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TheNUBASEevaluationofnuclearanddecaypropertiesG.
Audia,§,O.
Bersillonb,J.
BlachotbandA.
H.
WapstracaCentredeSpectrometrieNucleaireetdeSpectrometriedeMasse,CSNSM,IN2P3-CNRS&UPS,Batiment108,F-91405OrsayCampus,FrancebServicedePhysiqueNucleaire,CEA,B.
P.
12,F-91680Bruy`eres-le-Chatel,FrancecNationalInstituteofNuclearPhysicsandHigh-EnergyPhysics,NIKHEF,POBox41882,1009DBAmsterdam,TheNetherlandsAbstractThispaperpresentstheNUBASEevaluationofnuclearanddecaypropertiesofnuclidesintheirground-andisomeric-states.
Allnuclidesforwhichsomeexperimentalinformationisknownareconsidered.
NUBASEusesextensivelytheinformationgivenbythe"EvaluatedNuclearStructureDataFiles"andincludesthemassesfromthe"AtomicMassEvaluation"(AME,secondpartofthisissue).
Butitalsoincludesinformationfromrecentliteratureandismeanttocoverallexperimentaldataalongwiththeirreferences.
Incasenoexperimentaldataisavailable,trendsinthesystematicsofneighboringnuclideshavebeenused,wheneverpossible,toderiveestimatedvalues(labeledinthedatabaseasnon-experimental).
Adoptedproceduresandpoliciesarepresented.
AMDC:http://csnwww.
in2p3.
fr/AMDC/1.
IntroductionThepresentevaluationrespondstotheneedsexpressedbythenuclearphysicscom-munity,fromfundamentalphysicstoappliednuclearsciences,foradatabasewhichcontainsvaluesforthemainbasicnuclearpropertiessuchasmasses,excitationen-ergiesofisomers,half-lives,spinsandparities,decaymodesandtheirintensities.
A*ThisworkhasbeenundertakenwiththeencouragementoftheIUPAPCommissiononSymbols,Units,Nomenclature,AtomicMassesandFundamentalConstants(SUN-AMCO).
§Correspondingauthor.
E-mailaddress:audi@csnsm.
in2p3.
fr(G.
Audi).
4G.
Audietal.
/NuclearPhysicsA729(2003)3–128requirementisthatalltheinformationshouldbeproperlyreferencedinthatdatabasetoallowchecksontheirvalidity.
Oneoftheapplicationsofsuchadatabaseisthe"AtomicMassEvaluation"(AME)inwhichitisessentialtohaveclearidenticationofthestatesinvolvedinadecay,areactionoramass-spectrometricline.
Thisisthemainreasonforwhichthesetwoevaluationsarecoupledinthepresentissue.
Furthermore,calculationsrequiringradioactiveparametersfornuclearapplications(e.
g.
reactors,wastemanagement,nuclearastrophysics)needtoaccessthisbasicinformationonanynuclide.
Inthepreparationofanuclearphysicsexperiment,suchadatabasecouldalsobequiteuseful.
Mostofthedatamentionedaboveareinprinciplealreadypresentintwoevaluatedles:the"EvaluatedNuclearStructureDataFiles"(ENSDF)[1]andthe"AtomicMassEvaluation"(AME2003,secondpartofthisissue).
Thedemandforadatabaseasdescribedabovecouldbethuspartiallyfullledbycombiningthemina'horizontal'structure(whichexistsintheAME,butnotinENSDF).
NUBASEistherefore,atarstlevel,acriticalcompilationofthesetwoevaluations.
WhilebuildingNUBASE,wefounditnecessarytoexaminetheliterature,rstly,toreviseseveralofthecollectedresultsinENSDFandensurethatthementioneddataarepresentedinamoreconsistentway;secondly,tohaveasfaraspossiblealltheavailableexperimentaldataincluded,notonlytherecentones(updatingrequirement),butalsothosemissedinENSDF(completenessrequirement).
Thisimpliedsomeevaluationwork,whichappearsintheremarksaddedintheNUBASEtableandinthediscussionsbelow.
Fullreferencesaregivenforalloftheaddedexperimentalinformation(cf.
Section2.
7).
Thereisnostrictcut-offdateforthedatafromliteratureusedinthepresentNUBASE2003evaluation:alldataavailabletousuntilthematerialwassent(November19,2003)tothepublisherhavebeenincluded.
Thosewhichcouldnotbeincludedforspecialreasons,liketheneedforaheavyrevisionoftheevaluationatatoolatestage,areaddedinremarkstotherelevantdata.
ThecontentsofNUBASEaredescribedbelow,alongwithsomeofthepoliciesadoptedinthiswork.
UpdatingproceduresofNUBASEarepresentedinSection3.
Finally,theelectronicdistributionofNUBASEandaninteractivedisplayofitscontentswithaWorldWideWebJavaprogramorwithaPC-programaredescribedinSection4.
ThepresentpublicationupdatesandincludesalltheinformationgiveninthepreviousandveryrstevaluationofNUBASE[2],publishedin1997.
2.
ContentsofNUBASENUBASEcontainsexperimentallyknownnuclearpropertiestogetherwithsomevaluesestimatedbyextrapolationofexperimentaldatafor3177nuclides.
NUBASEalsoG.
Audietal.
/NuclearPhysicsA729(2003)3–1285containsdataonisomericstates.
Wepresentlyknow977nuclideshavingoneormoreexcitedisomersaccordingtoourdenitionbelow.
InthepresentevaluationweextendedthedenitionofisomerscomparedtoNUBASE'97whereonlystateswithhalf-livesgreaterthan1millisecondwereconsidered.
Inpresentmassspectrometricexperimentsperformedataccelerators,withimmediatedetectionoftheproducednuclei,isomerswithhalf-livesasshortas100nsmaybepresentinthedetectedsignals.
Weaimedatincludingasmuchaspossibleallthosewhichplayormightplayinthenearfuturearoleinsuchexperiments.
WeincludealsothedescriptionofthosestatesthatareinvolvedinmassmeasurementsandthusentertheAME2003.
Foreachnuclide(A,Z),andforeachstate(groundorexcitedisomer),thefollowingquantitieshavebeencompiled,andwhennecessaryevaluated:massexcess,excitationenergyoftheexcitedisomericstates,half-life,spinandparity,decaymodesandintensitiesforeachmode,isotopicabundancesofthestablenuclei,andreferencesforallexperimentalvaluesoftheaboveitems.
Inthedescriptionbelow,referencestopapersthatarealsoquotedintheNUBASEtablearegivenwiththesameNuclearStructureReferencekeynumberstyle[3].
Theyarelistedattheendofthisissue(AME2003,PartII,p.
579).
InNUBASE'97,thenamesandthechemicalsymbolsusedforelements104to109werethoserecommendedthenbytheCommissiononNomenclatureofInorganicChemistryoftheInternationalUnionofPureandAppliedChemistry(IUPAC).
Sincethen,unfortunatelyfortheresultingconfusion,thenameswerechangedandmoreovertwoofthemweredisplaced[4](seealsoAME2003,PartI,Section6.
5).
TheusershouldthereforebecarefulwhencomparingresultsbetweenNUBASE'97andthepresentNUBASE2003fornuclideswithZ≥104.
Thenallyadoptednamesandsymbolsare:104rutherfordium(Rf),105dubnium(Db),106seaborgium(Sg),107bohrium(Bh),108hassium(Hs),and109meitnerium(Mt),whiletheprovisionalsymbolsEa,Eb,Eiareusedforelements110,111,118.
Besidesconsideringallnuclidesforwhichatleastonepieceofinformationisexperimentallyavailable,wealsoincludedunknownnuclides-forwhichwegiveestimatedproperties-inordertoensurecontinuityofthesetoftheconsiderednuclidesatthesametimeinN,inZ,inAandinNZ.
Thechartofthenuclidesdenedthiswayhasasmoothcontour.
Asfaraspossible,onestandarddeviations(1σ)aregiventorepresenttheuncer-taintiesconnectedwiththeexperimentalvalues.
Unfortunately,authorsdonotalwaysdenethemeaningoftheuncertaintiestheyquote;undersuchcircumstances,theuncertaintiesareassumedtobeonestandarddeviations.
Inmanycases,theuncer-taintiesarenotgivenatall;wethenestimatedthemonthebasisofthelimitationsofthemethodofmeasurement.
ValuesanderrorsthataregivenintheNUBASEtablehavebeenrounded,evenifunroundedvalueswerefoundinENSDForintheliterature.
Incaseswherethetwo6G.
Audietal.
/NuclearPhysicsA729(2003)3–128furthest-leftsignicantdigitintheerrorwerelargerthanagivenlimit(30fortheenergies,tomaintainstrictidentitywithAME2003,and25forallotherquantities),valuesanderrorswereroundedoff(seeexamplesinthe'Explanationoftable').
Inveryfewcases,whenessentialfortraceability,weaddedaremarkwiththeoriginalvalue.
Whennoexperimentaldataexistforanuclide,valuescanoftenbeestimatedfromobservedtrendsinthesystematicsofexperimentaldata.
IntheAME2003,massesestimatedfromsystematictrendswerealreadyaggedwiththesymbol'#'.
TheuseofthissymbolhasbeenextendedinNUBASEtoallotherquantitiesandhasthesamemeaningofindicatingnon-experimentalinformation.
2.
1.
MassexcessThemassexcessisdenedasthedifferencebetweentheatomicmass(inmassunits)andthemassnumber,andisgiveninkeVforeachnuclearstate,togetherwithitsonestandarddeviationuncertainty.
ThemassexcessvaluesgiveninNUBASEareexactlythoseoftheAME2003evaluation,giveninthesecondpartofthisissue.
Itsometimeshappensthatknowledgeofmassescanyieldinformationonthedecaymodes,inparticularregardingnucleon-stability.
Suchinformationhasbeenusedhere,ascanbeseeninthetablefor10He,19Na,39Sc,62Asor63As.
Insomecaseswerejectedclaimedobservationofdecaymodes,whennotallowedbyenergeticconsideration.
Asanexample,ENSDF2000compilesfor142Bavemeasurementsofdelayedneutrondecayintensities,whereasQ(βn)=2955(7)keV.
