284h0.
0043/2+061938β=100153Smm72460.
71.
698.
370.
1010.
6ms0.
311/2061971IT=100153Eu73366.
31.
7STABLE5/2+061933IS=52.
196153Eum71595.
31.
71771.
00.
4475ns1019/2062000IT=100153Gd72881.
91.
6240.
4d1.
03/2061947ε=100153Gdm72786.
71.
695.
17360.
00083.
5s0.
49/2+061979IT=100153Gdn72710.
71.
6171.
1880.
00476.
0s1.
4(11/2)061967IT=100153Tb7131342.
34d0.
015/2+061957β+=100153Tbm711504163.
1750.
005186s411/2061965IT=100153Dy6914346.
4h0.
17/2()061958β+≈100;α=0.
009414153Ho6501252.
01m0.
0311/2061963β+≈100;α=0.
05125153Hom64943568.
70.
39.
3m0.
51/2+061963β+≈100;α=0.
188153Hon6224011277210229ns2(31/2+)061980IT=100153Er604721037.
1s0.
27/2()0685Ah.
AJ1963α=533;β+=473153Erm57674102798.
21.
0373ns9(27/2)061979IT=100153Ern55224105248.
11.
0248ns32(41/2)061979IT=100153Tm53989151.
48s0.
01(11/2)061964α=913;β+=93153Tmm539461543.
20.
22.
5s0.
2(1/2+)061988α=923;β+=153Yb47210#200#4.
2s0.
27/2#0688Wi05D1977β+=;α=50#;.
.
.
153Ybm44510#220#270010015s127/2061989IT=100153Lu38420160900ms20011/20697Ir01D1989β+;α=;p=0153Lum383401608051#s1/2+0697Ir01ED1997β+;α=;IT=;p=0153Lun359201602502.
50.
4>100ns23/2061993IT=100153Lup357901602632.
90.
515s327/2061993IT=100153Hf27300#500#400#ms(>200ns)1/2+#0600So11I2000β+153Hfm26550#510#750#100#500#ms11/2#β+;IT153NdmT:average10Si03=1.
17(0.
07)96Ya12=1.
06(0.
05)153ErJ:and89Ot.
A153YbD:.
.
.
;β+p=0.
0082153YbmE:inENSDF2578.
2+x153LuD:p=0%decayisfrom97Ir01154La41760#400#100#msβ;βn;β2n154Ce52350#300#300#ms(>150ns)0+0994Be24I1994β;βn154Pr581901502.
3s0.
1(3+)091988β=100;βn154Nd6568011025.
9s0.
20+091970β=100154Ndm643801101297.
90.
43.
2s0.
3(4)0909Si21ETJ1970IT=100154Pm6849040&1.
73m0.
10(0,1)091958β=100154Pmm68370110120120BD&2.
68m0.
07(3,4)091958β=100154Sm72454.
51.
8STABLE(>2.
3Ey)0+091933IS=22.
7529;2β154Eu71737.
21.
78.
601y0.
0103091947β≈100;ε=0.
01812154Eum71669.
01.
768.
17020.
00042.
2s0.
12+091964IT=100154Eun71591.
91.
7145.
30.
346.
3m0.
4(8)091975IT=100154Gd73705.
31.
6STABLE0+091938IS=2.
183154Tb701605021.
5h0.
40(+#)091950β+≈100;β150ns)5/2#0594Be24I1994β;βn155Pr55415171#s(>300ns)5/2#051992β;βn155Nd6228498.
9s0.
23/2#051986β=100155Pm66940541.
5s0.
2(5/2)051982β=100155Sm70190.
21.
822.
3m0.
23/2051951β=100155Smm70173.
71.
916.
50.
52.
8s0.
55/2+10Si03ETJ2010IT=100155Smn69651.
61.
9538.
60.
71.
00s0.
0811/210Si03ETJ2010IT=100155Eu71817.
21.
84.
753y0.
0145/2+051947β=100155Gd72069.
21.
6STABLE3/2051933IS=14.
8012155Gdm71948.
21.
6121.
050.
1931.
97ms0.
2711/2051967IT=100155Tb71249105.
32d0.
063/2+051957ε=100155Dy69155109.
9h0.
23/2051958β+=100155Dym6892110234.
330.
036s1(11/2)051970IT=100155Ho660391748m15/2+051959β+=100155Hom6589717141.
970.
11880s80(11/2)051984IT=100155Er6220965.
3m0.
3(7/2)051969β+≈100;α=0.
0227155Tm566261021.
6s0.
2(11/2)051971β+=99.
1124;α=0.
8924155Tmm565851241645s31/2+05FGK12aJ1990β+>92;α300ns)95Cz.
AI1992β;βn156Nd604702005.
06s0.
130+0307Sh05T1987β=100156Ndm590402001431.
30.
4365ns145(5)0309Si21ET1998IT=100156Pm64164426.
70s0.
104(+)0311So05J1986β=100156Pmm640144150.
30.
12.
3s2.
0(1+)07Sh05ETJ2007β1Ey)0+0358Ri23T1948IS=0.
0563;α;2β+156Ho654806056m14031957β+=100156Hom654306052.
40.
59.
5s1.
51031995IT=;β+156Hon653042817070MD7.
8m0.
3(9+)031975β+=75;IT156Er642102519.
5m1.
00+031967β+=100;α=17e–64156Tm568291583.
8s1.
82031971β+≈100;α=0.
06410156Tmm56430#200#400#200#400ns(11)031985IT=100156TmnnonexistentRN19s39+0391To08I156Yb532581026.
1s0.
70+031970β+=902;α=102156Lu4375070494ms12(2)031965α=;β+=5#156Lum43530#100#220#130#198ms2(9)+0396Pa01D1979α=946;β+156Hf3787016023ms10+0396Pa01D1979α=973;β+156Hfm359101601959.
01.
0AD480s408+0396Pa01T1979α=100156Ta26050#300#106ms4(2)0311Da12TD1992p=713;β+=293156Tam25960#300#948AD360ms40(9+)031993β+=95.
89;p=4.
29156NdT:others89Ok.
A=5.
51(0.
10)87Gr12=5.
47(0.
11),seediscussionin07Sh05156NdmE:least-squaresttoγ-rayenergiesin09Si21T:98Ga12=135ns(nounc.
)156SmmT:otherrecent09Si21=186(44)156TbmE:derivedfromE324hto4+49.
630levelandE(IT)300ns)5/2#0595Cz.
AI1992β157Pm62297710.
56s0.
10(5/2)051987β=100157Sm6667848.
03m0.
073/2#051973β=100157Eu69458415.
18h0.
035/2+051951β=100157Gd70822.
81.
6STABLE3/2051933IS=15.
652157Gdm70758.
91.
663.
9170.
005460ns405/2+051964IT=100157Gdn70396.
21.
6426.
600.
0518.
5s2.
311/2051961IT=100157Tb70762.
81.
671y73/2+051960ε=100157Dy6942458.
14h0.
043/2051953β+=100157Dym692625161.
990.
031.
3s0.
29/2+051974IT=100157Dyn692255199.
380.
0721.
6ms1.
611/2051970IT=100157Ho668312312.
6m0.
27/2051966β+=100157Er633892518.
65m0.
103/2071966β+=100157Erm6323425155.
40.
376ms69/2+051971IT=100157Tm58736263.
63m0.
091/2+051974β+=100157Yb534261138.
6s1.
07/2051970β+=99.
5;α=0.
5157Lu46457156.
8s1.
8(1/2+,3/2+)051977β+;α=157Lum464361520.
92.
0AD4.
79s0.
12(11/2)051972β+=;α=62157Hf38900#200#115ms17/20596Pa01T1965α=869;β+=149157Ta2964016010.
1ms0.
41/2+051979α=;p=3.
412;.
.
.
157Tam29620160225AD4.
3ms0.
111/2051996α=;β+=1#;p=0157Tan2805016015939AD1.
7ms0.
125/2#051996α=100157W19710#400#275ms40(7/2)10Bi03TJD2010β+=100;α=0157Wp19390#400#32030AD(9/2)10Bi03EJ2010IT157LuT:ENSDF'05averageofveryconicting91To09=5.
7(0.
5)91Le15,92Po14=9.
6(8)157TaD:.
.
.
;β+=1#158Pr44330#400#200#msβ;βn158Nd54060#300#700#ms(>300ns)0+0495Cz.
AI1992β158Pm59089134.
8s0.
5041987β=100158Sm6525055.
30m0.
030+041970β=100158Smm6397151279.
11.
8115ns18(5)041973IT=100158Eu672551045.
9m0.
2(1)041951β=100158Gd70688.
91.
6STABLE0+041933IS=24.
847158Tb69469.
91.
9180y113041957β+=83.
47;β=16.
67158Tbm69359.
62.
2110.
31.
210.
70s0.
170041957IT≈100;β81;β+93;IT300ns)7/2+#12Ku26I2012β;βn159Pm56554101.
5s0.
25/2#1205Ic02T1998β=100159Sm62208611.
37s0.
155/2121986β=100159Smm6093161276.
80.
5116ns8(11/2)1209Ur04ET2009IT=100159Eu66043418.
1m0.
15/2+121961β=100159Gd68560.
81.
618.
479h0.
0043/2121949β=100159Tb69531.
61.
8STABLE3/2+1212Vi.
1J1933IS=100.
159Dy69166.
32.
0144.
4d0.
23/2121951ε=100159Dym68813.
52.
0352.
770.
14122s311/2121965IT=100159Ho67329333.
05m0.
117/2121958β+=100159Hom671233205.
910.
058.
30s0.
081/2+121966IT=100159Er64560436m13/2121962β+=100159Erm643774182.
6020.
024337ns149/2+121971IT=100159Ern641314429.
050.
03590ns6011/2121971IT=100159Tm60570289.
13m0.
165/2+121971β+=100159Yb55839181.
67m0.
095/2()121975β+=100159Lu497104012.
1s1.
01/2+12FGK12aJ1980β+≈100;α=0.
1#159Lum49610#90#100#80#10#s11/2#β+;IT;α159Hf42853175.
20s0.
107/21296Pa01T1973β+=657;α=357159Ta34444201.
04s0.
091/2+1297Da07T1979β+;α=345159Tam3438119645AD560ms6011/2121994α=551;β+159W25490#300#8.
2ms0.
77/2#1296Pa01TD1981α=8216;β+159Re14740#510#40#s1/2+#2006p;α159Rem14600#500#140#50#21.
6s3.
311/21207Pa27T2006p=;α=7.
535159TbJ:3/2conrmedbyanoveltechniquein12Vi.
1(seetext)159LuJ:favoredαdecayfrom163Ta1/2+159TaT:average97Da07=0.
83(0.
18)96Pa01=1.
10(0.
10)159WD:derivedfromoriginalα=92(23)%159RemT:average07Pa27=23(6)06Jo10=21(4)160Nd47130#400#300#ms(>300ns)0+12Ku26I1985β;βn160Pm53000#300#2#s(>300ns)12Ku26I2012β;βn160Sm6023569.
6s0.
30+051986β=100160Smm5887461361.
30.
4120ns46(5)09Si21ETJ2009IT=100160Eu634801038s4(1)(#)051973β=100160Gd67940.
91.
7STABLE(>31Ey)0+0501Da22T1933IS=21.
8619;2β160Tb67835.
51.
872.
3d0.
23051943β=100160Dy69671.
41.
9STABLE0+051938IS=2.
32918160Ho663811525.
6m0.
35+051950β+=100160Hom663211559.
980.
035.
02h0.
052051955IT=733;β+=273160Hon6618422197163s(9+)05GAuE1988IT=100160Er660642428.
58h0.
090+051954ε=100160Tm60300309.
4m0.
31051970β+=100160Tmm6023040702074.
5s1.
5(5+)051983IT=855;β+=155160Tmn60200#60#100#50#200ns(8)051986IT=100160Yb58165164.
8m0.
20+051967β+=100160Lu502706036.
1s0.
32#051979β+=100;α300ns)5/2#12Ku26I2012β;βn161Sm5667274.
8s0.
47/2+#111998β=100161Eu617921026s35/2+#111986β=100161Gd65505.
02.
03.
646m0.
0035/21194It.
AT1949β=100161Tb67460.
81.
86.
89d0.
023/2+111949β=100161Dy68054.
51.
9STABLE5/2+111934IS=18.
88942161Dym67568.
91.
9485.
560.
16760ns17011/21112Sw01T2012IT=100161Ho67196.
52.
82.
48h0.
057/2111954ε=100161Hom66985.
42.
8211.
150.
036.
76s0.
071/2+111965IT=100161Er6520093.
21h0.
033/2111954β+=100161Erm648049396.
440.
047.
5s0.
711/2111969IT=100161Tm618992830.
2m0.
87/2+111959β+=100161Tmm61891287.
510.
245#m(1/2+)111981β+;IT161Tmn618212878.
200.
03110ns37/2111981IT=100161Yb57839154.
2m0.
23/2111974β+=100161Lu525622877s21/2+111973β+=100161Lum523882817447.
3ms0.
4(9/2)111973IT=100161Hf463152318.
2s0.
53/2#111973β+≈100;α300ns)12Ku26I2012β;βn162Sm54530#200#2.
4s0.
50+072005β=100162Eu586906010.
6s1.
0071987β=100162Gd6428048.
4m0.
20+071967β=100162Tb65670407.
60m0.
15(1)071965β=100162Dy68180.
21.
9STABLE0+071934IS=25.
47536162Dym65992.
11.
92188.
10.
38.
3s0.
38+11Sw02ETD2011IT=100162Ho66041415.
0m1.
01+071957β+=100162Hom659354105.
870.
0667.
0m0.
76071961IT=62;β+=38162Er66333.
21.
9STABLE(>140Ty)0+0756Po16T1938IS=0.
1395;α;2β+162Erm64307.
21.
92026.
010.
1388ns167()0712Sw01TJ1974IT=100162Tm614762621.
70m0.
191071963β+=100162Tmm61350501304024.
3s1.
75+07GAuE1974IT;β+=194162Yb598271518.
87m0.
190+071963β+=100162Lu52830801.
37m0.
021()071978β+=100162Lum52710#220#120#200#1.
5m4#071980β+≈100;IT162Lun52530#220#300#200#1.
9m071980β+≈100;IT162Hf49169939.
4s0.
90+071982β+≈100;α=0.
0081162Ta39780503.
57s0.
127+#071985β+≈100;α=0.
07410162W34000181.
36s0.
070+071973β+;α=45.
216162Re22500#200#107ms13(2)071979α=946;β+162Rem22330#200#1759AD77ms9(9+)071979α=915;β+162Os14500#500#2.
1ms0.
10+071989α=100162ErT:lowerlimitisforαdecay162TmmE:above66.
90levelandlessthan192keV,fromENSDF163Pm43250#500#200#ms(>300ns)5/2#12Ku26I2012β;βn163Sm50720#300#1#s(>300ns)1/2#12Ku26I2012β163Eu56640707.
7s0.
45/2+#1008Os02T2007β=100163Gd61314868s37/2+#101982β=100163Tb64595419.
5m0.
33/2+101966β=100163Dy66379.
91.
9STABLE5/2101934IS=24.
89642163Ho66377.
31.
94.
570ky0.
0257/2101957ε=100163Hom66079.
41.
9297.
880.
071.
09s0.
031/2+101957IT=100163Hon64267.
91.
92109.
40.
4800ns150(23/2+)12Sw01ETJ2012IT=100163Er65167575.
0m0.
45/2101953β+=100163Erm647225445.
50.
6580ns100(11/2)101974IT=100163Tm6272861.
810h0.
0051/2+101959β+=100163Tmm62641686.
920.
05380ns30(7/2)101975IT=100163Yb592991511.
05m0.
353/2101967β+=100163Lu54791283.
97m0.
131/2(+)101979β+=100163Hf492642540.
0s0.
63/2#101982β+=100;α300ns)0+12Ku26I2012β;βn164Eu53330#210#4.
2s0.
20808Os02T2007β=100164Gd59770#200#45s30+061988β=100164Tb620801003.
0m0.
1(5+)011968β=100164Dy65966.
71.
9STABLE0+011934IS=28.
26054164Ho64980.
82.
329m11+011938ε=605;β=405164Hom64841.
02.
3139.
770.
0836.
4m0.
360108Ha21T1966IT=100164Er65941.
61.
9STABLE0+011938IS=1.
6013;α;2β+164Erm62565.
52.
23376.
11.
1>170ns(12+)011980IT=100164Tm61904242.
0m0.
11+011960ε=611;e+=391164Tmm61894251065.
1m0.
1601GAuE1971IT≈80;β+≈20164Yb610181575.
8m1.
70+011960ε=100164Lu54642283.
14m0.
031()011977β+=100164Hf5181816111s80+011981β+=100164Ta432832814.
2s0.
3(3+)011982β+=100164W38228116.
3s0.
20+011973β+=96.
212;α=3.
812164Re2752070719ms161(2)0109Ha42TD1979α=;β+=42#164Rem27370#100#160#130#890ms130(9+)09Ha42TD2009β+;α=31164Os2047016021ms10+011981α=;β+=2#164Ir7540#310#1#ms2#06p;α;β+164Irm7260#300#280#110#94s27(9+)0602Ma61T2001p=;α;β+164HomT:other66Jo07=37.
5(+1.
5–0.
5)164TmmE:lessthan20keV,fromENSDF164LuJ:negativeparityproposedin98Ge13;odd-odd160Tm162Tm162Luhave1ground-state164TaD:waserroneouslyconsideredasαemitter,insteadof163Tain83Sc18164ReT:average09Ha42=848(+140–105)96Pa01=380(160)81Ho10=880(240)164RemT:symmetrizedfrom864(+150–110)164IrmT:average02Ma61=58(+46–18)01Ke05=110(+60–30)165Sm43810#400#200#ms(>300ns)5/2#12Ku26I2012β;βn165Eu50690#320#2.