Figure1complementsthemaintableindisplayingtheprecisionsonthemasses,inacolor-codedchart,asafunctionofNandZ.
2.
2.
IsomersIntherstversionofNUBASEin1997[2],asimpledenitionfortheexcitediso-merswasadopted:theywerestatesthatlivelongerthan1millisecond.
AlreadyinNUBASE97,wenoticedthatsuchasimpledenitionhadseveraldrawbacks,par-ticularlyforalphaandprotondecayingnuclides:whereasforβ-decayalimitof1millisecondwasacceptable(theshortest-livedknownβ-decayingnuclide(35Na)hasahalf-lifeof1.
5millisecond),forαorprotondecay,severalcasesareknownwhereanisomerwithahalf-lifefarbelow1millisecondlivesstilllongerthantheground-state.
Asmentionedearlier,thedenitionofisomersisnowextendedtoincludealargenumberofexcitedstates,withhalf-livesasshortas100ns,thatareofinterestformassspectrometricworksataccelerators.
Isomersaregiveninorderofincreasingexcitationenergyandidentiedbyappending'm','n','p'or'q'tothenuclidename,e.
g.
90Nbfortheground-state,90Nbmfortherstexcitedisomer,90NbnforthesecondG.
Audietal.
/NuclearPhysicsA729(2003)3–1287Figure1:Chartofthenuclidesfortheprecision'u'onmasses(createdbyNUCLEUS-AMDC).
8G.
Audietal.
/NuclearPhysicsA729(2003)3–128one,90Nbpand90Nbqforrespectivelythethirdandfourth.
InNUBASE97wecouldnotreportinanormalwaythethirdexcitedisomerof178Tawithhalf-life59ms,becauseofpoornessofnotation;thenewnotationadoptedhereremovesalsosuchalimitation.
Theexcitationenergycanbederivedfromanumberofdifferentexperimentalmethods.
Whenthisenergyisderivedfromamethodotherthanγ-rayspectrometry,theoriginisindicatedbyatwo-lettercodeandthenumericalvalueistakenfromAME.
Otherwise,thecodeisleftblankandthenumericalvalueistakenfromENSDForfromliteratureupdate.
Whentheexistenceofanisomerisunderdiscussion(e.
g.
141Tbm)itisaggedwith'EU'intheorigineldtomean"existenceuncertain".
Acommentisgenerallyaddedtoindicatewhyitsexistenceisquestioned,orwherethismatterhasbeendiscussed.
Dependingonthedegreeofourcondenceinthisexistence,wecanstillgiveamassexcessvalueandanexcitationenergy,oromitthemaltogether(e.
g.
138Pmn).
Inthelattercase,themention"non-existent"appearsinplaceofthatexcitationenergy.
Whenanisomerhasbeenreported,andlaterprovednottoexist(e.
g.
184Lum),itisaggedwith'RN'intheorigineldtomean"reported,non-existent".
Insuchcasewegiveofcoursenomassexcessvalueandnoexcitationenergy,and,asinthecaseofthe'EU'sabove,theyarereplacedbythesamemention"non-existent".
Note:wehaveextendedtheuseofthetwoags'EU'and'RN'tocaseswherethediscoveryofanuclide(e.
g.
260Fm)isquestioned.
Inthiscasehoweverwealwaysgiveanestimate,derivedfromsystematictrends,forthegroundstatemasses.
Inseveralcases,ENSDFgivesalowerandahigherlimitforanisomericexcitationenergy.
Auniformdistributionofprobabilitieshasbeenassumedwhichyieldsavalueatthemiddleoftherangeanda1σuncertaintyof29%ofthatrange(cf.
AppendixBoftheAME2003,PartI,foracompletedescriptionofthisprocedure).
Anexampleis136Laforwhichitisknownthattheexcitedisomerliesabovethelevelat230.
1keV,but,asexplainedinENSDF,therearegoodexperimentalindicationsthatthedifferencebetweenthesetwolevelsliesbetween10and40keV.
WepresentthisinformationasE=255(9)keV.
However,ifthatdifferencewouldhavebeenderivedfromtheoryorfromsystematics,theresultingEisconsideredasnon-experimentalandthevalueaggedwiththe'#'symbol.
IncasethattheuncertaintyσontheexcitationenergyEisrelativelylargecomparedtothevalue,theassignmenttogroundstateandisomericstateisuncertain.
Ifσ>E/2aagisaddedintheNUBASEtable.
Asaresultofthiswork,theorderingsofseveralground-statesandisomeric-stateshavebeenreversedcomparedtothoseinENSDF.
TheyareaggedintheNUBASEtablewiththe'&'symbol.
InseveralcaseswefoundevidenceforastatebelowtheadoptedENSDFground-state.
Also,inmanyothercases,thesystematicsofnuclideswiththesameparitiesinNandZstronglysuggestthatsuchalowerstateshouldexist.
G.
Audietal.
/NuclearPhysicsA729(2003)3–1289TheyhavebeenaddedintheNUBASEtableandcanbelocatedeasily,sincetheyarealsoaggedwiththe'&'symbol.
Inafewcases,newinformationonmassescanalsoleadtoreversalofthelevelordering.
ThankstothecouplingoftheNUBASEandtheAMEevaluations,allchangesinlevelorderingarecarefullysynchronized.
NewsonisomericexcitationenergiesInterestingly,thetechniqueofinvestigatingprotondecayofveryproton-richnu-clidesgivesinformationonisomericexcitationenergies.
Thus,suchworkon167Ir[1997Da07]showsthatithasanisomericexcitationenergyE=175.
3(2.
2)keV.
Thisinformationisdisplayedbythe'p'symbolfollowingtheexcitationenergy.
Inaddi-tion,studyoftheα-decayseriesoftheseactivitiesnotonlyshowedthatanumberofαlinesearlierassignedtoground-statesbelonginrealitytoisomers,butalsoallowedtoderivevaluesfortheirexcitationenergies.
Anothercaseofsuchachangeis181Pb.
Theαdecayhalf-lifethatwasprevioulyassignedto181Pbmisnowassignedtotheground-state,followingtheworkofTothetal.
[1996To01]whoshowed,rst,thatcontrarytoapreviouswork,thereisnoαlineathigherenergythantheonejustmentioned,andsecond,thattheobservedαisincorrelationwiththedecayofthedaughter177Hg,whichisalsomostprobablya5/2state.
2.
3.
Half-lifeForsomelightnuclei,thehalf-life(T1/2)isdeducedfromtheleveltotalwidth(Γcm)bytheequationΓcmT1/2hln2:T1/2(s)4.
5621022/Γcm(MeV).
Quiteoftenuncertaintiesforhalf-livesaregivenasymmetricallyT+ab.
Iftheseuncertaintiesareusedinsomeapplications,theyneedtobesymmetrized.
Earlier(cf.
AME'95)aroughsymmetrizationwasused:takethecentralvaluetobethemid-valuebetweentheupperandlower1σ-equivalentlimitsT+(ab)/2,anddenetheuncertaintytobetheaverageofthetwouncertainties(a+b)/2.
Astrictstatisticalderivation(seeAppendix)showsthatabetterapproximationforthecentralvalueisobtainedbyusingT+0.
64*(ab).
TheexactexpressionfortheuncertaintyisgivenintheAppendix.
Whentwoormoreindependentmeasurementshavebeenreported,theyareaver-aged,whilebeingweighedbytheirreportedprecision.
Whiledoingthis,weconsidertheNORMALIZEDCHI,χn(or'consistencyfactor'or'Birgeratio'),asdenedinAME2003,PartI,Section5.
2.
Onlywhenχnisbeyond2.
5,dowedepartfromthestatisticalresult,andadopttheexternalerrorfortheaverage,followingthesame10G.
Audietal.
/NuclearPhysicsA729(2003)3–128policyasdiscussedandadoptedinAME2003,PartI,Section5.
4.
Veryrarely,whentheBirgeratioχnissolargethatweconsiderallerrorsgivenasnon-relevant,doweadoptthearithmeticaverage(unweighed)fortheresultandthecorrespondingerror(basedonthedispersionofvalues).
Inallsuchcases,aremarkisaddedtothedata,givingthelistofvaluesthatwereaveraged,and,whenrelevant,thevalueoftheBirgeratioχnandthereasonforourchoice.
Inthecaseofexperimentsinwhichextremelyrareeventsareobserved,andwheretheresultsareveryasymmetric,wedidnotaveragedirectlythehalf-livesderivedfromdifferentworks,butinstead,whentheinformationgiveninthepaperswassufcient(e.
g.
264Hsor269Hs),wecombinedthedelaytimesoftheindividualevents,asprescribedbySchmidtetal[1984Sc13].
Somemeasurementsarereportedasarangeofvalueswithmostprobablelowerandupperlimits.
Theyaretreated,asexplainedabove(cf.
Section2.
2),asauniformdistributionofprobabilitieswithavalueatthemiddleoftherangeanda1σuncertaintyof29%ofthatrange(cf.
AppendixBoftheAME2003foracompletedescriptionofthisprocedure).
Forsomenuclidesidentiedbyusingatime-of-ightspectrometer,anupperoralowerlimitonthehalf-lifeisgiven.
i)Forobservedspecies,wegivethisimportantbutisolatedpieceofinformation(lowerlimit)inplaceoftheuncertaintyonthehalf-life,andwithinbrackets(e.
g.
36Mg,p.
34).
Theuserofourtableshouldbecarefulinthatthislimitcanbeveryfarbelowtheeventuallymeasuredhalf-life.
Tohelptoavoidconfusion,wenowgive,inaddition,anestimate(asalwaysinthepresenttwoevaluations,aggedwith#)forthehalf-lifederivedfromtrendsinsystematics.
ii)Fornuclidessoughtforbutnotobserved,wegivethefoundupperlimitinplaceofthehalf-life.
UpperlimitsforundetectednuclideshavebeenevaluatedforNUBASEbyF.
Pougheon[1993Po.
A],basedonthetime-of-ightoftheexperimentalsetupandtheyieldsexpectedfromthetrendsinneighboringnuclides(e.
g.
19Na).
Whenhalf-livesfornuclideswiththesameparitiesinZandNarefoundtovarysmoothly(seeFig.
2),interpolationorextrapolationisusedtoobtainreasonableestimates.
2.
4.
SpinandparityAsinENSDF,valuesarepresentedwithoutandwithparenthesesbaseduponstrongandweakassignmentarguments,respectively(seetheintroductorypagesofRef.
[5]).
Unfortunately,thelatterincludeestimatesfromsystematicsortheory.
Wherewecandistinguishthem,weuseparenthesesiftheso-called"weak"argumentisanexperimentalone,butthesymbol'#'intheothercases.
Thesurveymighthavenotbeencomplete,andthereadermightstillndnon-aggednon-experimentalcases(theG.
Audietal.
/NuclearPhysicsA729(2003)3–12811Figure2:Chartofthenuclidesforhalf-lives(createdbyNUCLEUS-AMDC).
12G.
Audietal.
/NuclearPhysicsA729(2003)3–128authorswillgratefullyappreciatementionofsuchcasestoimprovefutureversionsofNUBASE).
Ifspinandparityarenotknownfromexperiment,theycanbeestimated,insomecases,fromsystematictrendsinneighboringnuclideswiththesameparitiesinNandZ.
Thisisoftentrueforodd-Anuclides(seeFig.
3andFig.
4),butalso,notsorarely,forodd–oddones,ascanbeseeninFig.
5.
Theseestimatedvaluesarealsoaggedwiththe'#'symbol.
InseveralcaseswereplacedtheENSDFsystematicsbyourown.
ThereviewofnuclearradiiandmomentsofOtten[1989Ot.
A],inwhichthespinswerecompiled,wasusedtocheckandcompletethespinvaluesinNUBASE.
2.
5.
DecaymodesandintensitiesThemostimportantpolicy,fromourpointofview,incodingtheinformationforthedecaymodes,isinestablishingaverycleardistinctionbetweenadecaymodethatisenergeticallyallowedbutnotyetexperimentallyobserved(representedbyaquestionmarkalone,whichthusreferstothedecaymodeitself),andadecaymodethatisactuallyobservedbutforwhichtheintensitycouldnotbedetermined(representedby'=',thequestionmarkreferringheretothequantityaftertheequalsign).
AsinENSDF,nocorrectionshavebeenmadetonormalizetheprimaryintensitiesto100%.
Besidesdirectupdatesfromtheliterature,wealsomadeuseofpartialevaluationsbyotherauthors(withproperquotation).
Theyarementionedbelow,whendiscussingsomeparticulardecaymodes.
Theβ+decayInthecourseofourworkwerenedsomedenitionsandnotationsfortheβ+decay,inordertopresentmoreclearlytheavailableinformation.
Wedenotewithβ+thedecayprocessthatincludesbothelectroncapture,denotedε,andthedecaybypositronemission,denotede+.
Onecanthensymbolicallywrite:β+=ε+e+.
Asiswellknown,foranavailableenergybelow1022keV,onlyelectroncaptureεisallowed;abovethatvaluebothprocessescompete.
Remark:thisnotationisnotthesameastheoneimplicitlyusedinENSDF,wherethecombinationofbothmodesisdenoted"EC+B+".
Whenbothmodescompete,theseparatedintensitiesarenotalwaysavailablefromexperiment.
Mostofthetime,separatedvaluesinENSDFarecalculatedones.
Incontinuationofoneofourgeneralpolicies,inwhichweretainwheneverpossibleonlyexperimentalinformation,wedecidednottoretainENSDF'scalculatedseparatedvalues(whicharescarceandnotalwaysupdated).
Mostoften,itisinsomeveryparticularcasesthatthedistinctionisofimportance,likeinthecaseofrareorextremelyrareprocesses(e.
g.
91Nb,54Mn,119Tem).
Then,theuseofournotationisuseful.
G.
Audietal.
/NuclearPhysicsA729(2003)3–12813Figure3:Chartofthenuclidesforspinsandparities.
Shownareonlytheodd-Zeven-Nnuclides(createdbyNUCLEUS-AMDC).
14G.
Audietal.
/NuclearPhysicsA729(2003)3–128Figure4:Chartofthenuclidesforspinsandparities.
Shownareonlytheeven-Zodd-Nnuclides(createdbyNUCLEUS-AMDC).
G.
Audietal.
/NuclearPhysicsA729(2003)3–12815Figure5:Chartofthenuclidesforspinsandparities.
Shownareonlytheodd-Zodd-Nnuclides(createdbyNUCLEUS-AMDC).
16G.
Audietal.
/NuclearPhysicsA729(2003)3–128Inthesameline,wegivebothelectroncaptureε-delayedssionandthepositrone+-delayedssionwiththesamesymbolβ+SF.
Thedouble-βdecayInthecourseofourworkwefoundthathalf-livesfordouble-βdecaywerenotalwaysgiveninaconsistentwayinENSDF.
ForNUBASEwedecidedtogiveonlyhalf-lifevaluesorupper-limitsrelatedtothedominantprocess,whichisingeneralthetwo-neutrinogs-gstransition(oneexceptionmaybe98Mo,forwhichtheneutrinolessdecayispredictedtobefaster,see[2002Tr04]).
Noattemptwasmadetoconverttothesamestatisticalcondencelevel(CL)upperlimitresultsgivenbydifferentauthors.
TheexcellentrecentcompilationofTretyakandZdesenko[2002Tr04]wasofgreathelpinthispartofourwork.
Theβ-delayeddecaysFordelayeddecays,intensitieshavetobeconsideredcarefully.
Bydenition,theintensityofadecaymodeisthepercentageofdecayingnucleiinthatmode.
Buttraditionally,theintensitiesofthepureβdecayandofthoseofthedelayedonesaresummedtogiveanintensitythatisassignedtothepureβdecay.
Forexample,ifthe(A,Z)nuclidehasadecaydescribed,accordingtothetradition,by'β=100;βn=20',thismeansthatfor100decaysoftheparent(A,Z),80(A,Z+1)and20(A–1,Z+1)daughternucleiareproducedandthat100electronsand20delayed-neutronsareemitted.
Astrictnotation,followingthedenitionabove,wouldhavebeeninthiscase'β=80;βn=20'.
Howeverwedecidedtofollowthetraditionanduseinourworkthenotation:'β=100;βn=20'.
Thisalsoholdsformorecomplexdelayedemissions.
Adecaydescribedby:'β=100;βn=30;β2n=20;βα=10'correspondstotheemissionof100electrons,(30+2*20=70)delayed-neutronsand10delayed-αparticles;andintermsofresidualnuclides,to40(A,Z+1),30(A–1,Z+1),20(A–2,Z+1)and10(A–4,Z–1).
Moregenerally,Pn,thenumberofemittedneutronsper100decays,canbewritten:Pn=∑ii*βin;andsimilarexpressionsforαorprotonemission.
Thenumberofresidualβdaughter(A,Z+1)is:β∑iβin∑jβjα.
.
.
Anotherspecialremarkconcernstheintensityofaparticularβ-delayedmode.
Theprimaryβ-decaypopulatesseveralexcitedstatesintheβ-daughter,thatwillfurtherdecaybyparticleemission.
However,inthecasewherethedaughter'sgroundstatealsodecaysbythesameparticleemission,someauthorsincludeditsdecayG.
Audietal.
/NuclearPhysicsA729(2003)3–12817inthevaluefortheconcernedβ-delayedintensity.
Wedecidednottodosofortworeasons.
Firstly,becausetheenergiesoftheparticlesemittedfromtheexcitedstatesaregenerallymuchhigherthanthatfromtheground-state,implyingdifferentsubsequentprocesses.
Secondly,becausethecharacteristictimesforthedecaysfromtheexcitedstatesarerelatedtotheparent,whereasthoseforthedecaysfromthedaughter'sgroundstateareduetothedaughter.
Forexample9Cdecaysthroughβ+modewithanintensityof100%ofwhich12%and11%totwoexcitedp-emittingstatesin9B,and17%toanα-emittingstate.
Wegivethusβ+p=23%andβ+α=17%,fromwhichtheuserofourtablecanderivea60%directfeedingoftheground-stateof9B.
Inaslightlydifferentexample,8Bdecaysonlytotwoexcitedstatesin8Bewhichinturndecaybyαandγemission,butnottothe8Beground-state.
Wewritethusβ+=100%andβ+α=100%,thedifferenceofwhichleaves0%forthefeedingofthedaughter'sgroundstate.
Finally,wewanttodrawtotheattentionoftheuserofourtable,thatthepercentagesare,bydenition,relatedto100decayingnuclei,nottotheprimarybeta-decayfraction.
Anillustrativeexampleisgivenbythedecayof228Np,forwhichthedelayed-ssionprobabilityisgivenintheoriginalpaperas0.
020(9)%[1994Kr13],butthisnumberisrelativetotheεprocess,theintensityofwhichis59(7)%.
Wethusrenormalizedthedelayed-ssionintensityto0.
012(6)%ofthetotaldecay.
Incollectingthedelayedprotonandαactivities,theremarkableworkofHardyandHagberg[1989Ha.
A],inwhichthisphysicswasreviewedanddiscussed,wasanappreciablehelpinourwork.
ThereviewofHonkanen,¨Ayst¨oandEskola[6]ondelayed-protonshasalsobeenveried.
Similarly,thereviewofdelayedneutronemissionbyHansenandJonson[1989Ha.
B]wascarefullyexaminedandusedinourtable,aswellastheevalua-tionofRudstam,AleklettandSihver[1993Ru01].
2.
6.
IsotopicabundancesIsotopicabundancesaretakenfromthecompilationofK.
J.
R.
RosmanandP.
D.
P.
Tay-lor[1998Ro45]andarelistedinthedecayeldwiththesymbolIS.
Theyaredisplayedasgivenin[1998Ro45],i.
e.
wedidnotevenapplyourroundingpolicy.
2.
7.
ReferencesTheyearofthearchivalleisindicatedforthenuclidesevaluatedinENSDF;otherwise,thisentryisleftblank.