7s0.
35/2+#0808Os02TD2007β=100;βn165Gd56490#300#10.
3s1.
61/2#061998β=100165Tb60570#200#2.
11m0.
103/2+#061983β=100165Dy63611.
31.
92.
334h0.
0017/2+061935β=100165Dym63503.
11.
9108.
15520.
00131.
257m0.
0061/2061963IT=97.
7611;β=2.
2411165Ho64898.
32.
0STABLE7/2061934IS=100.
165Hom64536.
62.
0361.
6750.
0111.
512s0.
0043/2+061958IT=100165Hon64183.
02.
0715.
330.
0260;β+80;IT300ns)5/2+#12Ku26I2012β;βn167Gd50810#400#3#s(>300ns)5/2#12Ku26I2012β167Tb55930#200#19s33/2+#0099As03T1999β=100167Dy59930606.
20m0.
08(1/2)001960β=100167Ho6228163.
1h0.
17/2001955β=100167Hom620226259.
340.
116.
0s1.
03/2+001977IT=100167Er63290.
72.
0STABLE7/2+001934IS=22.
8699167Erm63082.
92.
0207.
8010.
0052.
269s0.
0061/2001986IT=100167Tm62544.
12.
39.
25d0.
021/2+001948ε=100167Tmm62364.
62.
3179.
4800.
0191.
16s0.
06(7/2)+001964IT=100167Tmn62251.
32.
3292.
8200.
0200.
9s0.
17/2001965IT=100167Yb60591417.
5m0.
25/2001954β+=100167Ybm600194571.
5480.
022180ns(11/2)001976IT=100167Lu575003051.
5m1.
07/2+061958β+=100167Lum57500#40#0#30#>1m1/2(#)061998IT;β+167Hf53468282.
05m0.
05(5/2)001969β+=100167Ta48351281.
33m0.
07(3/2+)001982β+=100167W420991819.
9s0.
53/2#001985β+=99.
961;α=0.
041167Re34840#40#&3.
4s0.
4(9/2)0010An01J1992α≈100;β+167Rem3470040140#16#&5.
9s0.
31/2+0011Ko.
BEJ1984β+≈99;α≈1167Os2650070839ms57/20910Sc02TJD1977α=514;β+167Osm2606070435.
11.
0672ns7(13/2+)0910Sc02E2009IT=100167Ir170781929.
3ms0.
61/2+0205Sc22TD1981α=432;p=39.
313;β+167Irm1690219175.
52.
1p25.
7ms0.
811/20204Ke06T1995α=903;β+;.
.
.
167Pt6810#310#800s1607/2#0004Ke06T1996α=100167WJ:lowestobservedstatein92Th06is13/2+167OsD:average10Sc02=51(5)%96Pa01=49(7)%81Ho10=58(12)%167OsmE:also10Sc02=434.
3(1.
1),unc.
estimatedbyevaluator,basedonTableII167IrT:fromp-decay;α-decay05Sc22=30.
9(1.
3)97Da07=35.
2(2.
0)notused167IrmD:.
.
.
;p=0.
428D:pfrom05Sc22167IrmT:othernotused05Sc22=28.
7(3.
3)fromα-decayand28.
8(1.
3)fromp-decay167IrmT:97Da07=30.
0(0.
6)conicting,notused167PtT:average04Ke06=900(+300–200)96Bi07=700(200)No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1243TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)168Eu(>300ns)12Ku26I2012β;βn168Gd48360#400#300#ms(>300ns)0+12Ku26I1985β168Tb52720#300#8.
2s1.
34#101999β=100168Dy585601408.
7m0.
30+101982β=100168Ho60060302.
99m0.
073+101960β=100168Hom6000030591132s4(6+)1090Ch37E1990IT≈100;β4s(1)101990IT=100168Hop5987030192.
570.
20108ns111+101990IT=100168Er62990.
72.
0STABLE0+101934IS=26.
97818168Erm61896.
72.
01094.
03830.
0016109.
0ns0.
74101974IT=100168Tm61313.
32.
693.
1d0.
23+101949β+≈100;β=0.
0107168Yb61581.
42.
0STABLE(>130Ty)0+1056Po16T1938IS=0.
1233;α;2β+168Lu57070405.
5m0.
16()101960β+=100168Lum5687040202.
810.
126.
7m0.
43+101960β+>99.
64;IT300ns)7/2#12Ku26I2012β;βn169Tb50330#300#2#s(>300ns)3/2+#12Ku26I2012β;βn169Dy5560030039s8(5/2)081990β=100169Ho58798204.
72m0.
107/2081963β=100169Hom57412201386.
20.
4118s6(19/2+)10Dr05ETJ2010IT=100169Er60922.
62.
09.
392d0.
0181/2081956β=100169Erm60830.
62.
092.
050.
10285ns20(5/2)081969IT=100169Ern60678.
92.
0243.
690.
17200ns107/2+081969IT=100169Tm61275.
62.
1STABLE1/2+081934IS=100.
169Tmm60959.
52.
1316.
14630.
0001659.
9ns2.
37/2+081950IT=100169Yb60377.
12.
132.
018d0.
0057/2+081946ε=100169Ybm60352.
92.
124.
19990.
001646s21/2081949IT=100169Lu58084434.
06h0.
057/2+081955β+=100169Lum58055429.
00.
5160s10(1/2)081965IT=100169Hf54717283.
24m0.
04(5/2)081969β+=100169Ta50290284.
9m0.
4(5/2+)0898Zh03J1969β+=100169W449181574s65/2#081985β+=100169Re38409118.
1s0.
5(9/2)0892Me10D1978β+=;α=0.
0053169Rem382341417513AD15.
1s1.
5(1/2+,3/2+)08FGK129J1984β+;α≈0.
2;IT169Os30723253.
46s0.
11(5/2)0896Pa01T1972β+=86.
38;α=13.
78169Ir2207825353ms4(1/2+)081978α=4512;β+169Irm219181716022AD281ms4(11/2)081984α=727;β+;p169Pt12510#200#6.
99ms0.
09(7/2)0809Go16T1981α=;β+=1#169Au1790#300#150#s1/2+#p;α;β+169TmmE:ENSDF2008=316.
146330.
00011169ReD:α=0.
005(3)%derivedfromoriginalα=0.
001%-0.
01%169ReJ:favoredαdecayfrom(11/2)173Irto(11/2)levelat136.
2keV169RemJ:favoredαdecayfrom(1/2+,3/2+)173Irground-state169OsT:average96Pa01=3.
6(0.
2)95Hi02=3.
2(0.
3)84Sc06=3.
5(0.
2)82En03=3.
4(0.
2)169PtT:average09Go16=6.
99(0.
10)04Ke06=7.
0(0.
2)1244ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)170Gd(>300ns)0+12Ku26I2012β;βn170Tb46720#400#3#s(>300ns)12Ku26I2012β;βn170Dy53660#200#30#s0+1010So03I2010β170Ho56240502.
76m0.
056+#021960β=100170Hom561406010080BD43s2(1+)021960β=100170Er60109.
12.
4STABLE(>320Py)0+0296De60T1934IS=14.
91036;.
.
.
170Tm59796.
32.
1128.
6d0.
31021936β≈100;ε=0.
13110170Tmm59613.
12.
1183.
1970.
0044.
12s0.
13(3)+021967IT=100170Yb60764.
72.
1STABLE0+021938IS=2.
98239170Ybm59506.
22.
11258.
460.
14370ns154021981IT=100170Lu57307172.
012d0.
0200+021951β+=100170Lum572141792.
910.
09670ms100(4)021965IT=100170Hf562542816.
01h0.
130+061961ε=100170Ta50138286.
76m0.
06(3)(+#)021969β+=100170W47290132.
42m0.
040+021971β+≈100;α300ns)3/2+#12Ku26I2012β;βn171Dy50190#300#6#s(>300ns)7/2#12Ku26I2012β171Ho5452060053s27/2#021989β=100171Er57719.
42.
47.
516h0.
0025/2021938β=100171Erm57520.
82.
4198.
60.
1210ns101/2021969IT=100171Tm59211.
52.
21.
92y0.
011/2+021948β=100171Tmm58786.
52.
2424.
95600.
00152.
60s0.
027/2021948IT=100171Tmn57537.
02.
21674.
50.
31.
7s0.
219/2+09Wa06ETJ2009IT=100171Yb59308.
02.
0STABLE1/2021934IS=14.
0914171Ybm59212.
72.
095.
2820.
0025.
25ms0.
247/2+021968IT=100171Ybn59185.
62.
0122.
4160.
002265ns205/2021968IT=100171Lu57830.
02.
58.
24d0.
037/2+021951β+=100171Lum57758.
92.
571.
130.
0879s21/2021965IT=100171Hf554312912.
1h0.
47/2+0200Ye02J1951β+=100171Hfm554092921.
930.
0929.
5s0.
91/20200Ye02J1997IT≈100;β+171Ta517202823.
3m0.
3(5/2)021969β+=100171W47086282.
38m0.
04(5/2)021983β+=100171Re412502815.
2s0.
4(9/2)021987β+=100171Os34303188.
3s0.
2(5/2)021972β+;α=1.
8021171Ir26420403.
1s0.
31/2+0211Ko.
BTJ1967α≈100;β+171Irm26260#40#160#14#1.
47s0.
06(11/2)0211Ko.
BT1967α=545;β+;p171Pt174707045.
5ms2.
57/21010Sc02J1981α=907;β+171Ptm1706070412.
61.
0901ns913/2+10FGK128J2010IT=100171Au75682122.
3s2.
4(1/2+)0204Ke06T1997p≈100;α171Aum73131925510p1.
036ms0.
01611/20204Ke06TD1996α=60.
028;p=40.
028171Hg3290#310#70s303/2#042004α≈100;β+=0.
01#171IrT:other02Ro17=3.
2(+1.
3–0.
7)171IrmD:average10An01=53(5)%96Pa01=58(11)%171IrmT:average11Ko.
B=1.
50(0.
07)10An01=1.
40(0.
10)171PtmJ:M2to9/2171AuT:average04Ke06=22(+3–2)99Po09=17(+9–5)171AuT:other03Ba20=37(+7–5)conicting,notused171AumT:average04Ke06=1.
09(0.
03)03Ba20=1.
014(0.
019)171AumD:average04Ke06=34(4)%97Da07=46(4)%;BirgeratioB=2.
1171HgT:symmetrizedfrom59(+36–16)No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1245TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)172Tb(>300ns)12Ku26I2012β;βn172Dy48010#300#3#s(>300ns)0+12Ku26I2012β172Ho51480#200#25s3951991β=100172Er56484449.
3h0.
30+951956β=100172Erm5498341500.
90.
3579ns62(6+)10Dr02ETJ2006IT=100172Tm57375663.
6h0.
22951956β=100172Tmm568996476.
21.
0132s76+08Hu05ETJ2008IT=100172Yb59256.
22.
0STABLE0+951934IS=21.
6813172Ybm57705.
82.
01550.
430.
063.
6s0.
16951969IT=100172Lu56738.
12.
86.
70d0.
034951951β+=100172Lum56696.
22.
841.
860.
043.
7m0.
51951962IT=100;β+300ns)9/2+#12Ku26I2012β173Ho49350#300#10#s(>300ns)7/2#12Ku26I2012β173Er53650#200#1.
434m0.
017(7/2)9594It.
AT1972β=100173Tm5625458.
24h0.
08(1/2+)951961β=100173Tmm559365317.
730.
2010s3(7/2)951972IT=100173Yb57552.
22.
0STABLE5/2951934IS=16.
10363173Ybm57153.
32.
1398.
90.
52.
9s0.
11/2951963IT=100173Lu56882.
62.
21.
37y0.
017/2+951951ε=100173Lum56758.
92.
2123.
6720.
01374.
2s1.
05/2951962IT=100173Hf554122823.
6h0.
11/2061951β+=100173Hfm5530528107.
160.
05180ns85/2061973IT=100173Hfn5521528197.
470.
10160ns407/2+061973IT=100173Ta52397283.
14h0.
135/2951960β+=100173Tam5222428173.
100.
21225ns159/29595Ca27E1977IT=100173Tan50678281719.
41.
0132ns321/206Th07ETJ2006IT=100173W48727287.
6m0.
25/2951963β+=100173Re43554282.
0m0.
3(5/2)951986β+=100173Os374381522.
4s0.
9(5/2)9595Hi02TD1971β+≈100;α=0.
42173Ir30268119.
0s0.
8(1/2+,3/2+)9501Ko44J1967β+>93;α300ns)0+12Ku26I2012β;βn174Ho45690#300#8#s(>300ns)12Ku26I2012β174Er51950#300#3.
2m0.
20+991989β=100174Erm50840#300#1111.
61.
14.
02s0.
35809Dr06T2006IT=100174Tm53870405.
4m0.
1(4)991960β=100174Tmm5362040252.
40.
52.
29s0.
01(0+)06Ch10TJD2006IT>98.
5;β187ns991976IT=100174Wn48307281919.
70.
5187ns25991976IT=100174Wp47959282267.
80.
4158ns3806Ta13ETJ2006IT=100174Wq45711284515.
60.
4128ns812+06Ta13ETJ2006IT=100174Re43673282.
40m0.
043+#991972β+=100174Rem43570#60#100#50#1#m(>1s)7+#12Gu14T2012IT;β+174Os399951044s40+991971β+≈100;α=0.
0247174Ir30869287.
9s0.
6(3+)991967β+=99.
53;α=0.
53174Irm306762619311AD4.
9s0.
3(7+)991992β+=97.
53;α=2.
53174Pt2531810889ms170+991966α=768;β+174Au14240#90#139ms3low9902Ro17TD1983α=906;β+174Aum1399070250#50#171ms29high96Pa01TJ1995α=;β+174Hg6646192.
0ms0.
40+9999Se14T1997α≈100;β+=0.
4#174ErmE:uncertaintyestimatedbyNUBASE174TmmE:uncertaintyestimatedbyNUBASE174HfmJ:multipledecaybranches,transitionmult.
,magneticmoment;alsonandp174WpE:derivedfromleast-squaresttoγ-rayenergies174WqE:derivedfromleast-squaresttoγ-rayenergies174OsD:symmetrizedfrom71Bo06α=0.
020(+10–4)%174AuT:others96Pa01=171(29)83Sc24=120(20)174HgT:symmetrizedfrom1.
9(+0.
4–0.
3)175Ho43200#400#5#s(>300ns)7/2#12Ku26I2012β;βn175Er48650#400#1.
2m0.
39/2+#041996β=100175Tm523105015.
2m0.
51/2+#041961β=100175Yb54696.
62.
04.
185d0.
001(7/2)041945β=100175Ybm54181.
72.
0514.
8660.
00468.
2ms0.
31/2041972IT=100175Lu55167.
61.
9STABLE7/2+041934IS=97.
40113175Lum54814.
11.
9353.
480.
131.
49s0.
075/2041965IT=100175Lun53775.
42.
01392.
20.
6984s3019/2+0498Wh02J1998IT=100175Hf54483.
82.
770d25/2()041949ε=100175Hfm54357.
92.
7125.
890.
1253.
7s1.
51/2041964IT=100175Hfn53050.
42.
71433.
410.
121.
10s0.
0819/2+0495Gj01J1990IT=100175Hfp51468.
22.
73015.
60.
41.
21s0.
1535/20495Gj01J1980IT=100175Hfq49847.
63.
04636.
21.
21.
9s0.
145/2+0404Ko.
AJT1990IT=100175Ta524092810.
5h0.
27/2+041960β+=100175Tam5227828131.
410.
17222ns89/20496Ko17JT1972IT=100175Tan5207028339.
21.
3170ns20(1/2+)041969IT=100175Tap50841281567.
60.
31.
95s0.
1521/20496Ko17JT1996IT=100175W496332835.
2m0.
6(1/2)041963β+=100175Wm4939828234.
960.
15216ns6(7/2+)041978IT=100175Re45288285.
89m0.
055/2#041967β+=100175Os40105121.
4m0.
1(5/2)041972β+=100175Ir33394129s25/2#041967β+=99.
1528;α=0.
8528175Pt25700182.
53s0.
06(7/2)041966α=645;β+175Au1742040188ms121/2+0411Ko.
BTJD1975α=874;β+175Aum17250#40#167#12#AD134ms4(11/2)0411Ko.
BTD1975α=754;β+175Hg79707010.
6ms0.
4(7/2)091983α=;β+=1#175Hgm7480704942340ns30(13/2+)092009IT=100175AuJ:favoredαdecayto1/2+statesin171Irand167Reandfrom1/2+in179Tl175AuD:α=87(4)from11Ko.
B,aftercorrectionforα=64(5)of175Ptdaughter175AumT:average11Ko.
B=124(8)10An01=138(5);theformersupersedes01Ko44=143(8)175AumT:others02Ro17=158(3)96Pa01=185(30)83Sc24=200(22)formixtureground-stateandm175AumJ:favoredαdecayto(11/2)excitedisomer171Irm175AumD:α=75(4)%from11Ko.
B,aftercorrectionforα=64(5)%of175PtdaughterNo.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1247TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)176Ho(>300ns)12Ku26I2012β;βn176Er46630#400#20#s(>300ns)0+12Ku26I2012β176Tm493701001.
85m0.
03(4+)0694It.
AT1961β=100176Yb53489.
72.
2STABLE(>160Py)0+0696De60T1934IS=12.
99683;.
.
.
176Ybm52439.
92.
31049.
80.
611.
4s0.
38061967IT=;β300ns)1/2#12Ku26I2012β177Tm47470#300#90s6(7/2)031989β=100177Yb50984.
82.
31.
911h0.
003(9/2+)031945β=100177Ybm50653.
32.
3331.
50.
36.
41s0.
02(1/2)031962IT=100177Lu52385.
81.
96.
647d0.
0047/2+031945β=100177Lum52235.
41.
9150.
39670.
0010130ns39/2031949IT=100177Lun51816.
11.
9569.
70680.
0016155s71/2+031965IT=100177Lup51415.
61.
9970.
17500.
0024160.
44d0.
0623/2031962β=78.
68;IT=21.
48177Luq49614.
22.
02771.
60.
7625ns6233/2+04Dr06ETJ2004IT=100177Lur48855.
52.
03530.
30.
76s239/20311Ko.
AT2003IT=100177Hf52883.
01.
9STABLE7/2031934IS=18.
609177Hfm51567.
51.
91315.
45040.
00081.
09s0.
0523/2+031966IT=100177Hfn51540.
61.
91342.
380.
2055.
9s1.
2(19/2)031976IT=100177Hfp50143.
01.
92740.
020.
1551.
4m0.
537/2031971IT=100177Ta51717456.
56h0.
067/2+031948β+=100177Tam51644473.
360.
15410ns79/2031973IT=100177Tan515314186.
150.
063.
62s0.
105/2031971IT=100177Tap5036241355.
010.
195.
31s0.
2521/2031971IT=100177Taq4706144656.
30.
5133s449/2031994IT=100177W4970228132m21/2031950β+=100177Re462692814m15/2031957β+=100177Rem461842884.
710.
1050s105/2+031972IT=100177Os41949163.
0m0.
21/2031970β+=100177Ir360472030s25/2031967β+≈100;α=0.
061177Pt293701510.
6s0.
45/2031966β+=94.
35;α=5.
75177Ptm2922315147.
40.
42.
2s0.
31/2031979IT=100177Au21545101.
46s0.
03(1/2+,3/2+)0301Ko44TJ1968α=406;β+177Aum21356101898AD1.
180s0.
01211/20301Ko44ETJ1975α=6610;β+177Hg1278080127.
3ms1.
8(7/2)0305Ca43J1975α=85;β+=15177Hgm124608032311.
50s0.
15(13/2+)03Me20ETJ2003IT=100177Tl33252318ms5(1/2+)031999α=7313;p=2713177Tlm25181580718p180s60(11/2)0304Ke06TD1997p=518;α=498177LurE:derivedbyNUBASEfromleast-squaresttoγ-rayenergies177LurT:04Al04=7(2)m,nottrusted177HfpT:other04Al04=76(+16–9)fromdecaygrowth177AuT:average09An14=1.
53(0.
07)01Ko44=1.
46(0.
03)D:from09An14177AumD:from09An14177HgJ:also09An20177TlmT:04Ke06=160(+70–40)D:also04Ke06=55(20)%1248ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)178Er(>300ns)0+12Ku26I2012β;βn178Tm44120#400#30#s(>300ns)1109St16I2008β178Yb496941074m30+091973β=100178Lu50339.
82.
728.
4m0.
21(+)091957β=100178Lum502163123.
82.
6RQ23.
1m0.
39()0998Ge13J1951β=100178Hf52437.
71.
9STABLE0+091934IS=27.
287178Hfm51290.
31.
91147.
4160.
0064.
0s0.
28091960IT=100178Hfn49991.
61.
92446.
090.
0831y116+091968IT=100178Hfp49865.
31.
92572.
40.
368s214091977IT=100178Ta50600#50#2.
36h0.
087#091950β+=100178Tam5050115100#50#9.
31m0.
031+#0996Ko13E1950β+=100178Tan49130#50#1467.
820.
1659ms3150996Ko13ETJ1979IT=100178Tap47700#50#2901.
90.
7290ms12210996Ko13ETJ1996IT=100178W504091521.
6d0.
30+091950ε=100178Wm43836156572.
70.
3220ns1025+091998IT=100178Re456532813.
2m0.
2(3+)091957β+=100178Os43544145.
0m0.
40+091967β+=100178Ir362522012s2091972β+=100178Pt319971020.
7s0.
70+091966β+=92.
33;α=7.
73178Au22330602.
6s0.
5091968β+40178Aup219206040725AD178Hg1631611266.
5ms2.
40+091971α=;β+=30#178Tl4790#100#255ms10091997α=;β+=47#178Pb356924230s1500+0901Ro.
BT2001α≈100;β+178TamE:1+state(p9/2[514]+n7/2[514])isexpected104keVabovethe7ground-state,178TamE:basedonE=220keVfor8+(p9/2[514]+n7/2[514])andresidualenergy178TamE:shiftof50keVfromknownGallagher-Moszkowskisplittingenergy178TanE:fromleast-squaresttoγ-raysin96Ko13178TanT:average96Ko13=58(4)79Du02=60(5)178TapE:fromleast-squaresttoγ-raysin96Ko13178TlT:symmetrizedfrom02Ro17=254(+11–9)178PbT:twoeventsat202and147s,see84Sc13179Tm41600#500#20#s(>300ns)1/2+#12Ku26I2012β;βn179Yb46540#200#8.
0m0.
4(1/2)091982β=100179Lu4906154.
59h0.
067/2+091961β=100179Lum484695592.
40.
43.
1ms0.
91/2+091982IT=100179Hf50465.
41.
9STABLE9/2+091934IS=13.
622179Hfm50090.
41.
9375.
03520.
002518.
67s0.
041/2091962IT=100179Hfn49359.
71.
91105.
740.
1625.
05d0.
2525/2091970IT=100179Hfp46690.
22.
83775.
22.
115s5(43/2+)092000IT=100179Ta50359.
81.
91.
82y0.
037/2+091950ε=100179Tam50329.
11.
930.
70.
11.
42s0.
089/2091964IT=100179Tan49839.
61.
9520.
230.
18280ns801/2+09FGK128J1974IT=100179Tap49107.
21.
91252.
600.
23322ns1621/20997Ko13J1982IT=100179Taq49042.
61.
91317.
20.
49.
0ms0.
225/2+0997Ko13J1982IT=100179Tar49031.
81.
91328.
00.
41.
6s0.
423/20997Ko13J1982IT=100179Tax47720.
52.
02639.
30.
554.
1ms1.
737/2+0997Ko13J1982IT=100179W492971537.
05m0.
167/2091950β+=100179Wm4907515221.
910.
036.
40m0.
071/2091950IT≈100;β+=0.
294179Wn47665151631.
900.
08390ns3021/2+0994Wa05J1978IT=100179Wp45949153348.
410.
14750ns8035/20994Wa05J1978IT=100179Re465852519.
5m0.
15/2+091960β+=100179Rem465202565.
350.
0995s25(5/2)091972IT=100179Ren4476060182250408ns12(23/2+)091972IT=100179Rep41177255408.
00.
5466s15(47/2+,49/2+)091989IT=100179Os43019176.
5m0.
31/2091968β+=100179Osm4287417145.
410.
12500ns(7/2)091983IT=100179Osn4277617243.
00.
8783ns14(9/2)+091983IT=100179Ir380791079s1(5/2)091992β+=100179Pt32268821.
2s0.
41/2091966β+≈100;α=0.
243179Au24989127.
1s0.
3(1/2+,3/2+)091968β+=78.
09;α=22.
09179Aum249001289.
50.
5328ns2(3/2)11Ve01ETD2011IT=100179Hg16924271.
05s0.
037/20902Ko09J1970α=5525;β+=;β+p≈0.
15179Hgm1675327171.
40.
46.
4s0.
913/2+0902Je09J2002IT=100179Tl828040480ms201/2+09FGK128J1983α=;β+=30#179Tlm7460#40#825#10#1.
41ms0.
03(11/2)0911Ko.
BTJ1983α≈100;IT;β+179Pb2050803.
9ms1.
1(9/2)1010An01TDJ2010α=100179RenE:xkeVabove1772.
20(0.
22)level;xestimated50(50)byNUBASE179AumE:uncertaintyestimatedbyNUBASE179AupE:44(15)above89.
5keVlevel179TlT:average11Ko.
B=489(21)02Ro17=415(55)179TlJ:αdecayto1/2+in175Au179TlmJ:fromαdecayto175AumE:estimatedfromtrendsin177,181,183Tl179TlmT:average11Ko.
B=1.
36(0.
04)10An01=1.
46(0.
04)179PbT:symmetrizedfrom3.
5(+1.
4–0.
8)No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1249TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)180Tm(>300ns)12Ku26I2012β;βn180Yb44600#300#2.
4m0.
50+041987β=100180Lu46680705.
7m0.
15+041971β=100180Lum466707013.
90.
31s30495Me03JT1995β;IT180Lun4606070624.
00.
5>1ms(9)01Wh02EJT2001IT=100180Hf49781.
81.
9STABLE0+041934IS=35.
0816180Hfm48640.
31.
91141.
500.
055.
47h0.
048041951IT≈100;β=0.
31180Hfn48407.
71.
91374.
150.
04570s20(4)041990IT=100180Hfp47295.
52.
12486.
30.
9880ns9012+0411Ch.
AT2000IT=100180Hfq47243.
52.
22538.
31.
2>10s(14+)041999IT=100180Hfr46182.
52.
63599.
31.
890s10(18)041999IT=100180Ta48936.
22.
38.
154h0.
0061+041938ε=863;β=143180Tam48860.
91.
975.
31.
4RQSTABLE(>1.
2Py)9041940IS=0.
0120132;β180Tan47483.
82.
31452.
400.
1831.
2s1.
415041996IT=100180Tap45257.
22.
53679.
01.
12.
0s0.
5(22)042000IT=100180Taq44764.
02.
84172.
21.
617s5(24+)0400Wh04EJ2000IT=100180W49638.
61.
91.
8Ey0.
20+0404Co26TD1937IS=0.
121;α≈100;2β+180Wm48109.
61.
91529.
010.
035.
47ms0.
098041978IT=100180Wn46374.
01.
93264.
560.
212.
33s0.
1914041966IT=100180Re45837212.
44m0.
06(1)041955β+=100180Rem45750#40#90#30#>1s(4+,5+)0405El10J2005IT≈100;β+180Ren42280#40#3561#30#9.
0s0.
7(21)0405El10TJD2005IT=100180Os443621621.
5m0.
40+041967β+=100180Ir37978221.
5m0.
1(4,5)(+#)041972β+=100180Pt344361156s20+041966β+≈100;α≈0.
3180Au25594208.
1s0.
3041977β+1.
8180Hg20250132.
575s0.
0140+0400Ko48T1970β+=524;α=484180Tl9260601.
09s0.
014()0410An13TD1987β+=944;α=64;.
.
.
180Pb1930144.
2ms0.
50+111996α=100180HfnI:isomerat2425.
8(1.
0)15(5)s(10+)reportedthenretractedbyauthors180WT:alsoindicationin03Da05for1.
1(+0.
8–0.
4)Ey,butimportantbackground180WT:03Da09>80Pyfor2βdecay180RenE:3471.
0(0.
8)above(5+)level,mostlikelyisomer,estimatedtobe90#30keV180HgT:average00Ko48=2.
59(0.
02)93Wa03=2.
56(0.
02)180TlD:.
.
.
;β+SF=0.
00367J:from12Bi.
A;other11El07=(4,5)181Tm(>300ns)12Ku26I2012β;βn181Yb41090#300#1#m(>300ns)3/2#0609St16I2000β181Lu448001603.
5m0.
37/2+#061982β=100181Hf47405.
31.
942.
39d0.
061/2061935β=100181Hfm46810.
01.
9595.
270.
0480s59/2+0601Sh36T2001IT=100181Hfn46361.
82.
11043.
50.
8100s(17/2+)062001IT=100181Hfp45663.
42.
31741.
91.
31.
5ms0.
5(25/2)062001IT=100181Ta48441.
61.
8STABLE7/2+061932IS=99.
9879932181Tam48435.
41.
86.
2370.
0206.
05s0.
129/2061979IT=100181Tan47826.
41.
8615.
190.
0318s11/2+061948IT=100181Tap4701414142814140ns36(19/2+)061998IT=100181Taq46958.
21.
81483.
430.
2125.
2s1.
821/20698Wh02T1998IT=100181Tar46213.
72.
02227.
90.
9210s2029/20698Wh02J1998IT=100181W482535121.
2d0.
29/2+061947ε=100181Wm478875365.
550.
1314.
59s0.
155/2061968IT=100181Wn4660051653.
10.
6140ns2021/2+061973IT=100181Re465211319.
9h0.
75/2+061957β+=100181Rem4625813262.
910.
11156.
7ns1.
99/2061967IT=100181Ren44865131656.
370.
14250ns1021/2061974IT=100181Rep44640131880.
570.
1611.
5s0.
925/2+062000IT=100181Req42652133869.
400.
181.
2s0.
2(35/2)062000IT=100181Os4355025105m31/2061966β+=100181Osm435012549.
200.
142.
7m0.
17/2061966β+=100181Osn4339325156.
910.
15262ns69/2+061974IT=100181Ir39472264.
90m0.
155/2061972β+=100181Irm3918326289.
330.
13298ns5/2+061992IT=100181Irn3910626366.
300.
22126ns69/2061992IT=100181Pt343741552.
0s2.
21/20695Bi01D1966β+≈100;α=0.
07410181Ptm3425715116.
650.
08>300ns(7/2)061992IT=100181Au278712013.
7s1.
4(3/2)061968β+=;α=2.
75181Hg20661153.
6s0.
11/2(#)061969β+=732;α=272;.
.
.
181Hgm204505021050480s2013/2+0609An17T2009IT181Tl1279993.
2s0.
31/2+0909An14J1996β+;α300ns)0+12Ku26I2012β182Lu41880#200#2.
0m0.
21#101982β=100182Hf4605268.
9My0.
90+101961β=100182Hfm4487961172.
870.
1861.
5m1.
5(8)10FGK128J1971β=542;IT=462182Hfn4348072572.
22.
540s10(13+)101999IT=100182Ta46433.
21.
8114.
74d0.
123101938β=100182Tam46416.
91.
816.
2730.
004283ms35+101968IT182Tan45913.
61.
8519.
5770.
01615.
84m0.
1010101947IT=100182W48247.
70.
8STABLE(>7.
7Zy)0+101930IS=26.
5016;α182Wm46017.
00.
82230.
650.
141.
3s0.
1(10+)101969IT=100182Re4545010064.
0h0.
57+101950β+=100182Rem453882060100BD12.
7h0.
22+101950β+=100182Ren45150140300100585ns30(2)101969IT=100182Rep44930140520100780ns90(4)101984IT=100182Os446092221.
84h0.
200+101950ε=100182Osm42778221831.
40.
3780s70(8)101966IT=100182Osn37560227049.
50.
4150ns10(25+)101988IT=100182Ir390522115m13+101961β+=100182Irm389812171.
020.
17170ns40(5+)101990IT=100182Irn3887621176.
40.
3130ns50(6)101990IT=100182Pt36168132.
67m0.
120+101963β+≈100;α=0.
0382182Au283012015.
5s0.
4(2+)101970β+≈100;α=0.
135182Hg235771010.
83s0.
060+1097Ba21D1968β+=86.
29;α=13.
89;.
.
.
182Tl13310602.
2s0.
3(7+)1091Bo22TJ1991β+=97.
525;α300ns)12Ku26I2012β183Lu397209058s4(7/2+)911983β=100183Hf43290301.
018h0.
002(3/2)9106Vo12T1956β=100183Hfm418307014646440s3027/2#10Re07ETJ2010IT4.
1Zy)1/20104Co26T1930IS=14.
314;α183Wm46057.
70.
8309.
4930.
0035.
2s0.
311/2+011961IT=100183Re45811870.
0d1.
45/2+991950ε=100183Rem4390381907.
60.
31.
04ms0.
04(25/2+)991966IT=100183Os436605013.
0h0.
59/2+911950β+=100183Osm4349050170.
710.
059.
9h0.
31/291β+=852;IT=152183Ir402032458m55/29161Di04T1961β+≈100;α=0.
05#183Pt35772166.
5m1.
01/29395Bi01D1963β+≈100;α=0.
00965183Ptm357381634.
500.
0843s5(7/2)931979β+≈100;α150ns(9/2)+931990IT=100183Au30189942.
8s1.
05/29994Pa37J1968β+≈100;α=0.
5525183Aum30116973.
30.
4>1s(1/2)+991984IT=100183Aup299589230.
60.
68#s13/2+#81Mi12Iβ+183Tl1658796.
9s0.
71/2(+)0212Bi.
AJ1980β+=;α=2#183Tlm159599628.
70.
560ms15(9/2)0211Ve.
AEJD1980IT=;α=1.
53;β+183Tln156129975.
50.
61.
48s0.
10(13/2+)0201Mu26EJ2001IT=100183Pb757128535ms303/20309Se13J1980α=;β+=10#183Pbm747728948AD415ms2013/2+0309Se13J1980α≈100;β+183HfmT:forq=71+(H+likeion);symmetrizedfrom10(+48–5)183TamT:average09Sh17=101(20)67Mo13=107(11)183TanE:lessthan50keVabove1311level183WT:also03Da05>80Ey03Ce01>13Ey97Ge15>1.
9Ey183IrT:average61Di04=55(7)61La05=60(6)183HgD:.
.
.
;β+p=2.
6e–48183HgmI:lackofE(a)=6073-γcoinc.
in187Pbmdecay;noisomerseenin01Sc41183TlmE:uncertaintyestimatedbyNUBASED:αfrom06An11;ITfrom11Ve.