ReferencesforalloftheexperimentalupdatesaregivenbytheNSRkeynumber[3],andlistedattheendofthisissue(p.
579).
Theyarefollowedbyone,twoorthreeone-lettercodeswhichspecifytheaddedormodiedphysicalquantities(seethe18G.
Audietal.
/NuclearPhysicsA729(2003)3–128Figure6:Chartofthenuclidesfordecaymodes(createdbyNUCLEUS-AMDC).
G.
Audietal.
/NuclearPhysicsA729(2003)3–12819ExplanationofTable).
Incaseswheremorethanonereferenceisneededtodescribetheupdates,theyaregiveninaremark.
Noreferenceisgivenforsystematicvalues.
TheABBWreferencekeyisusedincaseswhereitmaynotappearunambiguouslythatre-interpretationsofthedataweremadebythepresentauthors.
3.
UpdatingprocedureNUBASEisupdatedviatworoutes:fromENSDFaftereachnewA-chainevaluation(orfromthebi-annualreleases),anddirectlyfromtheliterature.
ENSDFlesareretrievedfromNNDCusingtheon-lineservice[1]andtransferredthroughtheInternet.
Twoofthepresentauthors[7]developedprogramstosucces-sively:checkthateachZintheA-chainhasan'adoptedlevels'dataset;ifnot,acorre-spondingdatasetisgeneratedfromthe'decay'or'reaction'dataset,extractthe'adoptedlevels'datasetsfromENSDF,extractfromthesedatasetstherequiredphysicalquantities,andconvertthemintoaformatsimilartotheNUBASEformat.
TheprocesseddataareusedtoupdatemanuallythepreviousversionofNUBASE.
Thisstepisdoneseparatelybythefourauthorsandcross-checkeduntilfullagreementisreached.
TheENSDFisupdatedgenerallybyA-chains,and,morerecently,alsobyindividualnuclides.
Itscontentshoweverisverylarge,sinceitencompassesallthecomplexnuclearstructureanddecayproperties.
Thisisahugeeffort,anditisnowonderthatsomeolderdata(includingannualreports,conferenceproceedings,andtheses)aremissing,andthatsomerecentdatahavenotyetbeenincluded.
Wherewenoticesuchmissingdata,theyareanalyzedandevaluated,asabove,independentlybythefourauthorsandtheproposedupdatingsarecompared.
MostoftenthesenewdataareincludedinthenextENSDFevaluationandthecorrespondingreferencescanberemovedfromtheNUBASEdatabase.
4.
DistributionanddisplaysofNUBASEFullcontentofthepresentevaluationisaccessibleon-lineatthewebsiteoftheAtomicMassDataCenter(AMDC)[8]throughtheWorldWideWeb.
AnelectronicASCIIlefortheNUBASEtable,forusewithcomputerprograms,isalsodistributedbytheAMDC.
Thislewillnotbeupdated,toallowstablereferencedataforcalculations.
Anyworkusingthatleshouldmakereferencetothepresentpaperandnottotheelectronicle.
ThecontentsofNUBASEcanbedisplayedbyaJavaprogramJVNUBASE[9]throughtheWorldWideWebandalsowithaPC-programcalled"NUCLEUS"[10].
Bothcan20G.
Audietal.
/NuclearPhysicsA729(2003)3–128beaccessedordownloadedfromtheAMDC.
TheywillbeupdatedregularlytoallowtheusertocheckforthelatestavailableinformationinNUBASE.
5.
ConclusionsA'horizontal'evaluateddatabasehasbeendevelopedwhichcontainsmostofthemainpropertiesofthenuclidesintheirgroundandisomericstates.
Thesedataoriginatefromacriticalcompilationoftwoevaluateddatasets:theENSDF,updatedandcompletedfromtheliterature,andtheAME.
Theguidelinesinsettingupthisdatabaseweretocoverascompletelyaspossiblealltheexperimentaldata,andtoprovideproperreferenceforthoseusedinNUBASEandnotalreadyincludedinENSDF;thistraceabilityallowsanyusertochecktherecommendeddataand,ifnecessary,undertakeare-evaluation.
Asaresultofthis'horizontal'work,agreaterhomogeneityindatahandlingandpresentationhasbeenobtainedforallofthenuclides.
Furthermore,isomericassignmentsandexcitationenergieshavebeenreconsideredonarmerbasisandtheirdataimproved.
ItisexpectedtofollowupthissecondversionofNUBASEwithimprovedtreatments.
Amongthem,weplantocompletetheextensionduetothenewdenitionofisomertostateswithhalf-livesbetween100nsand1millisecondthatareavailableatthelarge-scalefacilities.
Anotherforeseeableimplementationwouldbetoprovidethemainα,γ,conversionandX-raylinesaccompanyingthedecays.
NUBASEcouldalsobeextendedtoothernuclearproperties:energiesoftherst2+statesineven-evennuclides,radii,moments.
.
.
Aninterestingfeaturethatisalreadyimplemented,butnotyetcheckedsufcientlytobeincludedhere,istogiveforeachnuclide,ingroundorisomeric-state,theyearofitsdiscovery.
6.
AcknowledgementsWewishtothankourmanycolleagueswhoansweredourquestionsabouttheirexperimentsandthosewhosentuspreprintsoftheirpapers.
Continuousinterest,discussions,suggestionsandhelpinthepreparationofthepresentpublicationbyC.
Thibaultwerehighlyappreciated.
WeappreciatethehelpprovidedbyJ.
K.
Tuliinsolvingsomeofthepuzzlesweencountered.
SpecialthanksareduetoS.
AudiforthepreparationofthecolorguresfromtheNUCLEUSprogram,andtoC.
GaulardandD.
Lunneyforcarefulreadingofthemanuscript.
A.
H.
W.
expresseshisgratitudetotheNIKHEF-KlaboratoryandespeciallytoMr.
K.
Huyserforhiscontinualhelp,andJ.
B.
totheISN-GrenobleandDRFMC-Grenoblelaboratoriesforpermissiontousetheirfacilities.
G.
Audietal.
/NuclearPhysicsA729(2003)3–12821510152000XmbaσFigure7:Simulatedasymmetricprobabilitydensityfunction(heavysolidline)andtheequivalentsymmetricone(dashedline).
AppendixA.
SymmetrizationofasymmetricuncertaintiesExperimentaldataaresometimesgivenwithasymmetricuncertainties,X+ab.
Ifthesedataaretobeusedwithotheronesinsomeapplications,theiruncertaintiesmayneedtobesymmetrized.
Asimplemethod(Method1),usedearlier,consistedintakingthecentralvaluetobethemid-valuebetweentheupperandlower1σ-equivalentlimitsX+(ab)/2,anddenetheuncertaintytobetheaverageofthetwouncertainties(a+b)/2.
Analternativemethod(Method2)istoconsidertherandomvariablexassociatedwiththemeasuredquantity.
Forthisrandomvariable,weassumetheprobabilityden-sityfunctiontobeanasymmetricnormaldistributionhavingamodal(mostprobable)valueofx=X,astandarddeviationbforxX(Fig.
7).
Thentheaveragevalueofthisdistributionisx=X+2/π(ab),withvarianceσ2=(12/π)(ab)2+ab.
(1)Themedianvaluemwhichdividesthedistributionintotwoequalareasisgiven,fora>b,byerfmX√2a=ab2a,(2)andbyasimilarexpressionforb>a.
Wedenetheequivalentsymmetricnormaldistributionwearelookingforasadistributionhavingameanvalueequaltothemedianvaluemofthepreviousdistributionwithsamevarianceσ.
22G.
Audietal.
/NuclearPhysicsA729(2003)3–128TableA.
Examplesoftreatmentofasymmetricuncertaintiesforhalf-lives.
Method1istheclassicalmethod,usedpreviously,asintheAME'95.
Method2istheonedevelopedinthisAppendixandusedforhalf-livesandintensitiesofthedecaymodes.
NuclideOriginalT1/2Method1Method276Ni240+550–190ms420±370470±390222U1.
0+1.
0–0.
4s1.
3±0.
71.
4±0.
7264Hs327+448–120s490±280540±300266Mt1.
01+0.
47–0.
24ms1.
1±0.
41.
2±0.
4IftheshiftmXofthecentralvalueissmallcomparedtoaorb,expression(2)canbewritten[11]:mXπ/8(ab)0.
6267(ab).
Inordertoallowforasmallnon-linearitythatappearsforhighervaluesofmX,weadoptforMethod2therelationmX=0.
64(ab).
TableAillustratestheresultsfrombothmethods.
InNUBASE,Method2isusedforthesymmetrizationofasymmetrichalf-livesandofasymmetricdecayintensities.
Referencesquotedinthetextas[1993Po.
A]or[2002Tr04](NSRstyle)arelistedunder"ReferencesusedintheAME2003andtheNUBASE2003evaluations",p.
579.
References[1]T.
W.
Burrows,Nucl.
Instrum.
Meth.
286(1990)595;http://www.
nndc.
bnl.
gov/[2]G.
Audi,O.
Bersillon,J.
BlachotandA.
H.
Wapstra,Nucl.
Phys.
A624(1997)1;http://csnwww.
in2p3.
fr/AMDC/nubase/nubase97.
pdf[3]NuclearStructureReference(NSR):acomputerleofindexedreferencesmaintainedbyNNDC,BrookhavenNationalLaboratory;http://www2.
nndc.
bnl.
gov/nsr/[4]CommissiononNomenclatureofInorganicChemistry,PureandAppliedChemistry69(1997)2471.
[5]GeneralPolicies,NuclearDataSheets,71(1994)v.
G.
Audietal.
/NuclearPhysicsA729(2003)3–12823[6]J.
Honkanen,J.
¨Ayst¨oandK.
Eskola,Phys.
Scr.
34(1986)608.
[7]O.
BersillonandJ.
Blachot,NEANDC(E)246/L,INDC(FR)071/L,September1991.
[8]TheNUBASE2003lesintheelectronicdistributionandcomplementaryinforma-tioncanberetrievedfromtheAtomicMassDataCenter(AMDC)throughtheWeb:http://csnwww.
in2p3.
fr/amdc/[9]E.
Durand,ReportCSNSM97-09,July1997;http://csnwww.
in2p3.
fr/AMDC/nucleus/stg-durand.
doc[10]B.
Potet,J.
DuoandG.
Audi,ProceedingsENAM'95conference,Arles,June1995,p.
151;http://csnwww.
in2p3.
fr/AMDC/nucleus/arlnucleus.
ps[11]R.
D.
Evans,TheAtomicNucleus(McGraw-Hill,NewYork,1955)p.
766.
24G.
Audietal.
/NuclearPhysicsA729(2003)3–128TableI.
TableofnuclearanddecaypropertiesEXPLANATIONOFTABLEDataarepresentedingroupsorderedaccordingtoincreasingmassnumberA.
NuclideNuclidicname:massnumberA=N+Zandelementsymbol(forZ>109seeSection2).
Elementindicationswithsufx'm','n','p'or'q'indicateassignmentstoexcitedisomericstates(dened,seetext,asupperstateswithhalf-liveslargerthan100ns).
Sufxes'p'and'q'indicatealsonon-isomericlevels,ofuseintheAME2003.
Sufx'r'indicatesastatefromaprotonresonanceoccurringin(p,γ)reactions(e.
g.
28Sir).
Sufx'x'appliestomixturesoflevels(withrelativeratioR,giveninthe'Half-life'column),e.
g.
occurringinspallationreactions(indicated'spmix'inthe'Jπ'column)orssion('fsmix').
MassexcessMassexcess[M(inu)A],inkeV,anditsonestandarddeviationuncertaintyasgiveninthe'AtomicMassEvaluation'(AME2003,secondpartofthisvolume).
Roundingpolicy:incaseswherethefurthest-leftsignicantdigitintheerrorislargerthan3,valuesanderrorsareroundedoff,butnottomorethantensofkeV.
(Examples:2345.
67±2.
78→2345.
7±2.
8,2345.
67±4.
68→2346±5,but2346.
7±468.
2→2350±470).
#inplaceofdecimalpoint:valueanduncertaintyderivednotfrompurelyexperi-mentaldata,butatleastpartlyfromsystematictrends(cf.
AME2003).
ExcitationenergyForexcitedisomersonly:energydifference,inkeV,betweenlevelsadoptedashigherlevelisomerandgroundstateisomer,anditsonestandarddeviationuncertainty,asgiveninAME2003whenderivedfromtheAME,otherwiseasgivenbyENSDF.
Theroundingpolicyisthesameasforthemassexcess(seeabove).
#inplaceofdecimalpoint:valueanduncertaintyderivedfromsystematictrends.
Theexcitationenergyisfollowedbyitsorigincodewhenderivedfromamethodotherthanγ-rayspectrometry:MDMassdoubletRQReactionenergydifferenceADαenergydifferenceBDβenergydifferencepprotondecayXLLX-raysNmestimatedvaluederivedwithhelpofNilssonmodelWhentheexistenceofanisomerisquestionablethefollowingcodesareused:EUexistenceofisomerisunderdiscussion(e.
g.
141Tbm).
Ifexistenceisstronglydoubted,noexcitationenergyandnomassaregiven.
Theyarereplacedbythemention"non-existent"(e.
g.
138Pmn).
RNisomerisprovednottoexist(e.
g.
184Lum).
Excitationenergyandmassarereplacedbythemention"non-existent".
Remark:codesEUandRNarealsousedwhenthediscoveryofanuclide(e.
g.
260Fm)isquestioned.
Inthiscasehoweverwealwaysgiveanestimate,derivedfromsystematictrends,forthegroundstatemass.
Isomericassignment:IncasetheuncertaintyσontheexcitationenergyEislargerthanhalfthatenergy(σ>E/2),thesequantitiesarefollowedbyanasterix(e.
g.
130Inand130Inm).
&Incasetheorderingoftheground-andisomeric-statesarereversedcom-paredtoENSDF,anampersandsignisadded(e.
g.
90Tcand90Tcm).
G.
Audietal.
/NuclearPhysicsA729(2003)3–12825Half-lifes=seconds;m=minutes;h=hours;d=days;y=years;1y=31556926sor365.
2422dadoptedvaluesforNUBASE(seetext)STABLE=stablenuclideornuclideforwhichnonitevalueforhalf-lifehasbeenfound.
#valueestimatedfromsystematictrendsinneighboringnuclideswiththesameZandNparities.
subunits:ms:103smillisecondky:103ykiloyears:106smicrosecondMy:106ymegayearns:109snanosecondGy:109ygigayearps:1012spicosecondTy:1012yterayearfs:1015sfemtosecondPy:1015ypetayearas:1018sattosecondEy:1018yexayearzs:1021szeptosecondZy:1021yzettayearys:1024syoctosecondYy:1024yyottayearForisomericmixtures:Ristheproductionratioofexcitedisomericstatetoground-state.
JπSpinandparity:()uncertainspinand/orparity.
#valuesestimatedfromsystematictrendsinneighboringnuclideswiththesameZandNparities.
highhighspin.
lowlowspin.
amsameJπasα-decayparent;Forisomericmixtures:mix(spmixandfsmixifcomingfromspallationandssionrespec-tively).
EnsYearofthearchivalleoftheENSDF(inordertoreducethewidthoftheTable,thetwodigitsforthecenturiesareomitted).
ReferenceReferencekeys:(inordertoreducethewidthoftheTable,thetwodigitsforthecenturiesareomitted;attheendofthisvolumehowever,thefullreferencekey-numberisgiven:1992Pa05andnot92Pa05)92Pa05UpdatestoENSDFderivedfromregularjournal.
ThesekeysaretakenfromNuclearDataSheets.
Wherenotyetavailable,thestyle03Ya.
1isprovisionallyadopted.
95Am.
AUpdatestoENSDFderivedfromabstract,preprint,privatecommunication,con-ference,thesisorannualreport.
ABBWRe-interpretationbythepresentauthors.
Thereferencekey-numbersarefollowedbyone,twoorthreelettercodeswhichspeciestheaddedormodiedphysicalquantities:Tforhalf-lifeJforspinand/orparityEfortheisomerexcitationenergyDfordecaymodeand/orintensityIforidentication26G.
Audietal.
/NuclearPhysicsA729(2003)3–128DecaymodesDecaymodesfollowedbytheirintensities(in%),andtheironestandarddeviationanduncertainties.
Thespecialnotation1.
8e–12standsfor1.
8*1012.
intensitiesTheuncertaintiesaregiven-onlyinthiseld-intheENSDF-style:α=25.
923standsforα=25.
9±2.
3%Theorderingisaccordingtodecreasingintensities.
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:ISIsotopicabundanceAremarkonthecorrespondingnuclideisgivenbelowtheblockofdatacorrespondingtothesameA.
Remarks.
Fornuclidesindicatedwithanasterixattheendoftheline,remarkshavebeenadded.
TheyarecollectedingroupsattheendofeachblockofdatacorrespondingtothesameA.
Theystartwithacodeletter,liketheonesfollowingthereferencekey-number,asgivenabove,indicatingtowhichquantitytheremarkapplies.
Theygive:i)Continuationforthelistofdecays.
Inthiscase,theremarkstartswiththreedots.
ii)Informationexplaininghowavaluehasbeenderived.
iii)Reasonsforchangingavalueoritsuncertaintyasgivenbytheauthorsorforrejectingit.
iv)Complementaryreferencesforupdateddata.
v)Separatevaluesenteringanadoptedaverage.
G.
Audietal.
/NuclearPhysicsA729(2003)3–12827NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)1n8071.
31710.
0005613.
9s0.
61/2+0002PaDGTβ=1001H7288.
97050.
0001STABLE1/2+0098Ro45DIS=99.
9885701HD:allisotopicabundancesinNUBASEarefrom98Ro452H13135.
72160.
0003STABLE1+99IS=0.
0115703H14949.
80600.
002312.
32y0.
021/2+00β=1003He14931.
21480.
0024STABLE1/2+98IS=0.
00013733Li28670#2000#RNp-unstable98p4H25900100139ys1029803Me11Tn=1004He2424.
91560.
0001STABLE0+98IS=99.
99986334Li2532021091ys929865Ce02Tp=1004HT:width=3.
28(0.
23)MeV;also91Go19=4.
7(1.
0)outweighed,notused5H32890100>910ys(1/2+)0203Go11T2n=1005He1139050700ys303/202n=1005Li1168050370ys303/202p=1005Be38000#4000#1/2+#02p5HT:fromwidth260ns)5/2+#99Sa06Iβ;βn31Ne30840#900#3.
4ms0.
87/2#01β=100;βn31Na1265021017.
0ms0.
4(3/2+)0193Kl02Jβ=100;βn=375;31Mg321712230ms203/2+0195Re.
ADβ=100;βn=6.
22031Al1495420644ms25(5/2,3/2)+01β=100;βn1.
5s)0+02Le.
AIβ;βn34Na32760#900#5.
5ms1.
01+01ABBWDβ=100;β2n≈50;βn≈1534Mg881023020ms100+01β=100;βn34Al293011056.
3ms0.
54#0101Nu01Tβ=100;βn=12.
52534Si19957142.
77s0.
200+01β=10034P24558512.
43s0.
081+01β=10034S29931.
790.
11STABLE0+01IS=4.
292834Cl24439.
780.
181.
5264s0.
00140+01β+=10034Clm24293.
420.
18146.
360.
0332.
00m0.
043+01β+=55.
46;IT=44.
6634Ar18377.
20.
4845ms30+01β+=10034K1480#300#260ns34NaD:βn≈15%,β2n≈50%estimatedfromPn=βn+2*β2n=115(20)%in84La0334NaD:assumingβn/β2n=0.
3fromtrendsinthe30Na-33Naseries:26413434AlD:from95Re.
A;stronglyconictingwith89Ba50=27(5)%and88Mu08=54(12)%34AlT:also95Re.
A=42(6)ms35Na39580#950#1.
5ms0.
53/2+#01β=100;βn=35Mg16150#400#70ms407/2#0195Re.
ADβ=100;βn=524635Al13018038.
6ms0.