A183TlnE:346.
8(0.
3)keVabove183TlmNo.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1251TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)184Yb(>300ns)0+12Ku26I2012β184Lu36410#300#20s3(3+)1095Kr04TJ1989β=100184Hf41500404.
12h0.
050+101973β=100184Hfm40230401272.
20.
448s10(8)1012Re.
AD1995IT=;β=184Hfn390204024771016m715+#1010Re07ET2010β;IT184Ta42842268.
7h0.
1(5)101955β=100184W45707.
60.
9STABLE(>8.
9Zy)0+1004Co26T1930IS=30.
642;α184Wm44422.
60.
91284.
9970.
0088.
33s0.
185101969IT=100184Wn41844.
42.
73863.
22.
5188ns38(14,15,17)102004IT=100184Re44225435.
4d0.
73()101940β+=100184Rem440374188.
04630.
0017169d88(+)101964IT=74.
58;ε=25.
58184Os44256.
61.
3STABLE(>56Ty)0+101937IS=0.
021;α;2β+184Ir39611283.
09h0.
035101960β+=100184Irm3938528225.
650.
11470s303+101988IT=100184Irn3928328328.
400.
24350ns90(7)+101988IT=100184Pt373391517.
3m0.
20+1095Bi01D1963β+≈100;α=0.
00177184Ptm35499151840.
30.
81.
01ms0.
058101966IT=100184Au303192220.
6s0.
95+101969β+≈100;α20ns(10)1084Sc.
AT1984IT184Pb1105213490ms250+1004An07D1980α=8011;β+184Bi119080&6.
6ms1.
53+#102003α=184Bim1340#130#150#100#&13ms210#102002α=184HfmE:10Re07=1264(10)T:10Re07=113(+74–40)forq=72+(bareion)184HfnT:symmetrizedfrom10Re07=12(+10–4)forq=72+;also12Re.
A=12(+8–6)184OsT:lowerlimitisforαdecay184TlnT:α-decayfrom188BimnotcoincidentwithX(K)andγI:in02Sc.
A184TlnE:500.
7(6.
3)keVabove184Tlm,fromEadifference7462.
9(5)-6962.
2(3.
9)184PbD:average04An07=80(15)%03Va16=80(15)%185Yb(>300ns)12Ku26I2012β185Lu33890#300#6#s(>300ns)7/2+#09St16I2009β185Hf38320903.
5m0.
63/2#061993β=100185Ta413961449.
4m1.
57/2+#061950β=100185Tam40990144061900ns300(3/2+)0607Sh42ETJ2007IT=100185Tan40123141273.
40.
411.
8ms1.
421/20609La17EJT1999IT=100185W43389.
90.
975.
1d0.
33/2061940β=100185Wm43192.
50.
9197.
3830.
0231.
597m0.
00411/2+0694It.
AT1950IT=100185Re43822.
61.
2STABLE5/2+061931IS=37.
402185Rem41698.
81.
62123.
81.
1121ns13(21/2)061997IT=100185Os42809.
81.
392.
95d0.
091/20612Kr05T1947ε=100185Osm42707.
41.
3102.
370.
113.
0s0.
47/206FGK128J1970IT=100185Osn42534.
31.
3275.
530.
12780ns5011/2+061970IT=100185Ir403362814.
4h0.
15/2061958β+=100185Irm3814040219723120ns20061979IT=100185Pt366882670.
9m2.
4(9/2+)061960β+≈100;α=0.
005020185Ptm3658526103.
410.
0533.
0m0.
8(1/2)061970β+=;IT300ns)12Ku26I2012β186Hf36420502.
6m1.
20+031998β=100186Hfm3345070296843>20s17+#10Re07ET2010β;IT186Ta386106010.
5m0.
3(2,3)031955β=100186Tam3827060336201.
54m0.
059+#04Xu08T2010β;IT.
.
.
A-groupiscontinuedonnextpage.
.
.
1252ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%).
.
.
A-groupcontinued.
.
.
186W42510.
81.
5STABLE(>4.
1Ey)0+0303Da09T1930IS=28.
4319;2β;α186Wm40993.
61.
61517.
20.
618s1(7)031998IT=100186Wn38968.
02.
63542.
82.
18s4(16+)0398Wh02J1998IT=100186Re41930.
61.
23.
7183d0.
00111031939β=92.
5310;ε=7.
4710186Rem4178271497200ky(8+)0372Se06T1972IT=;β8.
2Zy,03Da05>170Ey,03Ce01>27Ey,186WT:and97Ge15>6.
5Ey186WnT:symmetrizedfrom12Re.
A=7.
5(+4.
8–3.
3)forq=72+186RemT:uncertainty50kyestimatedinENSDF'89evaluator,nottraceable186IrmT:average91Be25=1.
90(0.
05)70Fi.
A=2.
0(0.
1)186IrmE:Eispositiveandbelow1.
5keV186TlI:identiedasdecaylevelfrom190Biin91Va04186TlnE:374.
0(0.
2)keVabove186Tlm186BiT:average03An27=14.
8(0.
8)97Ba21=15.
0(1.
7)187Lu(>300ns)12Ku26I2012β187Hf32820#300#30#s(>300ns)3/2#0999Be63I1999β187Hfm32320#420#500#300#270ns809/2#09Al30TD2009IT=100187Ta36900702.
3m67/2+#0910Re07T1999β187Tam351107017891322s927/2#10Re07ET2010β;IT187Tan3397070293514>5m41/2+#10Re07ET2010β;IT187W39906.
31.
524.
000h0.
0043/2091940β=100187Wm39496.
21.
5410.
060.
041.
38s0.
07(11/2+)092008IT=100187Re41218.
51.
543.
3Gy0.
075/2+091931IS=62.
602;β=100;α1.
2e–4187Hgm28059195916MD&2.
4m0.
313/2+0970Ha18D1970β+=100;α>2.
5e–4187Tl22443851s(1/2+)091976β+300ns)12Ku26I2012β188Hf30880#300#20#s(>300ns)0+0299Be63I1999β188Ta336107019.
6s2.
00209Al30TD1999β=100188Tam3332070292.
40.
23.
6s0.
405Ca02ET2005IT=100188W38670369.
78d0.
050+021951β=100188Wm3674131929.
31.
6109.
5ns3.
5810La16ETJ2010IT=100188Re39018.
91.
517.
0040h0.
00221021939β=100188Rem38846.
81.
5172.
0690.
00918.
59m0.
04(6)021953IT=100188Os41139.
31.
5STABLE0+021931IS=13.
248188Ir383511041.
5h0.
51021950β+=100188Irm3738030970304.
2ms0.
211#02GAuE1971IT≈100;β+188Pt37829610.
2d0.
30+021954ε=100;α=2.
6e–53188Au32277158.
84m0.
061()021955β+=100188Hg30211113.
25m0.
150+021960β+=100;α=3.
7e–58188Hgm27487112724.
30.
4134ns15(12+)021983IT=100188Tl223363071s2(2)021970β+=100188Tlm2230893030MD71s1(7+)021970β+=100188Tln22030403103041ms4(9)021981IT≈100;β+188Pb178151125.
1s0.
10+0203Va16D1972β+=;α=9.
38188Pbm15237112578.
20.
71.
15s0.
03(8)0204Dr04T1999IT=100188Pbn15105112709.
70.
3136ns18(12+)0204Dr04ETJ2004IT=100188Pbp13032114783.
20.
3630ns80(19)0204Dr04ETJ2000IT=100188Bi718521&61.
2ms2.
73+#0206An04T1980α=;β+188Bim7120406630AD>5s7+#06An04ET1984IT188Bin70304015330AD&273ms8(10)0206An04T1984α=;β+188Po54420275s300+0203Va16T1999α=;β+188TamT:average11St21=3.
5(0.
4)09Al30=4.
4(1.
0);other05Ca02=5(2)188IrmE:lessthan100keVabove923.
5level,fromENSDF188HgmT:other04Gl04=270(51)188TlnE:268.
8(0.
2)keVabove188Tlm,from91Va04188PbD:also03Va16=8.
0(0.
6)%188BiT:average06An04=66(6)03An26=60(3);others97Wa05=46(7)84Sc.
A=44(3)188BinT:average06An04=280(20)03An26=265(15)188BinT:others97Wa05=218(50)84Sc.
A=210(90)189Hf27160#300#2#s(>300ns)3/2#1209Al30I2009β189Ta31830#300#3#s(>300ns)7/2+#0399Be63I1999β189Tam30230#500#1600#400#1.
6s0.
209Al30TD2009IT=100189W356204010.
7m0.
53/2#031963β=100189Re37981824.
3h0.
45/2+031963β=100189Os38988.
51.
6STABLE3/2031931IS=16.
155189Osm38957.
71.
630.
8120.
0155.
81h0.
069/2031960IT=100189Ir384571313.
2d0.
13/2+031955ε=100189Irm3808513372.
170.
0413.
3ms0.
311/2031960IT=100189Irn36124132333.
20.
53.
7ms0.
2(25/2)+031975IT=100189Pt364851110.
87h0.
123/2031955β+=100189Ptm3631211172.
800.
06464ns259/2031970IT=100189Ptn3629411191.
50.
7143s5(13/2+)031976IT=100189Au335822028.
7m0.
31/2+031955β+=100;α50;β+300ns)0+12Ku26I2012β190Ta28510#200#5.
3s0.
7(3)1009Al30TJD2009β=100190Tam28310#250#200#150#42ns71009Al30TD2009IT=100190W343804030.
0m1.
50+031976β=100190Wm32640401742.
02.
0111ns178+10La16ETJ2010IT=100190Wn32540401839.
02.
2166s6100310La16ETJ2000IT=100190Re35630703.
1m0.
3(2)031955β=100190Rem3543070204103.
2h0.
2(6)0312Re.
AE1962β=54.
420;IT190Os38709.
41.
6STABLE0+031931IS=26.
262190Osm37004.
01.
61705.
40.
29.
86m0.
03100312Kr05T1950IT=100190Ir36755.
62.
011.
78d0.
104031947β+=100;e+2s(4)+031996IT=100190Irp36379.
22.
0376.
40.
13.
087h0.
012(11)031950β+=91.
42;IT=8.
62190Pt373256650Gy300+031949IS=0.
0122;α=100;.
.
.
190Au328831642.
8m1.
01031959β+=100;α1s90391Va04ET1991IT190Pb204161371s10+031972β+;α=0.
404190Pbm17801132614.
80.
8150ns1410+0301Dr05J1998IT=100190Pbn177982426182024.
3s2.
1(12+)031998IT190Pbp17758132658.
20.
87.
7s0.
3110301Dr05JT1985IT=100190Bi10599236.
3s0.
1(3+)0391Va04J1972α=7721;β+=190Bim104703013040AD6.
2s0.
1(10)0391Va04J1988α=709;β+;β+p190Bin104782712115175ns8(5)09An11ET2009IT=100190Bip1020050404401.
3s0.
8(8)0309An11EJT2001IT=100190Po4564132.
46ms0.
050+031996α≈100;β+=0.
1#190WnT:others11St21=108(9)09Al30=106(18)s05Ca02=60(+1500–30)s00Po26300ns)1109St16I2009β191W311804020#s(>300ns)3/2#0799Be63I1999β191Wm309506023550340ns1411St21ETD2009IT=100191Re34352109.
8m0.
5(3/2+,1/2+)071963β=100191Rem32830500152050077s33high11St21ETJ2011IT=100191Os36396.
91.
614.
99d0.
029/20712Kr05T1940β=100191Osm36322.
51.
674.
3820.
00313.
10h0.
053/20712Kr05T1952IT=100191Ir36710.
81.
9STABLE3/2+071935IS=37.
32191Irm36539.
51.
9171.
290.
044.
899s0.
023(11/2)071955IT=100191Irn34609.
82.
12101.
00.
95.
7s0.
431/2(+)0712Dr02ETJ1979IT=100191Pt3570152.
83d0.
023/2071948ε=100191Ptm356005100.
6630.
020>1s(9/2)071976IT=100191Ptn355525149.
0350.
02295s5(13/2)+071967IT=100191Au33810403.
18h0.
083/2+071954β+=100191Aum3354040266.
20.
7920ms110(11/2)071971IT=100191Aun31320402489.
60.
9402ns20(31/2+)071985IT=100191Hg305932349m103/2()0786Ul02J1954β+=100;α300ns)0+99Be63I1999β192Re315908016.
0s0.
99812Al05T1965β=100192Rem3143080159188s811St21ETD2005IT=100192Ren31320802671070s3012Re.
AET2012β=;IT=192Os35883.
92.
7STABLE(>9.
8Ty)0+981931IS=40.
7819;2β;α192Osm33868.
52.
72015.
400.
115.
9s0.
11098FGK12aJ1965IT>87;β300ns)12Ku26I2012β193W26290#200#1#s(>300ns)1109St16I2009β193Re302404020#s(>300ns)5/2+#0699Be63I1999β193Rem3009040146.
00.
269s6(9/2)0611St21ETJ2005IT=100193Os33396.
02.
729.
830h0.
0183/20612Kr05T1940β=100193Osm33154.
02.
7242.
00.
5132ns2911St21ETD2011IT=100193Ir34538.
31.
9STABLE3/2+061935IS=62.
72193Irm34458.
11.
980.
2390.
00610.
53d0.
0411/2061957IT=100193Irn32260.
82.
12277.
51.
0124.
8s2.
131/2+12Dr02ETJ2012IT=100193Pt34481.
72.
050y61/2061948ε=100193Ptm34331.
92.
0149.
780.
044.
33d0.
0313/2+061949IT=100.
.
.
A-groupiscontinuedonnextpage.
.
.
1256ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%).
.
.
A-groupcontinued.
.
.
193Au33406917.
65h0.
153/2+061948β+=100;α10s0604Ni06ET2004IT=100193Biq13470#50#2400#50#3.
0s0.
1(29/2)062004IT=100193Po836030370ms40(3/2)061967α=;β+=5#193Pom8260#50#100#30#245ms22(13/2+)06GAuJ1981α=;β+=3#193At682229ms51/2+#062003α≈100193Atm592189AD21ms57/2#061995α≈100193Atn2621429AD28ms413/2+#062003α=2410;IT=7610193Rn9043251.
15ms0.
273/2#0706An36TD2006α≈100193RemE:aγof11St21=145.
2(0.
5)09Al30=146.
1(0.
2)keVisobservedindecay193RemT:average11St21=65(9)09Al30=72(8);also05Ca02=75(+450–40)s193OsT:other92An13=30.
11(0.
01);largesyst.
uncduetolargedead-timeeffect193OsI:alsoanisomerwithT=132(29)decayingviaa242keVγ-ray193TlmE:lessthan13keVabove365.
2level,fromENSDF193PbJ:fromαdecayfrom197Po193PbT:T=4.
0mreportedinKarlsruhecharts1981and1995.
Nottraceable193PbnE:2612.
5(0.
5)above193Pbm193BiD:α=3.
515isfromENSDF'98,wronglyattributedinENSDF'2006toNUBASE193BipE:ENSDF'062127.
9+x193BiqE:ENSDF'062357+x193PoT:symmetrizedfrom370(+46–40)J:αdecayto189Pb193AtT:symmetrizedfrom28(+5–4)193AtnT:symmetrizedfrom27(+4–3)194Ta(>300ns)12Ku26I2012β194W24530#300#1#s(>300ns)112008β194Re27240#200#1.
0s0.
5111999β=100194Rem26960#200#2854025s812Re.
AE2012β=100194Ren26410#200#83333100s1012Re.
AE2012β=100194Rep26140#200#1100#1000#45s1811St21TD2011IT=100194Req25240#200#2000#1000#38s37112005IT=194Os32437.
22.
86.
0y0.
20+061951β=100194Ir32533.
81.
919.
28h0.
131061937β=100194Irm32386.
71.
9147.
0720.
00231.
85ms0.
244+061959IT=100194Irn321607037070BD171d11(10,11)(#)061968β=100194Pt34762.
60.
9STABLE0+061935IS=32.
8640194Au32213.
22.
138.
02h0.
101061948β+=100194Aum32105.
82.
2107.
40.
5600ms8(5+)061975IT=100194Aun31737.
42.
2475.
80.
6420ms10(11)061953IT=100194Hg32183.
92.
9440y800+061962ε=100194Tl269371433.
0m0.
52061960β+=100;α300ns)12Ku26I2012β195Re25580#300#6s15/2+#112008β=100195Os29510609#m(>300ns)3/2#0709St16I2004β195Osm2906060454102h1.
713/2+#12Re.
AETD2012β=;IT=195Ir31694.
31.
92.
5h0.
2(3/2+)071952β=100195Irm31594510053.
8h0.
2(11/2)071968β=955;IT=55195Irn293406235464.
4s0.
6(27/2+)11St21ETJ2011IT=100195Pt32796.
30.
9STABLE1/2071935IS=33.
7824195Ptm32537.
00.
9259.
300.
084.
010d0.
00513/2+071960IT=100195Au32569.
51.
4186.
10d0.
053/2+071948ε=100195Aum32250.
91.
4318.
580.
0430.
5s0.
211/2071952IT=100195Hg310002310.
53h0.
031/2071952β+=100195Hgm3082423176.
070.
0441.
6h0.
813/2+071951IT=54.
220;β+=45.
820195Tl28155111.
16h0.
051/2+071955β+=100195Tlm2767211482.
630.
173.
6s0.
49/2071957IT=100195Pb237132315m3/2#071957β+;α195Pbm2351023202.
90.
715.
0m1.
213/2(+)0791Gr12E1957IT=100195Pbn21954231759.
00.
710.
0s0.