45/2+#0101Nu01TDβ=100;βn=411335Si1436040780ms1207/2#0195Re.
ADβ=100;βn200ns)0+0189Gu03Iβ36Al578021090ms4001β=100;βn1.
5s)3/2+#02Le.
AIβ;βn37Mg29250#900#40#ms(>260ns)7/2#0196Sa34Iβ;βn37Al995033020#ms(>1s)3/2+#0191Or01Iβ37Si658017090ms607/2#0195Re.
ADβ=100;βn=171337P18990402.
31s0.
131/2+#01β=10037S26896.
360.
205.
05m0.
027/201β=10037Cl31761.
530.
05STABLE3/2+01IS=24.
22437Ar30947.
660.
2135.
04d0.
043/2+01ε=10037K24800.
200.
091.
226s0.
0073/2+01β+=10037Ca1316222181.
1ms1.
0(3/2+)0195Tr03Dβ+=100;β+p=82.
1737Sc2840#300#7/2#p37NaI:also02No11>260ns38Mg35000#500#1#ms(>260ns)0+0197Sa14Iβ38Al1605073040#ms(>200ns)0189Gu03Iβ38Si407014090#ms(>1s)0+0191Zh24Iβ;βn38P14760100640ms1400195Re.
ADβ=100;βn=12538S268617170.
3m0.
70+01β=10038Cl29798.
100.
1037.
24m0.
05201β=10038Clm29126.
740.
10671.
3610.
008715ms3501IT=10038Ar34714.
60.
3STABLE0+01IS=0.
0632538K28800.
70.
47.
636m0.
0183+01β+=10038Km28670.
20.
4130.
500.
28RQ923.
9ms0.
60+01β+=10038Kn25342.
70.
43458.
00.
221.
98s0.
11(7+),(5+)01IT=10038Ca220595440ms80+01β+=10038Sc4940#300#200ns)3/2+#0189Gu03Iβ39Si193034090#ms(>1s)7/2#0190Au.
AIβ39P12870100190ms501/2+#0195Re.
ATDβ=100;βn=26839S231605011.
5s0.
5(3,5,7)/201β=10039Cl29800.
21.
755.
6m0.
23/2+01β=10039Ar332425269y37/201β=10039K33807.
010.
19STABLE3/2+01IS=93.
25814439Ca27274.
41.
9859.
6ms1.
43/2+01β+=10039Sc1416824260ns)0297Sa14Iβ;βn40Si547056020#ms(>200ns)0+0289Gu03Iβ;βn40P8110140153ms8(2,3)02β=100;40S228701408.
8s2.
20+02β=10040Cl27560301.
35m0.
02202β=10040Ar35039.
89600.
0027STABLE0+02IS=99.
60033040K33535.
200.
191.
251Gy0.
011402IS=0.
01171;40Km31891.
560.
191643.
6390.
011336ns120+02IT=10040Ca34846.
270.
21STABLE(>5.
9Zy)0+0199Be64TIS=96.
941156;2β+40Sc20523.
22.
8182.
3ms0.
7402β+=100;40Ti885016053.
3ms1.
50+02β+=100;β+p=10040V10330#500#2#p40MgI:oneeventexpected,noneobserved;similarsearchin02Le.
A40AlI:34eventsreportedin97Sa14;alsooneeventin96Sa3440PDβn=15.
82140KDβ=89.
2813;β+=10.
721340ScDβ+p=0.
447;β+α=0.
017541Al35700#800#2#ms(>260ns)3/2+#0297Sa14Iβ41Si13560184030#ms(>200ns)7/2#0289Gu03Iβ41P5280220150ms151/2+#02β=100;βn=301041S190201201.
99s0.
057/2#02β=100;βn41Cl273107038.
4s0.
8(1/2,3/2+)02β=10041Ar33067.
50.
3109.
61m0.
047/202β=10041K35559.
070.
19STABLE3/2+02IS=6.
73024441Ca35137.
760.
24102ky77/202ε=10041Sc28642.
390.
23596.
3ms1.
77/202β+=10041Scr25760.
100.
232882.
300.
05RQ7/2+02P=592;IT=41241Ti15700#100#80.
9ms1.
23/2+0298Bh12Tβ+=100;β+p≈10041V210#210#7/2#p41AlI:reported4events41TiT:average98Bh12=81.
3(2.
0)98Li46=82(3)96Fa09=81(4)74Se11=80(2)42Al43680#900#1#msβ;βn42Si18430#500#5#ms(>200ns)0+0190Le03Iβ;βn42P940450120ms300189Le16Tβ=100;βn=502042S176801201.
013s0.
0150+01β=100;βn260ns)3/2#02No11Iβ;βn43P577097033ms31/2+#01β=100;βn=10043S11970200260ms153/2#0198Wi.
ATβ=100;βn=401043Sm116502003195480ns50(7/2)0100Sa21EJIT=10043Cl241701603.
07s0.
073/2+#01β=100;βn43Ar3201055.
37m0.
06(5/2)01β=10043K36593922.
3h0.
13/2+01β=10043Ca38408.
60.
3STABLE7/201IS=0.
13510.
.
.
A-groupiscontinuedonnextpage.
.
.
36G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
43Sc36187.
91.
93.
891h0.
0127/201β+=10043Scm36036.
51.
9151.
40.
2438s73/2+01IT=10043Ti293217509ms57/201β+=10043Tim290087313.
01.
012.
6s0.
6(3/2+)01IT=10043Tin2625573066.
41.
0560ns6(19/2)01IT=10043V18020#230#80#ms7/2#01β+43Cr2130#220#21.
6ms0.
7(3/2+)01β+=100;β+p=236;43SmJ:fromcomparisonofB(E2)andhalf-lifewiththeoreticalones43VT:>800msreportedby92Bo37andadoptedinENSDF'01.
Tobeconrmed.
43CrDβ+2p=65;β+α44Si32840#800#10#ms0+β;βn44P12100#700#30#ms(>200ns)9989Gu03Iβ44S9120390123ms100+99β=100;βn=18344Cl20230110560ms11099β=100;βn200ns)1/2+#9390Le03Iβ45S3250174082ms133/2#97β=100;βn=5445Cl18360120400ms403/2+#95β=100;βn=24445Ar29770.
60.
521.
48s0.
15(1,3,5)/295β=10045K366081017.
3m0.
63/2+95β=10045Ca40812.
00.
4162.
67d0.
257/29594Lo04Tβ=10045Sc41067.
80.
8STABLE7/295IS=100.
45Scm41055.
40.
812.
400.
05318ms73/2+95IT=10045Ti39005.
71.
0184.
8m0.
57/295β+=10045V3188017547ms67/295β+=10045Cr1897050050ms67/2#95β+=100;β+p>2745Crm18920#510#50#100#1#ms3/2+#IT;β+45Mn5110#300#200ns)0090Le03Iβ46S700#700#30#ms(>200ns)0+0089Gu03Iβ46Cl14710720220ms4000β=100;βn=60946Ar29720408.
4s0.
60+00β=10046K3541816105s102()0082To02Jβ=10046Ca43135.
12.
3STABLE(>100Ey)0+0099Be64TIS=0.
0043;2β46Sc41757.
10.
883.
79d0.
044+00β=10046Scm41614.
60.
8142.
5280.
00718.
75s0.
04100IT=10046Ti44123.
40.
8STABLE0+00IS=8.
25346V37073.
01.
0422.
50ms0.
110+00β+=10046Vm36271.
51.
0801.
460.
101.
02ms0.
073+00IT=100.
.
.
A-groupiscontinuedonnextpage.
.
.
G.
Audietal.
/NuclearPhysicsA729(2003)3–12837NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
46Cr2947420260ms600+00β+=10046Mn12370#110#37ms3(4+)0092Bo37TDβ+=100;β+p=222;46Mnm12220#150#150#100#1#ms1#β+46Fe760#350#9ms40+0001Gi01TDβ+=100;β+p=362046CaT:limitisforneutrinolessββdecay46MnDβ+2p≈18;β+α46MnT:average92Bo37=41(+7–6)01Gi01=34.
0(+4.
5–3.
5)46MnD:β+2p≈18%estimatedfromPp=β+p+2*β+2p=58(9)%in01Gi0147S8000#800#20#ms(>200ns)3/2#9589Gu03Iβ47Cl10520#600#200#ms(>200ns)3/2+#9589Gu03Iβ=100;βn200ns)0+90Le03Iβ48Cl4700#700#100#ms(>200ns)89Gu03Iβ48Ar23720#300#500#ms0+β48K32124246.
8s0.
2(2)95β=100;βn=1.
141548Ca44214453Ey170+9500Br63TIS=0.
18721;48Sc44496543.
67h0.
096+95β=10048Ti48487.
70.
8STABLE0+95IS=73.
72348V44475.
42.
615.
9735d0.
00254+95β+=10048Cr42819721.
56h0.
030+95β+=10048Mn29320110158.
1ms2.
24+9787Se07Dβ+=100;β+p=0.
284;48Fe18160#70#44ms70+9596Fa09TDβ+=100;β+p=3.
61148Co1640#400#6+#p48Ni18400#500#10#ms(>500ns)0+0100Bl01I2p48CaD2β=;β48CaT:average00Br63=42(33-13)96Ba80=43(+24–11statistics+14systematics)48CaT:alsoT>36Eyfrom70Ba61.
Singleβdecay:T>6Ey(95%CL),from85Al1748MnDβ+α=6e–448MnD:oneβ+αeventwasobserved,versus437β+p,ing.
4of87Se0749S22000#950#200ns)3/2+#9589Gu03Iβ49Ar18150#500#170ms503/2#9503We09TDβ=100;βn=652049K30320701.
26s0.
05(3/2+)95β=100;βn=86949Ca4128948.
718m0.
0063/295β=10049Sc46552457.
2m0.
27/295β=10049Ti48558.
80.
8STABLE7/295IS=5.
41249V47956.
91.
2330d157/295ε=10049Cr45330.
52.
442.
3m0.
15/295β+=10049Mn3761624382ms75/201β+=10049Fe24580#150#70ms3(7/2)0196Fa09Jβ+=100;β+p=521049Co9580#260#97.
5;β1.