7(21/2)071976IT=100195Bi180265183s4(9/2)07GAuJ1971β+≈100;α=0.
032195Bim1762683996AD87s1(1/2+)07GAuJ1974β+=6717;α=3317195Bin1567050236050750ns5029/2#072003IT195Po11060404.
64s0.
09(3/2)0705Uu02J1967α=944;β+=64195Pom109652810050AD1.
92s0.
02(13/2+)0705Uu02J1967α≈90;β+≈10;IT300ns)0+12Ku26I2012β196Re22540#300#2.
4s1511Be.
AT2008β196Rem22420#300#120#40#3.
6s0.
611St21T2009IT=100196Os282804034.
9m0.
20+071977β=100196Ir294404052s1(0)071966β=100196Irm292292021040BD1.
40h0.
02(10,11)071959β≈100;IT2.
5Ey)0+0790Bu28T1930IS=0.
151;2β+196Tl27497121.
84h0.
032071955β+=100196Tlm2710312394.
20.
51.
41h0.
02(7+)071960β+=96.
24;IT=3.
84196Pb253611437m30+071957β+=100;α72keV(K-shellbindingenergy)196BinD:.
.
.
;α=0.
0003810196PoT:average05Uu02=5.
1(+3.
1–1.
4)97Pu01=5.
5(0.
1)93Wa04=5.
8(0.
2)196PoT:othernotused:10He25=4.
1(+5.
6–1.
5)ms196AtJ:sameas192Bi,fromα-decay196AtmI:levelnotacceptedinENSDF196RnT:symmetrizedfrom4.
4(+1.
3–0.
9)1258ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)197W(>300ns)12Ku26I2012β197Re20500#300#300#ms(>300ns)5/2+#09St16I2009β197Os25310#200#2.
8m0.
65/2#092003β=100197Ir28266205.
8m0.
5(3/2+)051952β=100197Irm281512111558.
9m0.
3(11/2)051976β≈100;IT=0.
2510197Irn27870#200#400#200#30s805Ca02T2005IT=100197Pt30422.
00.
919.
8915h0.
00191/2051936β=100197Ptm30022.
40.
9399.
590.
2095.
41m0.
1813/2+051941IT=96.
74;β=3.
34197Au31141.
00.
7STABLE3/2+051935IS=100.
197Aum30731.
90.
7409.
150.
087.
73s0.
0611/2051945IT=100197Aun28608.
51.
22532.
51.
0150ns527/2+#06Wh02ETJ2006IT=100197Hg30541364.
94h0.
071/20501Li17T1941ε=100197Hgm302423298.
930.
0823.
8h0.
113/2+051943IT=91.
47;ε=8.
67197Tl28340162.
84h0.
041/2+051955β+=100197Tlm2773216608.
220.
08540ms109/20512Bi.
AJ1953IT=100197Pb2474968.
1m1.
73/2051955β+=100197Pbm244296319.
310.
1142.
9m0.
913/2+051957β+=812;IT=192197Pbn2283561914.
100.
251.
15s0.
2021/2051978IT=100197Bi1968789.
33m0.
50(9/2)051971β+=100;α=1e–4#197Bim19155853212AD5.
04m0.
16(1/2+)051966α=5540;β+=4540;.
.
.
197Bin1728414240312263ns13(29/2)0586Ch01TJD1986IT=100197Bip1675882929.
50.
5209ns30(31/2)0586Ch01TJD1986IT=100197Po133605053.
6s0.
9(3/2)0593Wa04T1965β+;α=447197Pom13130#90#230#80#25.
8s0.
1(13/2+)0593Wa04T1967α=849;β+;IT=0.
01#197At634050388.
2ms5.
6(9/2)0505De01T1967α=96.
112;β+=3.
912197Atm6293135050AD2.
0s0.
2(1/2+)051985α≈100;β+;IT300ns)09St16I2009β;βn198Os23840#200#1#m(>300ns)0+1009Po02I2008β198Ir25820#200#8s1091973β=100198Pt29905.
72.
2STABLE(>320Ty)0+0952Fr23T1935IS=7.
3613;2β;α198Au29582.
00.
72.
6948d0.
001220911Ch22T41937-=100198Aum29269.
80.
7312.
22000.
0020124ns45+091968IT=100198Aun28770.
31.
7811.
71.
52.
272d0.
0161209FGK128J1972IT=100198Hg30954.
80.
5STABLE0+101925IS=9.
9720198Tl27490805.
3h0.
52091949β+=100198Tlm2695080543.
60.
41.
87h0.
037+091949β+=55.
923;IT=44.
123198Tln2680080687.
20.
5150ns40(5+)091977IT=100198Tlp2675080742.
40.
432.
1ms1.
01009FGK128J1975IT=100198Pb26050152.
4h0.
10+091955β+=100198Pbm23909152141.
40.
44.
19s0.
10709FGK128J1972IT=100198Pbn23819152231.
40.
5137ns10909FGK128J1989IT=100198Pbp23230152820.
50.
7212ns412+09FGK128J1973IT=100.
.
.
A-groupiscontinuedonnextpage.
.
.
No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1259TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%).
.
.
A-groupcontinued.
.
.
198Bi193692810.
3m0.
3(2+,3+)091950β+=100198Bim190852828040MD11.
6m0.
3(7+)091992β+=100198Bin188372853040MD7.
7s0.
5(10)09FGK128J1972IT=100198Po15473171.
77m0.
030+091965α=572;β+=432198Pom12907172565.
920.
20200ns2011091990IT=100198Pon1273050274050750ns5012+091990IT198At6720#50#4.
21s0.
22(3+)0995Bi.
AD1967α>94;β+198Atm64298290#50#AD1.
09s0.
11(10)0995Bi.
AD1967α>86;β+198Rn12301365ms30+091984α=;β+=1#198RnmnonexistentEU50ms9α=;β+=;IT=198ReI:other12Ku26>300ns198IrT:other11Be.
A=8(2)198PtT:lowerlimitisfor0ν-ββdecay198AuT:severalconictingvalues,evaluatedin11Ch22198AunJ:M4to8+;magneticmoment198TlpJ:E3to7+198PbmJ:E2to5;magneticmoment198PbnJ:E2to7198PbpJ:E2to10+;magneticmoment198BinE:248.
5(0.
5)keVabove198Bim,from92Hu04J:E3to(7+)198AtT:average05Uu02=3.
8(0.
4)92Hu04=4.
2(0.
3)67Tr06=4.
9(0.
5)198AtT:otherrecennotused12Fo09=4.
2(2.
0)198AtmT:average05Uu02=1.
04(0.
15)92Hu04=1.
0(0.
2)67Tr06=1.
5(0.
3)198RnmI:αdecayassignedtoisomerinENSDF'95,notacceptedbyNUBASE199Re(>300ns)12Ku26I2012β199Os20480#200#6s35/2#0711Be.
AT2008β=100199Ir24400407s53/2+#0711Be.
AT1993β199Irm24270#60#130#40#235ns9011/2#072005IT=100199Pt27390.
42.
230.
80m0.
215/2071937β=100199Ptm26966.
43.
0424213.
6s0.
4(13/2)+071959IT=100199Au29095.
00.
73.
139d0.
0073/2+071937β=100199Aum28546.
10.
7548.
94050.
0021440s30(11/2)071968IT=100199Hg29546.
40.
4STABLE1/2071925IS=16.
8722199Hgm29013.
90.
4532.
480.
1042.
67m0.
0913/2+071948IT=100199Tl28059287.
42h0.
081/2+071949β+=100199Tlm2731028748.
870.
0628.
4ms0.
29/2071963IT=100199Pb252321090m103/2071950β+=100199Pbm2480310429.
52.
712.
2m0.
3(13/2+)071955IT=93;β+=7199Pbn22668102563.
82.
710.
1s0.
2(29/2)071981IT=100199Bi207971127m19/2071950β+=100199Bim2013111667324.
70m0.
15(1/2+)071950β+=;IT300ns)1/2#09St16I2009β201Ir19900#200#21s53/2+#1111Be.
AT2008β=100201Pt23740502.
5m0.
1(5/2)071962β=100201Au26401326.
0m0.
83/2+071952β=100201Aum2580765945730s630(11/2)0711St21ETJ1981IT=100201Aun247916161055.
6s2.
411St21ETD2011IT=100201Hg27662.
70.
6STABLE3/2071925IS=13.
189201Hgm26896.
50.
6766.
220.
1594.
0s2.
013/2+071961IT=100201Tl27179143.
0421d0.
00171/2+071950ε=100201Tlm2626014919.
160.
212.
01ms0.
07(9/2)071962IT=100201Pb25259229.
33h0.
035/2071950β+=100201Pbm2463022629.
10.
360.
8s1.
813/2+071952IT≈100;β+201Pbn2232130293820508ns3(29/2)071981IT=100201Bi2141515103m39/2071950β+=100201Bim2056915846.
350.
1857.
5m2.
11/2+071950β+>91.
1#;IT300ns)0+09St16I2009β202Ir16780#300#13s21#0811Be.
AT2008β=100202Irm14780#300#2000#1000#3.
4s0.
611St21TD2011IT=100202Pt226922544h150+081992β=100202Ptm20904251788.
50.
4141s7(7)0811St21T2005IT≈100202Au243532328.
4s1.
2(1)081967β=100202Hg27345.
50.
6STABLE0+081920IS=29.
8626202Tl259861412.
31d0.
082081940ε=100202Tlm2503614950.
190.
10591s37+081958IT=100202Pb25940452.
5ky2.
80+081954ε=100202Pbm2377042169.
850.
083.
54h0.
029081954IT=90.
55;β+=9.
55202Pbn2180050414050110ns516+#081986IT=100202Pbp2064050530050107ns319#081987IT=100202Bi20741151.
72h0.
055(+#)081951β+=100;α300ns202IrT:average11Be.
A=11(3)usingβ-tand15(3)usingγ-t202IrmD:311.
5,655.
9,737.
2,889.
2,967.
6γraysseenindecay202HgD:lowerhalf-lifelimitfor24NedecayT>3.
7Zy,from90Bu28202PbnE:4091.
0(0.
7)+x;xestimated50(50)202PbpE:5251.
0(0.
5)+u;uestimated50(50)202BiJ:re-evaluationtoapossible6+isdiscussedin96Ca02202BimE:605+xwithx300ns)12Ku26I2012β203Ir14690#400#1#s(>300ns)3/2+#09St16I2009β203Irm12550#400#2140#50#798ns350(23/2+)11St21TJD2011IT=100203Pt19630#200#22s41/2#0611Be.
AT2008β=100#203Ptm16530#200#3100#1000#641ns5533/2+#11St21TJD2011IT=100203Au23143360s63/2+051952β=100203Aum2250246413140s4411/2#0511St21TJ2005IT=100203Hg25268.
81.
746.
594d0.
0125/2051943β=100203Hgm24335.
71.
7933.
140.
2321.
9s1.
0(13/2+)0511St21T1964IT=100203Hgn16987.
81.
88281.
00.
5146ns30(53/2+)11Sz01EJT2011IT=100203Tl25760.
81.
3STABLE1/2+051931IS=29.
521203Tlm22200503565507.
7s0.
5(25/2+)051998IT=100203Pb24786751.
92h0.
035/2051942ε=100203Pbm239617825.
20.
36.
21s0.
1113/2+051955IT=100203Pbn2183772949.
20.
4480ms729/2051977IT=100203Pbp2182050297050122ns425/2#051988IT=100203Bi215241311.
76h0.
059/2051950β+=100203Bim20426131098.
120.
12305ms51/2+051984IT=100203Bin19483132041.
50.
6194ns3025/2+051978IT=100203Po17311936.
7m0.
55/2051951β+≈100;α=0.
112203Pom166699641.
680.
1745s213/2+051969IT≈100;α=0.
04#203Pon1515392158.
50.
6>200ns051986IT=100203At12163117.
4m0.
29/2051951β+=693;α=313203Rn61592444s23/2#051967α=669;β+203Rnm5799233604AD26.
9s0.
513/2(+)0587Bo29J1967α=7510;β+203Fr8766550ms109/2#051967α≈100;β+=5#203Ra86708036ms13(3/2)0596Le09J1996α≈100;β+203Ram88553019090AD25ms5(13/2+)0596Le09J1996α≈100;β+203IrmE:207.
0,841.
3,894.
7γsincascadeto11/2estimatedat200(50)keV203PtT:05Ku.
A=10(3)sameauthor203TlmE:3514.
6+xandxestimated50(50)keV203PbpE:2923.
4(0.
7)+x;xestimated50(50)203RnJ:notyetknown,willbesameas195Pband199Po,fromα-decay203RaT:symmetrizedfrom31(+17–9)203RamT:symmetrizedfrom24(+6–4)1262ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)204Ir9690#400#200#msβ;βn204Pt17920#200#10.
3s1.
40+102008β=100204Ptm15930#200#1995.
10.
75.
5s0.
7(5)1011St21E2009IT=100204Ptn15890#200#20352355s3(7)102009IT204Ptp14730#200#319323146ns14(10+)102009IT=100204Au20650#200#38.
2s1.
4(2)1011Be.
AT1972β=100204Aum16830#200#3816#1000#2.
1s0.
316+#1011St21JD2008IT=100204Hg24690.
20.
5STABLE0+101920IS=6.
8715;2β204Tl24345.
61.
23.
783y0.
0122101953β=97.
087;ε+β+=2.
927204Tlm23241.
51.
21104.
10.
261.
7s1.
07+1011Br12EJ1972IT=100204Tln22026.
61.
22319.
00.
32.
6s0.
2121011Br12EJ1998IT=100204Tlp19954.
01.
34391.
60.
5420ns3018+1011Br12ETJ1998IT=100204Tlq18106.
21.
36239.
40.
590ns3221011Br12ETJ2011IT=100204Pb25109.
41.
2STABLE(>140Py)0+101932IS=1.
41;α204Pbm23835.
31.
21274.
130.
05265ns64+101963IT=100204Pbn22923.
51.
22185.
880.
0866.
93m0.
109101956IT=100204Pbp22845.
01.
22264.
420.
06490ns707101978IT=100204Bi20646911.
22h0.
106+101947β+=100204Bim198419805.
50.
313.
0ms0.
110101974IT=100204Bin1781392833.
41.
11.
07ms0.
0317+101974IT=100204Po18341113.
519h0.
0120+101951β+=99.
333;α=0.
673204Pom16702111639.
030.
06158.
6ns1.
88+1010Ka29T1970IT=100204At11875229.
12m0.
117+101961β+=96.
22;α=3.
82204Atm1128822587.
300.
20108ms1010101969IT=100204Rn7983151.
242m0.
0230+101967α=72.
49;β+204Fr607251.
75s0.
26(3+)1095Bi.
AD1964α=962;β+204Frm65825514AD2.
30s0.
24(7+)1095Bi.
AD1967α=902;β+204Frn935253274AD0.
8s0.
2(10)101992α=748;IT=268204Ra60471460ms90+1005Uu02T1995α≈100;β+=0.
3#204PtT:other11Be.
A=16(+6–5)204PtmE:872.
4(0.
5),1122.
7(0.
5)γsto0+204PtnE:1995.
1(0.
7)+X;x300ns)12Ku26I2012β;βn205Pt12970#300#1#s(>300ns)9/2+#1110Al24I2009β205Au18770#200#32.
5s1.
43/2+#0409Po01T1994β=100205Aum17860#200#90756s211/2#09Po01ETJ2009IT=;β=205Aun15920#200#28505163ns519/2+#11St21ET2011IT=100205Hg2228745.
14m0.
091/2041940β=100205Hgm2073141556.
400.
171.
09ms0.
0413/2+041985IT=100205Hgn1897143315.
80.
95.
89s0.
18(23/2)11St21ETJ2011IT=100205Tl23820.
31.
3STABLE1/2+041931IS=70.
481205Tlm20529.
71.
33290.
600.
172.
6s0.
225/2+041976IT=100205Tln18984.
72.
04835.
61.
5235ns10(35/2)042004IT=100205Pb23769.
71.
217.
3My0.
75/2041954ε=100205Pbm23767.
41.
22.
3290.
00724.
2s0.
41/2041994IT=100205Pbn22755.
91.
21013.
850.
035.
55ms0.
0213/2+041960IT=100205Pbp20574.
01.
33195.
70.
5217ns525/2041973IT=100205Bi21064515.
31d0.
049/2041951β+=100205Bim1956751497.
170.
097.
9s0.
71/2+041972IT=100205Bin1892552139.
00.
7220ns2525/2+041978IT=100205Po17509201.
74h0.
085/2041951β+≈100;α=0.
041205Pom1736620143.
1660.
017310ns601/2041960IT=100205Pon1662920880.
310.
07645s2013/2+041962IT=100205Pop16048201461.
210.
2157.
4ms0.
919/2041973IT=100205Poq14422203087.
20.
4115ns1029/2041985IT=100205At129701533.
8m0.
29/20410Ka29T1951β+;α=102205Atm10630152339.
650.
237.
76s0.
1429/2+041982IT=100205Rn7710502.
83m0.
075/2041967β+;α=24.
69205Rnm705050657.
10.
5>10s13/2+#0410De04ED2010IT≈100;α;β+205Fr131083.
82s0.
06(9/2)0410De04T1964α≈100;β+300ns)0+12Ku26I2012β;βn206Au14220#300#30#s(>300ns)1109St16I2009β206Hg20945208.
32m0.
070+081961β=100206Hgm18843202102.
40.
32.
09s0.
0250811St21T1982IT=100206Hgn17223203722.
31.
0106ns6(10+)0811St21ETJ2001IT=100206Tl22252.
81.
44.
202m0.
0110081935β=100206Tlm19609.
71.
42643.
100.
183.
74m0.
03(12)081976IT=100206Pb23785.
11.
2STABLE0+081927IS=24.
11206Pbm21584.
91.
22200.
160.
04125s27081953IT=100206Pbn19757.
81.
44027.
30.
7202ns312+081971IT=100206Bi2002886.
243d0.
0036(+)081947β+=100206Bim19968859.
8970.
0177.
7s0.
2(4+)081957IT=100206Bin1898381044.
80.
7890s10(10)081974IT=100206Po1818848.
8d0.
10+081947β+=94.
555;α=5.
455206Pom1660241585.
900.
11232ns48+#081970IT=100206Pon1592642262.
090.
121.
05s0.
069#081970IT=100206At124291530.
6m0.
8(5)+081961β+=99.
108;α=0.
908206Atm11619158103813ns21(10)0809Dr08T1999IT=100206Rn9115155.
67m0.
170+081954α=623;β+=383206Fr12422816s(2+,3+)0892Hu04D1964β+=;α=4224206Frm1048281904016s(7+)0892Hu04D1964α=4224;β+;IT206Frn5172873040MD700ms100(10)081983IT=;α≈5#206Frx1140100100100MDR=spmix206Ra356618240ms200+081967α=;β+=2.
5#206Ac13460#70#25ms7(3+)081998α≈100;β+=0.
2#206Acm1371030250#80#AD41ms16(10)081996α≈100;β+206HgmT:average11St21(=09Si35)=2.
09(0.
02)82Be38=2.
15(0.
21)206HgnT:average11St21(=09Si35)=112(4)09Al29=96(15)01Fo08=92(8)01La09=90(10)206PomE:lessthan40keVabove1573.
4level,fromENSDF206AtmT:others10Ka29=377(44)99Fe10=410(80)206AtmE:fromENSDF'08806.
7(1.
4)+x;x300ns)12Ku26I2012β;βn207Au10810#300#10#s(>300ns)3/2+#112010β;βn207Hg16487302.
9m0.
29/2+#111982β=100207Tl2103354.
77m0.
021/2+111908β=100207Tlm1968551348.
180.
161.
33s0.
1111/2111965IT≈100;β300ns)0+12Ku26I2012β;βn208Au6100#300#10#s(>300ns)1110Al24I2010β;βn208Hg132703042m50+101994β=100208Tl16749.
22.
03.
053m0.
0045+071909β=100208Pb21748.
11.
2STABLE0+071927IS=52.
41208Pbm16852.
91.
24895.
230.
05500ns1010+0798Pf02T1998IT=100208Bi18869.
72.
4368ky45+071953β+=100208Bim17298.
62.
41571.
10.
42.
58ms0.
0410071961IT=100208Po17469.
21.
82.
898y0.
0020+071947α≈100;β+=0.
00404208Pom15941.
01.
81528.
220.
04350ns208+071968IT=100208At1247091.
63h0.
036+071950β+=99.
456;α=0.
556208Atm1019492276.
41.
81.
5s0.
216071991IT=100208Rn96551124.
35m0.
140+071955α=627;β+=387208Rnm7827111828.
30.
4487ns128+071979IT=100208Fr26661159.
1s0.
37+071964α=893;β+=113208Frm18392182718432ns11(10)0709Dr08T2009IT=100208Ra1715151.
110s0.
0450+0710He25TD1967α=873;β+208Ram3862152147.
40.
4263ns17(8+)0705Re02T1998IT=100208Ac107606097ms16(3+)0796Ik01T1994α=;β+=1#208Acm112582850050AD28ms7(10)0796Ik01T1994α=;IT300ns)3/2+#1110Al24I2010β;βn209Hg8640#150#37s89/2+#081998β=100;βn209Tl1363882.
161m0.
007(1/2+)9194Ar23T1950β=100;βn209Pb17614.
11.
83.
253h0.
0149/2+911940β=100209Bi18258.
21.
419.
9Ey0.
79/29112Be06T1924IS=100.
;α=100209Po16365.
61.
8102y51/2911949α≈100;β+=0.
484209Pom12100.
01.
84265.
60.
1119ns4(31/2)911974IT=100209At1288255.
41h0.
059/2911951β+=95.
95;α=4.
15209Atm1045352429.
250.
23890ns40(29/2)+911975IT=100209Rn89292028.
5m1.
05/2911952β+=832;α=172209Rnm7755201173.
980.
1313.
4s1.
313/2+911985IT=100209Rnn5292203636.
780.
233.
0s0.
3(35/2+)911985IT=100209Fr37681550.
0s0.
39/2911964α=893;β+=113209Frm892154659.
80.
7420ns1845/209Dr04ETJ2009IT=100209Ra1850504.
71s0.
085/29108Ha12T1967α≈90;β+≈10209Ram273050882.
80.
7117s513/2+08Ha12ETJ2008α≈90;β+≈10209Ac88405092ms11(9/2)9100He17T1968α=;β+=1#209Th16540903.
1ms1.
25/2#9710He25TD1996α=;β+209HgT:symmetrizedfrom98Zh22=35(+9–6)209BiT:average12Be06=20.
1(0.
8)03De11=19(2)209FrmT:frommeanlife09Dr04=606(26);209FrmT:also06Me03=360(140)originallyassignedto210Fr209AcT:average00He17=98(+59–27)96Ik01=82(+18–13)94Le05=91(+21–14)209AcT:and68Va04=100(50)209ThT:average10He25=1.
9(+1.
9–0.
7)96Ik01=3.
8(+6.
9–1.
5)No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1265TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)210Au2330#400#1#s(>300ns)1110Al24I2010β;βn210Hg5370#200#10#m(>300ns)0+0398Pf02I1998β;βn210Tl9246121.
30m0.
035+#031909β=100;βn=0.
0096210Pb14728.
01.
522.
20y0.
220+031900β=100;α=1.
9e–64210Pbm13450512785201ns178+031980IT=100210Bi14791.
51.
45.
012d0.
0051031905β=100;α=13.
2e–510210Bim14520.
21.
4271.
310.
113.
04My0.
069031953α=100210Po15952.
71.
2138.
376d0.
0020+031898α=100210Pom14395.
71.
21556.
960.
0398.
9ns2.
58+031968IT=100210Pon10895.
11.
25057.
610.
04263ns516+031985IT=100210At1197288.
1h0.
4(5)+031949β+≈100;α=0.
17520210Atm942282549.
60.
2482ns6(15)031970IT=100210Atn794484027.
70.
25.
66s0.
07(19)+031975IT=100210Rn960552.
4h0.
10+031952α=961;β+210Rnm790030171030AD644ns408+#031979IT210Rnn5750303857301.
06s0.
05(17)031979IT=100210Rnp3090306514301.
04s0.
07(22)+031986IT=100210Fr3333153.
18m0.
066+0305Ku06D1964α=714;β+210Ra460154.
0s0.
10+0308Ha12T1967α=;β+=4#210Ram2510152050.
01.
12.
32s0.
038+0304Re04ETJ1998IT=100210Ac879060350ms407+#0300He17T1968α=;β+=9#210Th140601916.
0ms3.
60+0310He25T1995α=;β+=1#210TlD:symmetrizedfromβn=0.
007(+7–4)%210RnnE:ENSDF2003:2147.
4(0.
2)keVabovethe8+level,quoted3812.
0(0.
2)+x210RnpE:ENSDF2003:4803.
7(0.
4)keVabovethe8+level,quoted6468.
3(0.
4)+x210FrT:other10Ka09=3.
4(0.
2)210FrI:anisomerwasclaimedin06Me03=360(140)ns;buthasbeenre-assignedto210FrI:209Frin09Dr04210RaT:also07Le14=2.
5(+1.
4–0.
7)and3.
5(+4.
8–1.
3)210RamT:average06Ha17=2.
28(0.
08)04Re04=2.
1(0.
1)04He25=2.
36(0.
04)210AcT:average00He17=335(+64–46)68Va04=350(50)211Hg620#200#10#s(>300ns)9/2+#1110Al24I2010β;βn211Tl608040100s401/2+#0412Be28T1998β=100;βn211Pb10491.
32.
636.
1m0.
29/2+041904β=100211Pbm878715170415159ns28(27/2+)05La01ET2005IT=100211Bi1185852.
14m0.
029/2041905α≈100;β=0.
2764211Bim10601111257101.
4s0.
3(25/2)041998IT=100211Po12432.
11.
3516ms39/2+041913α=100211Pom10970514625AD25.
2s0.
6(25/2+)041954α≈100;IT=0.
0164211Pon10296.
41.
62135.
70.
9243ns21(31/2)041998IT≈100;α211Pop7558.
82.
14873.
31.
72.
8s0.
7(43/2+)041998IT≈100;α211At11646.
82.
87.
214h0.
0079/2041940ε=58.
208;α=41.
808211Atm683134816.
21.
74.
23s0.
0739/20401Ba79TJ1971IT=100211Rn8755714.
6h0.
21/2041952β+=72.
617;α=27.
417211Rnm715216160314596ns28(17/2)041981IT=100211Rnn12516888014201ns4(63/2)041981IT=100211Fr4140123.
10m0.
029/20405Ku06D1964α=873;β+211Frm1717122423.
20.
2146ns14(29/2+)041986IT=100211Frn517124657.
30.
4123ns14(45/2)041986IT=100211Ra832813.
2s1.
45/2()0407Le14T1967α>93;β+300ns)0+1110Al24I2010β;βn212Tl1550#200#100s405+#0512Be28T1998β=100;βn212Pb7547.
22.
210.
64h0.
010+051905β=100212Pbm6212.
23.
0133525.
0s0.
38+#0512Re.
BET1998IT=100212Bi8117.
02.
060.
55m0.
061()0589Ha.
AD1905β=64.
066;α=35.
946;.
.
.
212Bim78703025030AD25.
0m0.
2(8,9)051978α=671;β=331;βα=301212Bin663930147830MD7.
0m0.
3>16051978β≈100;IT212Po10369.
01.
2299ns20+051906α=100212Pom7446529234AD45.
1s0.
6(18+)051962α≈100;IT=0.
072212At8627.
82.
4314ms2(1)051954α≈100;β+99;IT300ns)5/2+#1110Al24I2010β;βn213Tl17842760s401/2+12Be28T2010β=100;βn213Pb3202710.
2m0.
3(9/2+)071964β=100213Bi5230545.
59m0.
069/2071947β=97.
913;α=2.
093213Bim3930#200#1300#200#>168s25/2#08Ch.
AT2008213Po665333.
72s0.
029/2+071947α=100213At65795125ns69/2071968α=100213Atm521050137050110ns17071980IT=100213Atn36005029805045s4(49/2+)072003213Rn5698619.
5ms0.
19/2+#071967α=100213Rnm3990501710501.
00s0.
21(25/2+)071988IT=100213Rnn3460502240501.
36s0.
07(31/2)071988IT=100213Rnp28050598050164ns11(55/2+)071988IT=100213Fr3553534.
82s0.
149/2071964α=99.
445;β+=0.
565213Frm196351590.
410.
18505ns1421/2071971IT=100213Frn101552537.
620.
23238ns629/2+071971IT=100213Frp454258094.
80.
73.
1s0.
2(65/2)071989IT=100213Ra358212.
73m0.
051/2071955α=805;β+213Ram21262117684AD2.
20ms0.
05(17/2)0706Ku26TD1976IT≈99;α=0.
64213Ac616050738ms169/2#071968α=;β+213Th1212070144ms215/2#071968α=;β+=1.
4#213Thm1330070118031.
4s0.
413/2+#07Kh22TD2007IT=100213Thp12380#90#260#50#213Pa19660707ms39/2#0795Ni05TD1995α=100213TlT:symmetrizedfrom12Be28=46(+55–26);other10Ch19=101(+484–46)s213AtmE:1318.
1(0.
6)+x;xestimated50(50)byNUBASE213AtnE:2926+y;yestimated50(50)byNUBASE213RnmE:1664.
0(1.
0)+x;x=50(50)estimatedbyNUBASE213RnnE:2186.
7+x;x=50(50)estimatedbyNUBASE213RnpE:5929+y;y=50(50)estimatedbyNUBASE213RamE:derivedfromdifferenceinαdecayenergyintheAMEevaluation.
213RamE:76Ra37lessthan10keVabove1769.
7level,thus1775(3)keV213RamJ:17/2or13/2+asproposedin76Ra37213ThmE:uncertaintyestimatedbyNUBASE213PaT:symmetrizedfrom5.
3(+4.
0–1.
6)No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1267TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)214Hg11180#400#1#s(>300ns)0+1110Al24I2010β;βn214Tl6470#200#10#s(>300ns)5+#1110Al24I2010β;βn214Pb180.
82.
326.
8m0.
90+091904β=100214Pbm1210301390305.
9s0.
18+#12Re.
BETD2012IT=100214Bi12001119.
9m0.
410989Ha.
AD1904β≈100;α=0.
0211;βα=0.
003214Bim1000#100#200#100#>93s8#08Ch.
AT2008214Po4469.
61.
5164.
3s2.
00+091912α=100214At33794558ns101091949α=100214Atm33208599AD265ns30091982α893;β+300ns)3/2+#1110Al24I2010β;βn215Tl9910#300#5#s(>300ns)1/2+#1110Al24I2010β;βn215Pb4420#100#2.
45m0.
209/2+#111998β=100215Bi1649157.
6m0.
2(9/2)011953β=100215Bim2997151347.
52.
536.
9s0.
6(25/2)0103Ku26ETD2001IT=76.
24;β=23.
84215Po540.
12.
51.
781ms0.
0049/2+011911α=100;β=2.
3e–42215At12557100s209/2011944α=100215Rn116882.
30s0.
109/2+011952α=100215Fr318786ns59/2011970α=100215Ra253481.
67ms0.
019/2+#0100He17T1967α=100215Ram441281877.
80.
57.
31s0.
13(25/2+)0104He25T1983IT=100215Ran478182246.
90.
51.
39s0.
07(29/2)011998IT=100215Rap634050381050555ns10(43/2)011987IT=100215Ac603112170ms109/2011968α≈100;β+=0.
092215Acm7827121796.
00.
9185ns3021/2011983IT=100215Acn852050249050335ns10(29/2+)011983IT=100215Th1092291.
2s0.
2(1/2)011968α=100215Thm1234391421.
30.
3770ns609/2+#05Ku31ETD2005IT=100215Pa178707014ms29/2#011979α=100215PbT:otherpreliminaryresult96Ry.
B=36(1)s215BimE:1347.
3(0.
2)+x;x=20(20)estimatedbyNUBASE215BimT:earlyunpublishedreportbythesamegroup02Fr.
B=36.
9(0.
6)s,was215BimT:erroneously36.
4minNUBASE2003215RaT:also05Li17=1.
64(0.
04)notused215RamT:average04He25=7.
6(0.
2)98St24=6.
9(0.
3)88Fu10=7.
2(0.
2)215RapE:3756.
6(0.
6)+x;x=50(50)estimatedbyNUBASE215AcnE:2438+x;x=50(50)fromENSDF'2001215ThT:also07Le14=0.
63(+1.
26–0.
21)1268ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)216Hg19860#400#100#ms(>300ns)0+1110Al24I2010β;βn216Tl14720#300#2#s(>300ns)5+#1110Al24I2010β;βn216Pb7480#200#7#m(>300ns)0+1110Al24I2009β216Pbm8980#200#150040400ns108+#12Re.
BETD2012IT=100216Bi5874112.
25m0.
05(6,7)071989β≈100216Bim5898152419MD6.
6m2.
1(3)(#)071989β≈100216Po1784.
02.
2145ms20+071910α=100;2β216At22584300s301()071948α≈100;β300ns)1/2+#1110Al24I2010β;βn217Pb12240#300#30#s(>300ns)9/2+#1110Al24I2009β217Bi87301898.
5s0.
89/2#0303Ku25T1998β=100217Bim10200401470402.
31s0.
0627/2#12Go.
AET2012IT=100217Po588561.
514s0.
026(9/2+)0304Li28TJ1956α>95;β300ns)0+1110Al24I2009β218Bi132162733s1(6,7,8)0604De16J1998β=100218Po8358.
82.
33.
098m0.
0120+061904α≈100;β=0.
02#218At8099121.
5s0.
31#061943α≈100;β=0.
1#218Rn5217.
82.
435ms50+061948α=100218Fr705951.
0ms0.
61061949α=100218Frm71466864AD22.
0ms0.
5061982α≈100;IT218Frp7260#150#200#150#high218Ra66511125.
2s0.
30+061970α=100;2β+218Ac10840501.
08s0.
091#061970α=100218Acm10990#70#150#50#32ns9(9)94De04ET1994218Acn11370#70#530#50#103ns11(11+)061994IT=100218Th1236711117ns90+061973α=100218Pa1868418113s10061979α=100218U2191218550s1400+061992α=100218Um2401524210319AD640s200(8+)062005α=100218AcmE:atleast122.
5in94De04218AcnE:384.
49(0.
13)keVabove218Acm,fromENSDF218UT:symmetrizedfrom510(+170–100)218UmT:symmetrizedfrom560(+260–140)No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1269TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)219Pb20280#400#10#s(>300ns)9/2+#1110Al24I2009β219Bi16280#200#22s79/2#1112Be28T2009β=100219Po12681162#m(>300ns)9/2+#0898Pf02I1998β;α219At10397456s35/2#011953α≈97;β≈3219Rn8830.
92.
53.
96s0.
015/2+011903α=100219Fr8619720ms29/2011948α=100219Ra9395810ms3(7/2)+011952α=100219Ac115705011.
8s1.
59/2011970α=100;β+=1e–6#219Th14470501.