3Ey)0+9503Bi05TIS=4.
34513;2β+50Mn42626.
81.
0283.
9ms0.
50+95β+=10050Mnm42398722971.
75m0.
035+95β+=10050Fe3448060155ms110+01β+=100;β+p≈050Co17200#170#44ms4(6+)0196Fa09JDβ+=100;β+p=541250Ni3790#260#9.
1ms1.
80+9701Ma.
ATβ+50VDβ=171151Cl13500#1000#2#ms(>200ns)3/2+#9790Le03Iβ51Ar7800#700#60#ms(>200ns)3/2#9789Gu03Iβ51K22000#500#365ms53/2+#97β=100;βn=47551Ca358609010.
0s0.
83/2#97β=100;βn51Sc432182012.
4s0.
1(7/2)97β=10051Ti49727.
81.
05.
76m0.
013/297β=10051V52201.
41.
0STABLE7/297IS=99.
750451Cr51448.
81.
027.
7025d0.
00247/297ε=10051Mn48241.
31.
046.
2m0.
15/297β+=10051Fe4022215305ms55/297β+=10051Co27270#150#60#ms(>200ns)7/2#9787Po04Iβ+51Ni11440#260#30#ms(>200ns)7/2#9787Po04Iβ+52Ar3000#900#10#ms0+00β52K16200#700#105ms52#00ABBWDβ=100;βn≈64;52Ca325107004.
6s0.
30+00β=100;βn3053Sc37620#300#>3s7/2#9998So03TDβ=100;βn53Ti4683010032.
7s0.
9(3/2)99β=10053V5184931.
60m0.
047/299β=10053Cr55284.
70.
8STABLE3/299IS=9.
5011753Mn54687.
90.
83.
7My0.
47/299ε=10053Fe50945.
31.
88.
51m0.
027/299β+=10053Fem47904.
91.
83040.
40.
32.
526m0.
02419/29997Ge11TIT=10053Co4264518242ms87/2#9902Lo13Tβ+=10053Com3944722319729p247ms12(19/2)99β+≈98.
5;p≈1.
553Ni29370#160#45ms157/2#9976Vi02Dβ+=100;β+p≈4553Cu13460#260#300ns)0+0197Be70Iβ;βn54Sc34220370260ms303+#0102Ja16Tβ=100;βn54Scm3411037011037s5(5+)0198Gr14EJIT=10054Ti455901201.
5s0.
40+01β=10054V498911549.
8s0.
53+01β=10054Vm49783151083900ns500(5+)98Gr14EJIT=10054Cr56932.
50.
8STABLE0+01IS=2.
365754Mn55555.
41.
3312.
03d0.
033+0102Un02Tε=100;β300ns)5/2#97Be70Iβ55Sc29580740120ms407/2#01β=100;βn55Ti41670150490ms903/2#0198Am04Tβ=10055V491501006.
54s0.
157/2#01β=10055Cr55107.
50.
83.
497m0.
0033/201β=10055Mn57710.
60.
7STABLE5/201IS=100.
55Fe57479.
40.
72.
737y0.
0113/201ε=10055Co54027.
60.
717.
53h0.
037/201β+=10055Ni4533611204.
7ms1.
77/20102Lo13Tβ+=10055Cu31620#300#40#ms(>200ns)3/2#0187Po04Iβ+;p55Zn14920#250#20#ms(>1.
6s)5/2#0101Gi10Iβ+55TiT:unweighedaverage98Am04=320(60)96Do23=600(40)and95So.
A=545(95)55TiT:(BirgeratioB=2.
75)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)supersededby99Re0640G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)56Ca13440#900#10#ms(>300ns)0+9997Be70Iβ56Sc25270#700#80#ms(>300ns)3+#9997Be70Iβ56Ti38940200164ms240+9998Am04TDβ=100;βn56V46080200216ms4(1+)9903Ma02TJβ=100;βn56Cr55281.
21.
95.
94m0.
100+99β=10056Mn56909.
70.
72.
5789h0.
00013+99β=10056Fe60605.
40.
7STABLE0+99IS=91.
7543656Co56039.
42.
177.
23d0.
034+99β+=10056Ni53904116.
075d0.
0100+99β+=10056Cu38600#140#93ms3(4+)9901Bo54TJDβ+=100;β+p=0.
401256Zn25730#260#36ms100+0195Wa.
ATβ+;β+p56Ga4740#260#3+#p56TiT:average98Am04=190(40)96Do23=150(30)56ZnT:half-lifeisderivedfromexperimental(p,n)crosssections56ZnI:identiedbytime-of-ight01Gi10withT>1.
6s57Ca7120#1000#5#ms5/2#β;βn57Sc20690#700#13ms47/2#9802So.
ATDβ=100;βn=33#57Ti3354046060ms165/2#9899So20Tβ=100;βn=0.
3#57V44190230350ms10(3/2)9803Ma02TJβ=100;βn=0.
4#57Cr52524.
11.
921.
1s1.
0(3/2)98β=10057Mn57486.
81.
885.
4s1.
85/298β=10057Fe60180.
10.
7STABLE1/298IS=2.
1191057Co59344.
20.
7271.
74d0.
067/298ε=10057Ni56082.
01.
835.
60h0.
063/298β+=10057Cu4731016196.
3ms0.
73/298β+=10057Zn32800#100#38ms47/2#9802Lo13Tβ+=100;β+p≈6557Ga15900#260#1/2#p57TiT:average99So20=67(25)96Do23=56(20);98Am04=180(30)atvariancenotused57ZnT:average02Lo13=37(5)76Vi02=40(10)58Sc15170#800#12ms53+#02So.
ATDβ=10058Ti30770#700#54ms70+9799So20TDβ=10058V40210250191ms83+#9703Ma02TDβ=100;βn58Cr518302007.
0s0.
30+97β=10058Mn55910303.
0s0.
11+97β=10058Mnm558403071.
780.
0565.
2s0.
5(4)+97β=;IT=20#58Fe62153.
40.
7STABLE0+97IS=0.
282458Co59845.
91.
270.
86d0.
062+00β+=10058Com59821.
01.
224.
950.
069.
04h0.
115+00IT=10058Con59792.
81.
253.
150.
0710.
4s0.
34+00IT=10058Ni60227.
70.
6STABLE(>700Ey)0+01IS=68.
076989;2β+58Cu51662.
11.
63.
204s0.
0071+01β+=10058Zn423005084ms90+9902Lo13Tβ+=100;β+p400Eyto2+levelof58Fe,>700Eytoground-state58ZnT:average02Lo13=83(10)98Jo18=86(18)G.
Audietal.
/NuclearPhysicsA729(2003)3–12841NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)59Sc10040#900#10#ms7/2#β;βn59Ti25220#700#30ms35/2#0202So.
ATβ=10059V3707031075ms77/2#02β=100;βn59Cr47890240460ms505/2#02β=10059Crm47390240503.
01.
796s20(9/2+)02IT=10059Mn55480304.
59s0.
05(5/2)02β=10059Fe60663.
10.
744.
495d0.
0093/202β=10059Co62228.
40.
6STABLE7/202IS=100.
59Ni61155.
70.
6101ky133/20294Ru19Tβ+=10059Cu56357.
20.
881.
5s0.
53/202β+=10059Zn4726040182.
0ms1.
83/202β+=100;β+p=0.
10359Ga34120#170#3/2#p59Ge17000#280#7/2#2p59TiT:supersedes99So20=58(17)samegroup59NiT:unweighedaverage94Ru19=108(13)94Ru19(meteorite)=120(22)81Ni08=76(5)59NiT:(BirgeratioB=2.
05)60Sc4000#900#3#ms3+#β60Ti21650#800#22ms20+02So.
ATDβ=10060V32580470122ms183+#9799So20TDβ=100;βn60Vm32580#490#0#150#40ms151+#03So02TDβ=;IT60Vn324804701011(>400ns)99So20EIIT=10060Cr46500210560ms600+9396Do23Tβ=10060Mn531809051s60+94β=10060Mnm5291090271.
900.
101.
77s0.
023+9492Sc.
AEβ=88.
58;IT=11.
5860Fe6141231.
5My0.
30+93β=10060Co61649.
00.
65.
2713y0.
00085+00β=10060Com61590.
40.
658.
590.
0110.
467m0.
0062+00IT≈100;β=0.
24360Ni64472.
10.
6STABLE0+96IS=26.
22317760Cu58344.
11.
723.
7m0.
42+93β+=10060Zn54188112.
38m0.
050+02β+=10060Ga40000#110#70ms10(2+)0201Ma96TJβ+=100;β+p=1.
67;60Ge27770#230#30#ms0+β+60As6400#600#5+#p60Asm6340#600#60#20#2+#p60VT:also98Am04=200(40),notused60CrT:weighedaverage96Do23=510(150)88Bo06=570(60);other95Am.
A=380(30)60GaDβ+α300ns)1/2#9997Be70Iβ;βn61V29360#400#47.
0ms1.
27/2#9903So02TDβ=100;βn99;IT300ns)9797Be70Iβ64Cr33150#400#43ms10+02So.
ATDβ=10064Mn4262027088.
8ms2.
5(1+)9699So20TJDβ=100;βn=64Mnm424902701353>100s98Gr14ETIT=10064Fe547702802.
0s0.
20+96β=10064Co5979320300ms301+96β=10064Ni67099.
30.
6STABLE0+96IS=0.
9256964Cu65424.
20.
612.
700h0.
0021+96β+=61.
03;β=39.
0364Zn66003.
60.
7STABLE(>2.
3Ey)0+9685No03TIS=48.
6360;2β+64Ga58834.
32.
02.
627m0.
0120(+#)96β+=10064Gam58791.
52.
042.
850.
0821.
9s0.
72+9699Ta29TJIT=10064Ge543503063.
7s2.
50+96β+=10064As39520#360#40ms300+#02Lo13TDβ+=10064CrT:also99So20=44(12)outweighed,notused64MnT:average02So.
A=91(4)99So20=85(5)99Ha05=89(4);98Am04=140(30)notusedG.
Audietal.