05s0.
039/2+#011973α=100;β+=1e–7#219Pa185405053ns109/2012005α=100;β+=5e–9#219U232905055s259/2+#011993α=100;β+=1.
4e–5#219Np29280#200#55#s9/2#α219UT:symmetrizedfrom42(+34–13);also05Le42=80(+100–30)220Pb23670#400#30#s(>300ns)0+1110Al24I2010β220Bi20820#300#7#s(>300ns)1#1110Al24I2009β;βn220Po152631840#s(>300ns)0+1198Pf02I1998β220At14376143.
71m0.
043(#)111989β=922;α=82220Rn10613.
62.
255.
6s0.
10+111900α=100;2β220Fr11483427.
4s0.
31+111948α≈100;β=0.
355220Ra10271817.
9ms1.
40+1100He17T1949α=100220Ac13744626.
36ms0.
19(3)1190An19T1970α=100;β+=5e–4#220Th14669229.
7s0.
60+111973α=100;ε=2e–7#220Pa20220#50#780ns1601#112005α=100;β+=3e–7#220U22930#100#60#ns0+α;β+220Np30310#200#100#ns1#α220RaT:average00He17=18(2)90An19=17(2)61Ru06=23(5)220AcT:average90An19=26.
4(0.
2)70Bo13=26.
1(0.
5)221Bi24100#300#5#s(>300ns)9/2#1110Al24I2009β;βn221Po19774202.
2m0.
79/2+#10Ch19T2010β221At16783142.
3m0.
23/2#071989β=100221Rn14473625.
7m0.
57/2+0797Li23T1956β=781;α=221221Fr1327954.
777m0.
0135/20710Wa42T1947α≈100;β=0.
004815;.
.
.
221Ra12964528s25/2+0794Bo28D1949α=100;14C=1.
2e–109221Ac145205052ms29/2#071968α=100221Th1693891.
68ms0.
06(7/2+)071970α=100221Pa20380505.
9s1.
79/2071983α=100221U24480#100#700#ns9/2+#07α;β+221Np29850#200#100#ns9/2#α221PoT:symmetrizedfrom10Ch19=112(+58–28)s221FrD:.
.
.
;14C=8.
8e–1111221FrD:βintensityisfrom97Ch53;14Cintensityisfrom94Bo28221FrT:average10Wa42=4.
768(0.
017)07Je07=4.
79(0.
02)221ThT:also05Li17=2.
3(0.
4)00He17=2.
0(+0.
3–0.
2)222Bi28670#300#2#s(>300ns)1#10Al24I2009β;βn222Po22490409.
1m7.
20+112010β222At209531654s10111989β=100222Rn16374.
02.
33.
8235d0.
00030+111899α=100222Fr163502114.
2m0.
32111975β=100222Ra14322533.
6s0.
40+1112Po13T1948α=100;14C=3.
0e–810222Ac1662255.
0s0.
51111949α=991;β+=11222Acm16830#150#200#150#1.
05m0.
05high111972α=;IT300ns)9/2#1110Al24I2009β;βn223Po27080#200#1#m(>300ns)9/2+#1110Al24I2010β223At234281450s73/2#011989β≈100;α=0.
008#223Rn20390824.
3m0.
47/2(#)011964β=100;α=0.
0004#223Fr18384.
02.
422.
00m0.
073/2()011939β≈100;α=0.
006223Ra17234.
82.
511.
43d0.
053/2+011905α=100;14C=8.
9e–84223Ac1782772.
10m0.
05(5/2)011948α=99;ε=1223Th193869600ms20(5/2)+011952α=100223Pa22320705.
1ms0.
39/2#0199Ho28T1970α=100;β+300ns)1#1110Al24I2010β;βn224Po29910#200#1#m(>300ns)0+1110Al24I2010β224At27711222.
5m1.
5122010β224Rn2244510107m30+971964β=100224Fr21795133.
33m0.
101971969β=100224Frx21900#100#100#100#MDcontamntn224Ra18827.
32.
23.
66d0.
040+971902α=100;14C=4.
0e–912224Ac2023542.
78h0.
170971948β+=90.
617;α=9.
417;β300ns)9/2+#1110Al24I2010β225At30400#300#2#m(>300ns)1/2+#1110Al24I2010β225Rn26534114.
66m0.
047/2091969β=100225Fr23821123.
95m0.
143/2091969β=100225Ra21994.
32.
914.
9d0.
21/2+091947β=100225Ac2163959.
920d0.
0033/2#0912Po14T1947α=100;14C=4.
5e–1214225Th2231158.
75m0.
04(3/2+)091949α≈90;ε≈10225Pa24340701.
7s0.
25/2#091958α=100225U273781261ms45/2+#0900He17T1989α=100225Np31590703#ms(>2s)9/2#0994Ye08ID1994α=100225UT:symmetrizedfrom00He17=59(+5–2);othersnotused03Ni10=135(+93–39)225UT:01Ku07=84(4)94An02=68(+45–20)92To02=95(15)and89He13=80(+40–10)226Po37550#400#20#s(>300ns)0+1110Al24I2010β226At34610#300#20#s(>300ns)1110Al24I2010β;βn226Rn28747107.
4m0.
10+961969β=100226Fr275411249s11961969β=100226Ra23669.
62.
31.
600ky0.
0070+9690We01D1898α=100;14C=2.
6e–96;2β226Ac24310329.
37h0.
12(1)(#)961950β=833;ε=173;α=0.
0062226Th23197530.
70m0.
030+9601Bo11D1948α=100;18O300ns)9/2+#1110Al24I2010β227At37480#300#20#s(>300ns)1/2+#1110Al24I2010β;βn227Rn328861420.
8s0.
75/2(+#)0197Ku20J1986β=100227Fr29686132.
47m0.
031/2+011972β=100227Ra27179.
52.
342.
2m0.
53/2+011953β=100227Ac25851.
12.
421.
772y0.
0033/2011902β=98.
6236;α=1.
3836227Th25806.
32.
518.
68d0.
091/2+011906α=100227Pa26832738.
3m0.
3(5/2)011948α=852;ε=152227U29022171.
1m0.
1(3/2+)011952α=100;β+300ns)1110Al24I2010β;βn228Rn352431865s20+971989β=100228Fr333691338s12971972β=100228Ra28942.
22.
45.
75y0.
030+971907β=100228Ac28896.
42.
56.
15h0.
023+971908β=100228Th26772.
32.
21.
9116y0.
00160+971905α=100;20O=1.
13e–1122228Pa28924422h13+971948β+=98.
02;α=2.
02228U29222149.
1m0.
20+971949α>95;ε300ns)1/2+#1110Al24I2010β;βn229Rn393621311.
9s1.
35/2+#092009β229Fr356741450.
2s0.
41/2+#0892Bo05T1975β=100229Ra32549144.
0m0.
25/2+081975β=100229Ac306981262.
7m0.
5(3/2+)081952β=100229Th29586.
82.
87.
932ky0.
0555/2+0811Ki16T1947α=100229Thm29586.
82.
80.
00760.
0005>1m3/2+#0809In01T1994IT;α229Pa2989841.
50d0.
05(5/2+)081949ε≈100;α=0.
485229Pam29910411.
60.
3420ns303/20898Le15EJD1982IT=100229U31211658m3(3/2+)081949β+≈80;α≈20229Np33780904.
00m0.
185/2+#0804Sa05TD1968α=6811;β+229Npp33940#100#160#50#5/2#229Pu373905091s263/2+#0810Kh06TD1994α=5020;β+=5020;SF20d)94He08=70(50)h229NpT:average04Sa05=4.
0(0.
4)68Ha14=4.
0(0.
2)229PuT:average10Kh06=67(+41–19)01Ca.
B=90(+71–27)229PuD:fromENSDF'97230Rn42050#200#10#s(>300ns)0+1110Al24I2010β230Fr395111619.
1s0.
5071987β=100230Ra345161093m20+071978β=100230Ac3383816122s3(1+)071973β=100;βSF=1.
2e–64230Th30864.
21.
875.
4ky0.
30+071907α=100;SF3230Pu36934151.
70m0.
170+0701Ca.
BT1990α≈100;β+230Am42930#130#1.
4m1.
3072003β+=100230ThD:.
.
.
;24Ne=5.
8e–1113230PaD:.
.
.
;α=0.
00321230UD:.
.
.
;SF300ns)1/2+#1110Al24I2010β231Fr420642517.
6s0.
61/2+#011985β=100231Ra3821611104.
0s0.
8(5/2+)0106Bo33T1983β=100231Ram382821166.
210.
0953s(1/2+)012001IT=100231Ac35763137.
5m0.
1(1/2+)011973β=100231Th33817.
51.
825.
52h0.
015/2+011911β=100;α=4e–11#231Pa33426.
02.
232.
76ky0.
113/2011918α=100;SF≤2e–11;.
.
.
231U3380834.
2d0.
1(5/2)(+#)011949ε≈100;α=0.
0041231Np356305048.
8m0.
2(5/2)(+#)011950β+=981;α=21231Pu38286268.
6m0.
53/2+#0199La14D1999β+=875;α=135231Am42440#300#1#mβ+;α231RaT:average06Bo33=104.
1(0.
8)85Hi02=103(3)231PaD:.
.
.
;24Ne=13.
4e–1017;23F=9.
9e–13231PuD:symmetrizedfrom90(+3–7)%and10(+7–3)%1272ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)232Fr45990#160#5.
5s0.
6(5)061990β=100;βSF1.
6%73Ja06300ns)1/2+#1110Al24I2010β;βn233Ra443221630s51/2+#051990β=100233Ac4130813145s10(1/2+)051983β=100233Th38733.
62.
021.
83m0.
04(1/2)+051935β=100233Pa37490.
02.
126.
975d0.
0133/2051938β=100233U36920.
32.
7159.
2ky0.
25/2+051947α=100;SF3233CmT:symmetrizedfrom23(+13–6)234Ra468903030s100+071990β=100;βSF80;β+93sandT=149(+95–42)s234PamE:lessthan10keVabove(3+)levelat73.
92(0.
02),seeENSDF2007234UD:.
.
.
;SF=1.
64e–922;28Mg=1.
4e–113;24Ne+26Ne=9e–127234AmD:.
.
.
;β+SF=0.
006618T:also04Sa05=3.
5(1.
3)notused234BkT:symmetrizedfrom140(+14–5)s235Ra51200#300#3#s5/2+#β235Ac473571462s41/2+#0808Ch.
AT2006β235Th44018137.
2m0.
11/2+#031969β=100235Pa422891424.
44m0.
11(3/2)031950β=100235U40920.
71.
8704My17/2031935IS=0.
72046;α=100;.
.
.
235Um40920.
81.
80.
07650.
000426m1/2+031966IT=100235Np41044.
92.
0396.
1d1.
25/2+031949ε≈100;α=0.
0026013235Pu421842125.
3m0.
5(5/2+)031957β+≈100;α=0.
00287235Am446305010.
3m0.
65/2#0304Sa05T1996β+≈100;α=0.
405235Cm48010#200#5#m5/2+#03β+;α235Cmp48060#210#50#50#am235Bk52700#400#1#mβ+;α235UD:.
.
.
;SF=7e–92;20Ne=8e–104;25Ne≈8e–10;28Mg=8e–10No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1273TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)236Ac51220404.
5m3.
610Ch19T2010β236Th462551437.
3m1.
50+061973β=100236Pa45334149.
1m0.
11()061963β=100;βSF=6e–84236U42446.
51.
823.
42My0.
030+061951α=100;SF=9.
4e–84236Um45197327503120ns2(0+)061969IT=876;SF=136;α250ns(5/2+)031994β=100239Un50707.
81.
9133.
79900.
0010780ns401/2+031975IT=100239Np49312.
62.
02.
356d0.
0035/2+031940β=100;α=5e–10#239Pu48590.
11.
824.
11ky0.
031/2+031946α=100;SF=3.
1e–106239Pum48981.
71.
8391.
5840.
003193ns47/2031955IT=100239Pun5169020031002007.
5s1.
0(5/2+)031970SF≈100;IT239Am49392.
22.
411.
9h0.
1(5/2)031949ε≈100;α=0.
0101239Amm518902002500200163ns12(7/2+)031969SF≈100;IT239Cm51150502.
5h0.
4(7/2)0302Sh.
CTD1952β+≈100;α=6.
2e–314239Cmp51390#110#240#100#1/2+239Bk54250#210#4#m(7/2+)0389Ha27Jβ+>99#;α500ns031969SF≈100;IT244Bk60716144.
35h0.
154#031972β+;α=0.
0063244Bkm61220#300#500#300#820ns60031972SF≈100;IT244Bkp60860#50#140#50#am244Cf61479.
42.
919.
4m0.
60+031956α≈100;ε244Es66030#180#37s4031973β+=;α=53;β+SF=0.
01244Esp66230#240#200#150#am244Fm68970#200#3.
12ms0.
080+0308Kh10TD1967SF≈100;β+1.
1Ey,from92Mo25;thus2β77;β+SF>10;α50;β+9y6+#991956α248Bkm681102130#70#23.
7h0.
21()991956β=705;ε=305;α=0.
001#248Bkp681305050#50#(5)248Cf672405334d30+991954α≈100;SF=0.
00293248Es70300#50#27m52#,0+#991956β+≈100;α≈0.
25;β+SF=3e–5248EsmnonexistentRN41m89Ha27I248Fm71899935.
1s0.
80+9911Ga19T1958α=937;β+=77;SF=0.
105248Md77150#240#7s3991973β+=8010;α=2010;.
.
.
248No80620#220#60;β+249Mdm77330#220#100#100#1.
9s0.
9(1/2)1101He35TJD2001α=100249No81780#280#57s125/2+#1103Be18T2003β+;α249BkD:.
.
.
;SF=47e–92249FmT:from04He28;others66Ak01=2.
6(0.
7)59Pe27=2.
5(1.
0)249MdT:average09He20=23(3)73Es01=24(4)249MdmT:symmetrizedfrom1.
5(+1.
2–0.
5)249NoT:symmetrizedfrom54.
0(+13.
9–9.
2)250Cm72990118300#y0+011966SF≈74;α≈18;β≈8250Bk7295243.
212h0.
0052011954β=100250Bkm72988435.
590.
1029s14+0108Ah02EJ1966IT=100250Bkn73036484.
12.
1AD213s87+0108Ah02EJ1972IT250Cf71172.
02.
013.
08y0.
090+011954α≈100;SF=0.
0773250Es73230#100#8.
6h0.
1(6+)011956β+>97;α250Esm73430#180#200#150#2.
22h0.
051()011970β+≈100;α250Fm74073830.
4m1.
50+0106Ba09T1954α>90;ε80;α50;α252Mdp805508040#100#am252No8287292.
45s0.
020+0611Ga19T1967α>66.
76;SF=32.
25;β+21/211Lo06T2011IT253Lr88580#200#&632ms46(7/2)0601He35TJD1985α=9010;SF=2.
621;β+=1#253Lrm88610#230#30#100#&1.
32s0.
14(1/2)0609He20TJD1985α=9010;SF=85;β+=1#253Rf93560#410#13ms5(7/2)(+#)0695Ho.
BTJ1997SF=;α253Rfm93760#440#200#150#52s14(1/2)(#)0697He29J1995SF=;α=5#253BkI:possibleidenticationin91Kr.
A;needsconrmation253EsD:SF=8.
7(0.
3)e–6%fromENSDF'99:fromα/SF=1.
15(0.
03)e7(1965Me02)253FmmE:211keVabove(7/2+)levelat130-150keV253MdT:symmetrizedfrom6.
4(+11.
6–3.
6)253NoT:average09He23=1.
56(0.
02)m09Qi04=1.
57(+0.
18–0.
15)m67Mi03=95(10)s253NoT:and67Gh01=105(20)s253NoJ:fromref.
11Lo06and10St14D:ε/e+=0.
45(0.
03)253NomE:average11An13=167.
5(0.
5)10St14=166.
7(1.
0)253NomT:average09He23=28(3)07Lo11=31.
1(2.
1)73Be33=31.
3(4.
1);253NomT:others11An13=22.
7(0.
5)and10St14=24(2)disagree253NonT:other11An13=627(5)253NonE:greaterthan1011andlessthan1380keV253LrT:average09He20=670(60)01He35=570(+70–60)253LrD:symmetrizedfromSF=1.
3(+3.
0–1.
0)%253LrT:othernotused10He11=700(+500–200)253LrmT:supersedes01He35=1.
49(+0.
30–0.
21);other10He11=1.
2(+0.
7–0.
4)253RfI:thestatewith≈1.
8sreportedinearlierENSDFisnotconrmed253RfT:symmetrizedfrom11(+6–3)253RfmT:symmetrizedfrom48(+17–10)1278ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)254Bk84390#300#1#m05β254Cf813421260.
5d0.
20+051955SF≈100;α=0.
312;2β254Es819924275.
7d0.
5(7+)051954α≈100;ε=0.
03#;.
.
.
254Esm82076384.
22.
5AD39.
3h0.
22+051954β=982;IT80;SF=0.
02012;α=0.
01254Non87950#300#3220#300#183.
8s1.
6(16+)10He10ETD2006IT=100;SF19.
101Ga20=21(8)76Be.
A=22(5)71Es01=22(5)255LrmT:average08Ha31=2.
6(0.
1)08An16=2.
53(0.
05)06Ch52=2.
53(0.
13)255LrnE:09Je02=1409keVabove9/2+,whichis160008Ha31>720D:αfrom09Je02255LrnT:unweighedaverage09Je02=1.
70(0.
03)08An16=1.
81(0.
02)08Ha31=1.
4(0.
1)255RfT:average06He27=1.
68(0.
09)01He35=1.
64(0.
11)255RfmT:symmetrizedfrom0.
8(+0.
5–0.
2)I:discardedinENSDF2007255DbT:symmetrizedfrom1.
6(+0.
6–0.
4)256Cf87040#310#12.
3m1.
20+991980SF=100;α=6.
2e–7#;2β256Es87190#100#25.
4m2.
4(1+,0)991981β=100256Esm87190#140#0#100#7.
6h(8+)991976β≈100;βSF=0.
002256Fm854877157.
6m1.
30+991955SF=91.
93;α=8.
13256Md87460#120#&30#m7#β+;α;SF256Mdm8762070160#100#&77m2(1)99FGK12bI1955β+=;α=9.
27;SF94;SF87;SF95;β+150000y,from86Lo16,thusSF90.
46;SF50;SF265Sgm112870#120#70#150#&16s2.
43/2+#0912Ha05T1994α>6516;SF265Bh116360#230#1.
19s0.
529904Ga29TD2004α=265Hs120901241.
96ms0.
163/2+#9909He20T1984α≈100;SF80;SF267Hsm122690#100#3924AD990s900504Fo08TD2004α=;IT267Mt127790#500#10#msα267Ds133920#140#10s89/2+#0595Gh04T1995α=100267RfT:symmetrizedfrom1.
3(+2.
3–0.
5);supersedes04Og12oneeventat2.
3h267DbT:symmetrizedfrom73(+350–33)m267SgT:symmetrizedfrom80(+60–20)s;other99Og.
B=19msnottrusted267BhT:symmetrizedfrom00Wi15=17(+14–6)267HsT:symmetrizedfrom52(+13–8)267HsmT:04Fo08(2events)=940(+120–45);othernottrusted04Mo40(1event)=803ms267DsT:onesingleevent,lifetime4s,thusT=2.
8(+13.
0–1.
3),see84Sc13268Rf115480#710#1#h0+α;SF268Db117060#530#30.
8h5.
00512Og02T2004SF≈100;β+268Dbp117220#540#160#100#268Sg116800#470#2#m0+α;SF268Bh120810#380#25#sα;SF268Hs122830#280#1.
42s1.
130+10Ni14TD2010α≈100268Mt129150#230#27ms65+#,6+#0504Mo26T1995α=100268Ds133650#300#100#s0+α268DbT:average12Og02=27.
9(+7.
8–5.
0)07St18=28(+11–4)268DbT:12Og02supersedes05Og02=29(+9–6)and04Og03=16(+19–6)268HsT:symmetrizedfrom0.
38(+1.
8–0.
17)268MtT:meanlifetimeof14eventsin04Mo26=30msand6eventsin02Ho11=60ms269Db119150#680#3#hα;SF269Sg119820#360#8.
0m6.
30510El06TD2010α≈100;SF269Bh121480#370#1#mα269Hs124590#130#27s179/2+#0502Ho11T1996α=100269Mt129310#460#100#msα269Ds13484030230s1109/2+#0595Ho03T1995α=100269SgT:oneαeventat185s,thusT=128(+613–58)s269SgT:ENSDF00=22(+32–11)sbasedon99Ni03workretractedbyauthorsin02Ni10269HsT:2eventsat19.
7and22.
0syield14(+26–6),see84Sc13269DsT:symmetrizedfrom170(+160–60)270Db122360#600#90h701010Og01TD2010SF=100270Sg121490#560#3#m0+α;SF270Bh124230#290#3.
8m3.
00707Og02TD2007α=100270Bhp124830#350#600#200#270Hs125090#250#30#s0+0503Tu05D2006α=100270Mt130710#170#6.
3ms1.
5052004α≈100270Ds13468050205s480+0511Ac.
AT2001α≈100;SF<0.
2270Dsm13607060139060AD10ms6(10)(#)052001α=;IT270DbT:oneeventat33.
4h,yields23.
15(110.
9-10.
6),see84Sc13270BhT:symmetrizedfrom61(+292–28)s270MtT:symmetrizedfrom5.
0(+2.
4–0.
3)270DsT:average11Ac.
A=200(+70–40)01Ho06=100(+140–40)270DsmT:symmetrizedfrom6.
0(+8.
2–2.
2)271Sg124760#590#3.
1m1.
60606Og05TD2004α=70;SF=30271Bh125990#440#1#m05α;SF271Hs127770#300#10#s2008α;SF271Mt131100#330#400#msα271Ds135950#100#&90ms4013/2#051998α=100271Dsm136020#100#6827AD&1.
7ms0.
49/2+#051995α=100271SgT:symmetrizedfrom1.
9(+2.
4–0.
6);supersedes04Og12=2.
4(4.
3-1.
0)α=50;SF=50271DsT:symmetrizedfrom69(+56–21)271DsmT:symmetrizedfrom1.
63(+0.
44–0.
29)No.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1283TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)272Sg126580#770#4#m0+α;SF272Bh128790#540#8.
8s2.
10512Og02T2004α≈100272Bhp128970#550#180#100#272Hs129010#510#10#s0+α;SF272Mt133580#490#400#msα;SF272Ds136020#410#200#ms0+SF272Rg142770#230#4.
5ms1.
05+#,6+#0504Mo26T1995α=100272BhT:symmetrizedfrom8.
2(+2.
5–1.
6);supersedes04Og03=9.
8(+11.
7–3.
5)272RgT:meanlifetimeof14eventsin04Mo26=5.
5msand6eventsin02Ho11=2.
3273Sg130020#500#5#mSF273Bh130630#740#1#mα;SF273Hs131970#370#910ms7203/2+#0510El06TD2010α≈100273Hsp132080#380#110#100#α;SF273Mt134510#480#800#msα;SF273Ds138380#130#240s12013/2#051996α=100273Dsm138580#130#19820EU120ms3/2+#051996α=100273Rg142640#530#2#msα273HsT:oneαeventat346ms,thusT=240(+1150–110)ms273HsT:99Ni03=1.
2(+1.
7–0.
6)sα-decayretractedbyauthorsin02Ni10273DsT:symmetrizedfrom170(+170–60)274Bh133710#600#3.
4m2.
71010Og01TD2010α=100274Hs133490#590#500#ms0+α;SF274Mt137160#350#850ms5400707Og02TD2007α=100274Ds139180#390#10#ms0+α;SF274Rg144620#180#29ms180508Mo09TD2004α≈100274BhT:oneeventat1.
3m,yields0.
901(+4.
32–0.
41),see84Sc13274MtT:symmetrizedfrom440(+810–170)ms274RgT:2eventsat9.
26and34.
3ms275Bh135690#600#5#mSF275Hs136620#590#290ms1500506Og05TD2004α=100275Hsp136860#600#240#100#275Mt138630#470#40ms300504Og03TD2004α=100275Ds141620#420#10#msα;SF275Rg145260#520#5#msα275HsT:symmetrizedfrom190(+220–70)ms;supersedes04Og12=150(+270–60)275MtT:symmetrizedfrom9.
7(+46–4.
4)276Hs138290#800#100#ms0+α;SF276Mt141210#550#730ms1600512Og02T2004α=100276Mtm141350#550#14070AD10s512Og02TD2012α=100276Mtp141510#560#300#100#276Ds142540#550#100#ms0+α;SF276Rg147490#630#10#msα;SF276Cn150350#600#100#s0+α;SF276MtT:symmetrizedfrom680(+200–120);supersedes04Og03=720(+870–250)276MtmT:symmetrizedfrom6(+8–2)277Hs141490#540#11ms93/2+#0510Du06TD2010SF=100277Hsm141590#550#100#100#130s10012Ho12TD2012SF=100277Hsp141960#550#470#100#277Mt142770#770#10#sα;SF277Ds145230#380#22ms1711/2+#0510El06TD2010α≈100;SF277Rg148170#570#10#msα;SF277Cn152430#140#990s4903/2+#051996α=100277HsT:symmetrizedfrom3.
0(+14.
4–1.
4);99Og10oneSFeventat16.
5m,nottrusted277HsmT:(SF1event)symmetrizedfrom34(+164–16)s277DsT:oneαeventat8.
21ms,thus5.
7(+27.
3–2.
6)277DsT:99Ni03=3.
0(+4.
7–1.
5)msα-decayretractedbyauthorsin02Ni10277CnT:foureventsat280s,1406s,1100sand1220s,see84Sc131284ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)278Mt145600#630#29s231010Og01TD2010α=100278Mtp145980#660#380#200#278Ds146280#630#270#ms0+α;SF278Rg150430#360#8ms50707Og02TD2007α=100278Cn152910#440#2#ms0+α;SF278Ed158890#180#2.
3ms1.
30512Mo25TD2004α≈100278MtT:10Og01oneα-decayeventat11.
0s278RgT:symmetrizedfrom4.
2(+7.
5–1.
7)278EdT:3eventsat0.
344,4.
930and0.
667ms;supersedes08Mo09279Mt147250#670#30#sα;SF279Ds149130#600#210ms500506Og05TD2004SF=90;α=10279Dsp149320#610#190#100#279Rg151570#470#640ms5100504Og03TD2004α=100279Rgp151780#480#210#100#279Cn155130#470#5#msα;SF279Ed159240#700#1#msα;SF279DsT:symmetrizedfrom200(+50–40);supersedes04Og12=180(+50–30)and279DsT:04Og07=290(+350–100);279DsT:others:09St21oneSFeventat185ms,07Ei02oneSFeventat536ms279RgT:symmetrizedfrom170(+810–80)280Ds150260#820#11s60+0501Og01TD1999SF=100280Rg153830#560#3.
8s0.
80512Og02T2004α=100280Rgp153950#570#120#100#280Cn155700#580#5#ms0+α;SF280Ed161080#700#10#msα;SF280DsT:3eventsat6.
93,14.
3and7.
4yield6.
6(+9–2.
4),see84Sc13280RgT:symmetrizedfrom3.
53(+0.
99–0.
63);supersedes04Og03=3.
6(+4.
3–1.
3)281Ds153240#550#14s43/2+#0510Du06TD2004SF=8512;α=1512281Dsm153470#550#230#160#0.
9s0.
712Ho12TD2012α=100281Rg154960#820#37s171010Og01TD2010SF=100281Cn158120#390#370ms2903/2+#0510El06TD2010α≈100;SF281Ed161600#700#100#msα;SF281DsT:average10Du06=20(+20–7)07Og01=11.
1(+5.
0–2.
7);supersedes281DsT:04Og07=9.
6(+5.
0–2.
5);99Og10oneαeventat1.
6m,nottrusted281DsD:symmetrizedfromSF=91(+7–16)%;α=9(+16–7)%281DsmT:symmetrizedfrom0.
25(+1.
18–0.
11)s281RgT:symmetrizedfrom26(+25–8)281CnT:oneαeventat140ms,thus97(+465–44)281CnT:99Ni03=0.
89(+1.
30–0.
45)α-decayretractedbyauthorsin02Ni10282Rg157530#670#1.
9s1.
50510Og01TD2010α=100282Cn158820#660#900s2400+0506Og05TD2004SF=100282Ed163640#360#140ms900707Og02TD2007α=100282RgT:oneeventat740ms,yields513(2457-234)ms,see84Sc13282CnT:symmetrizedfromSF=820(+300–180);supersedes04Og12=500(+330–140)282CnT:also10El06oneSFeventat522s;09St21oneSFat3600s282EdT:symmetrizedfrom73(+134–29)283Rg158860#730#30#sα;SF283Cn161400#610#4.
1s1.
00606Og05TD2004α=;SF<10283Ed164480#480#380ms3100504Og03TD2004α=100283CnT:symmetrizedfrom3.
8(+1.
2–0.
7);supersedes04Og12=4.
0(+1.
3–0.
7)and283CnT:04Og07=6.
1(+7.
2–2.
2);other07Ho18=6.
9(+6.
9–2.
3),SF=50283CnT:09St21oneαeventat1.
92s283CnT:FourSFeventsat99Og07=9.
3m,3.
8m,99Og05=3.
0m,0.
9m,nottrusted283EdT:symmetrizedfrom100(+490–45)284Cn162230#850#104ms200+0510Du06TD2004SF=100284Ed166480#580#1.
01s0.
240512Og02T2004α=100284CnT:average10Du06=101(+50–25)07Og01=97(+31–19);supersedes284CnT:04Og12=101(+41–22)and04Og07=98(+41–23)284CnTD:01Og013α'sat53.
9s,10.
3s,18.
0s,nottrusted284EdT:symmetrizedfrom940(+290–180)ms;supersedes04Og03=480(+580–170)msNo.
12G.
Audietal:TheNUBASEevaluationofnuclearanddecayproperties1285TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)285Cn164980#560#32s95/2+#0510Du06TD2004α=100285Cnm165740#560#750#170#15s1212Ho12TD2012α=100285Ed167420#830#8s41010Og01TD2010α=100285Fl171060#440#470ms38010El06TD2010α≈100;SF285CnT:average10Du06=30(+30–10)07Og01=29(+13–7);supersedes285CnT:04Og07=34(+17–9);99Og10oneeventat15.
4m,nottrusted285CnmT:symmetrizedfrom4.
0(+19.
1–1.
8)s285EdT:symmetrizedfrom5.
5(+5.
0–1.
8)285FlT:oneαeventat181ms,thus125(+600–57);escapeα,noQαmeasured285FlT:99Ni03=580(+870–290)α-decayretractedbyauthorsin02Ni10286Ed169730#670#70s601010Og01TD2010α=100286Edp170040#680#310#100#286Fl171610#660#140ms300+0506Og05TD2004SF≈60;α≈40286EdT:oneeventat28.
3s,yields19.
6(93.
9-12.
9),see84Sc13286FlT:symmetrizedfrom130(+40–20);supersedes04Og12=160(+70–30)and286FlT:04Og07=290(+540–110);alsooneαeach10El06=76ms,09St21=301ms287Ed170830#760#2#mα;SF287Fl173990#610#520ms1300506Og05TD2004α=100287Ef177640#490#120ms1000504Og03TD2004α=100287FlT:symmetrizedfrom480(+160–90);supersedes04Og12=510(+180–100)287FlT:supersedes04Og07=1.
1(+1.
3–0.
4);99Og072evts1.
32,14.
4snottrusted287FlT:also09St21oneαeventat815ms287EfT:symmetrizedfrom32(+155–14)288Fl174720#850#750ms1400+0511Ga19TD2004α=100288Ef179540#580#190ms400512Og02T2004α=100288FlT:average11Ga19=520(+220–130)07Og01=800(+270–160);supersedes288FlT:10Du06=470(+240–120);04Og12=800(+320–180)and04Og07=630(+270–140)288FlT:01Og01=1800(+2100–600)re-assignedto289Fl288EfT:symmetrizedfrom173(+52–32);supersedes04Og03=87(+105–30)289Fl177370#560#2.
4s0.
65/2+#0510Du06TD2004α=100289Flm178330#560#960#190#1.
1s0.
812Ho12TD2012α=100289Ef180360#830#340ms1801010Og01TD2010α=100289Lv184590#530#RN2#ms5/2+#0002Ni10Iα289FlT:average10Du06=0.
97(+0.
97–0.
32)07Og01=2.
6(+1.
2–0.
7);289FlT:supersedes04Og07=2.
7(+1.
4–0.
7);289FlT:99Og10oneeventat30.
4s,nottrusted289FlmT:symmetrizedfrom0.
28(+1.
35–0.
13)s289EfT:symmetrizedfrom220(+260–80)289LvT:99Ni03=600(+860–300)α-decayretractedbyauthorsin02Ni10290Ef182550#680#60ms501010Og01TD2010α=100290Efp182660#690#110#100#290Lv185030#660#8ms30+0506Og05TD2004α=100290EfT:oneeventat23ms,yields15.
9(+76.
2–7.
3),see84Sc13290LvT:symmetrizedfrom7.
1(+3.
2–1.
7);supersedes04Og07=15(+26–6)291Ef183570#820#1#sα;SF291Lv187300#610#28ms150506Og05TD2004α=100291Eh191450#630#2#msα;SF291LvT:symmetrizedfrom18(+22–6);supersedes04Og07=6.
3(+11.
6–2.
5)292Lv187920#850#24ms120+0504Og12TD2004α=100292Eh193250#700#10#msα;SF292LvT:symmetrizedfrom18(+16–6)292LvT:01Og01reportedoneeventat46.
9ms,re-assignedtonextisotope1286ChinesePhysicsC(HEP&NP)Vol.
36TableI.
TheNUBASE2012table(continued,ExplanationofTableonpage1176)NuclideMassexcessExcitationHalf-lifeJπEnsReferenceYearofDecaymodesand(keV)energy(keV)discoveryintensities(%)293Lv190480#560#80ms400507Og01TD2004α=100293Lvm191410#560#930#200#80ms6012Ho12TD2012α=100293Eh193970#830#18ms81010Og01TD2010α=100293Ei198930#730#RN1#ms1/2+#0002Ni10Iα293LvT:symmetrizedfrom61(+57–20);supersedes04Og07=53(+62–19)293LvmT:symmetrizedfrom20(+96–9)ms293EhT:symmetrizedfrom14(+11–4)293EiT:99Ni03=120(+180–60)α-decayretractedbyauthorsin02Ni10294Eh196040#690#290ms2301010Og01TD2010α=100294Ei199270#660#1.
4ms0.
70+0506Og05TD2006α=100294EhT:oneeventat112ms,yields78(+374–36),see84Sc13294EiT:symmetrizedfrom890(+1070–310)s;supersedes04Og12oneeventat1.
8ms295Ei201430#640#10#ms04Og05TDα295EiT:04Og05reportsoneαeventat2.
55ms;re-assignedto294Ei