/NuclearPhysicsA729(2003)3–12843NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)65V11250#800#10#ms5/2#β;βn65Cr27800#500#27ms31/2#9702So.
ATDβ=100;βn65Mn4067054092ms15/2#9302So.
ATDβ=100;βn=65Fe508802401.
3s0.
31/2#9399So20Tβ=10065Fem505202403643430ns130(5/2)98Gr14ETJIT=10065Co59170131.
20s0.
06(7/2)93β=10065Ni65126.
10.
62.
5172h0.
00035/297β=10065Nim64113.
11.
21013126.
7ns1.
09/2+95Bl01ETJ65Cu67263.
70.
7STABLE3/293IS=30.
83365Zn65911.
60.
7244.
06d0.
105/200β+=10065Znm65857.
70.
753.
9280.
0101.
6s0.
6(1/2)00IT=10065Ga62657.
20.
815.
2m0.
23/293β+=10065Ge5641010030.
9s0.
5(3/2)9387Vi01Dβ+=100;β+p=0.
011365As46980#300#170ms303/2#9302Lo13Tβ+=10065Se32920#600#100s(8)98Gr14ETJIT=10066Ni66006.
31.
454.
6h0.
40+98β=10066Cu66258.
30.
75.
120m0.
0141+98β=10066Zn68899.
40.
9STABLE0+98IS=27.
902766Ga6372439.
49h0.
070+98β+=10066Ge61620302.
26h0.
050+98β+=10066As5150068095.
77ms0.
23(0+)9898Gr12Jβ+=10066Asm501406801356.
700.
171.
1s0.
1(5+)01Gr07TJIT=10066Asn484806803023.
90.
38.
2s0.
5(9+)01Gr07TJIT=10066Se41720#300#33ms120+9802Lo13TDβ+=10066MnT:average02So.
A=64(2)99Ha05=66(4)66MnT:also99So20=62(14)98Am04=90(20)outweighed,notused66FeT:average99So20=440(60)98Am04=440(60)66CoT:average00Mu10=180(10)94Cz02=240(30)85Bo49=230(20)66AsmJ:3+#fromsystematics66AsnT:supersedes98Gr12=17.
5(1.
5)E:from98Gr1267Cr19050#700#10#ms(>300ns)1/2#97Be70Iβ67Mn33400#500#45ms35/2#9702So.
ATDβ=100;βn=67Fe45690420394ms91/2#9102So.
ATDβ=100;βn67Fem45320420367364s17(5/2)03Sa02ETIT=10067Co55060320425ms207/2#9199We07Tβ=10067Ni63742.
72.
921s11/20100Ri14Jβ=10067Nim6273641007313.
3s0.
29/2+0198Gr14EIT=10067Cu67318.
81.
261.
83h0.
123/291β=10067Zn67880.
40.
9STABLE5/291IS=4.
101367Ga66879.
71.
33.
2612d0.
00063/296ε=10067Ge62658518.
9m0.
31/291β+=10067Gem62640518.
20.
0513.
7s0.
95/291IT=10067Gen619065751.
700.
06110.
9ns1.
491IT=10067As5665010042.
5s1.
2(5/2)91β+=100.
.
.
A-groupiscontinuedonnextpage.
.
.
44G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
67Se46490#200#133ms115/2#9795Bl23TDβ+=100;β+p=0.
5167Br32800#500#1/2#p67MnT:average02So.
A=47(4)99Ha05=42(4)67FeT:others99So20=500(100)98Am04=470(50)outweighed,notused67FemT:average03Sa02=75(21)98Gr14=43(30),sameauthors,differentexperiment67CoT:others99Pr10=440(70)99So20=440(80)85Bo49=420(70)outweighed,notused67CoT:and95Am.
A=310(20)atvariance,notused67SeT:average02Lo13=136(12)94Ba50=107(35)67SeT:valuesfrom95Bl23for67Se=60(+17–11)and71Krquestionedby97Oi0168Mn28600#600#28ms40202So.
ATβ=100;βn=68Fe43130700187ms60+0202So.
ATβ=100;βn68Co51350320200ms21(7)0200Mu10Tβ=10068Com51200#350#150#150#1.
6s0.
3(3+)0200Mu10JDβ=;IT68Ni63463.
83.
029s20+02β=10068Nim6169431770.
01.
0276ns650+02IT=10068Nin6061532849.
10.
3860s50502IT=10068Cu65567.
01.
631.
1s1.
51+02β=10068Cum64845.
41.
7721.
60.
73.
75m0.
05(6)02IT=841;β=16168Zn70007.
21.
0STABLE0+02IS=18.
755168Ga67086.
11.
567.
71m0.
091+02β+=10068Gam65856.
21.
51229.
870.
0462.
0ns1.
4702IT=10068Ge669806270.
95d0.
160+02ε=10068As5890040151.
6s0.
83+02β+=10068Asm5847040425.
210.
16111s201+02IT=10068Se542103035.
5s0.
70+02β+=10068Br38640#360#500TyinENSDFisfor0ν-2βdecayalone70BrmE:from2002Je0771Fe31000#800#30#ms(>300ns)7/2+#9797Be70Iβ71Co4387084097ms27/2#9302So.
ATβ=100;βn71Ni552003702.
56s0.
031/2#9398Fr15Tβ=10071Cu62711.
11.
519.
4s1.
4(3/2)9399Pr10Tβ=10071Cum5995510275610271ns13(19/2)98Gr14ETJIT=10071Zn67327102.
45m0.
101/293β=10071Znm6716910157.
71.
33.
96h0.
059/2+93β≈100;IT≤0.
0571Ga70140.
21.
0STABLE3/293IS=39.
892971Ge69907.
71.
011.
43d0.
031/293ε=10071Gem69709.
31.
0198.
3670.
01020.
40ms0.
179/2+93IT=10071As67894465.
28h0.
155/293β+=10071Se63120304.
74m0.
055/293β+=10071Sem630703048.
790.
055.
6s0.
71/2to9/293IT=10071Sen6286030260.
480.
1019.
0s0.
5(9/2)+9300Ch07TIT=10071Br5706057021.
4s0.
6(5/2)93β+=10071Kr46920650100ms3(5/2)9797Oi01TJDβ+=100;β+p=2.
1771Rb32300#500#5/2#p71Rbm32250#510#50#100#1/2#71Rbn32040#510#260#100#9/2+#71CoT:othernotused:98Am04=210(40)71CuT:average99Pr10=19(3)83Ru06=19.
5(1.
6)71CumT:average98Is11=250(30)98Gr14=275(14)71KrT:average97Oi01=100(3)81Ew01=97(9);95Bl23=64(+8–5)atvariancenotused71KrT:valuesfrom95Bl23for67Seand71Krquestionedby97Oi0171KrD:95Bl23=5.
2(0.
6)atvariancenotused46G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)72Fe28300#800#10#ms(>300ns)0+9797Be70Iβ72Co39300#600#90ms2098Am04TDβ=100;βn72Ni539404401.
57s0.
050+98Fr15TDβ=100;βn72Cu59783.
01.
46.
6s0.
1(1+)95β=10072Cum59513327031.
76s0.
03(4)98Gr14ETJIT=10072Zn68131646.
5h0.
10+95β=10072Ga68589.
41.
014.
10h0.
02395β=10072Gam68469.
71.
0119.
660.
0539.
68ms0.
13(0+)95IT=10072Ge72585.
91.
6STABLE0+95IS=27.
543472Gem71894.
51.
6691.
430.
04444.
2ns0.
80+72As68230426.
0h0.
1295β+=10072Se67894128.
40d0.
080+97ε=10072Br590206078.
6s2.
41+9503Pi03Jβ+=10072Brm5892060100.
920.
0310.
6s0.
3195IT≈100;β+=72Kr53941817.
16s0.
180+9503Pi03Tβ+=10072Rb38120#500#300ns)7/2#0297Be70Iβ73Ni49860#300#840ms30(9/2+)02β=100;βn73Cu5898744.
2s0.
3(3/2)0298Fr15Jβ=100;βn73Zn654104023.
5s1.
0(1/2)02β=10073Znm6521040195.
50.
213.
0ms0.
2(5/2+)02IT=10073Znn6517040237.
62.
0EU5.
8s0.
8(7/2+)02IT=;β=73Ga69699.
31.
74.
86h0.
033/202β=10073Ge71297.
51.
6STABLE9/2+02IS=7.
73573Gem71284.
21.
613.
28450.
00152.
92s0.
035/2+02IT=10073Gen71230.
81.
666.
7260.
009499ms111/202IT=10073As70957480.
30d0.
063/293ε=10073Se68218117.
15h0.
089/2+03β+=10073Sem681921125.
710.
0439.
8m1.
33/203IT=72.
63;β+=27.
4373Br63630503.
4m0.
21/202β+=10073Kr56552728.
6s0.
63/20299Mi17Tβ+=100;β+p=0.
25373Krm561187433.
660.
12107ns10(9/2+)03IT=10073Rb46050#150#25ms1/2#03β+=100;β+p=73ZnnE:if42.
1keVγfeeds73Znm,EU:seediscussioninENSDF'0273KrT:average99Mi17=29.
0(1.
0)81Ha44=28.
4(0.
7);73Da22=25.
9(0.
6)atvariance,73KrT:notused74Co32250#800#50#ms(>300ns)0397Be70Iβ74Ni48370#400#680ms1200+0398Fr15Tβ=100;βn74Cu5600661.
594s0.
0101+#95β=10074Zn657105095.
6s1.
20+95β=10074Ga6805048.
12m0.
12(3)95β=10074Gam67990459.
5710.
0149.
5s1.
0(0)95IT=;β=25#74Ge73422.
41.
6STABLE0+95IS=36.
287374As70860.
02.
317.
77d0.
02295β+=662;β=34274Se72212.
71.
7STABLE0+95IS=0.
894;2β+74Br653061525.
4m0.
3(0)95β+=10074Brm652921513.
580.
2146m24(+#)95β+=10074Kr62331.
52.
011.
50m0.
110+95β+=10074Krm61824105081029ns60+00Ch07ETJIT=10074Rb51917464.
76ms0.
03(0+)9501Ba12Tβ+=10074Sr40700#500#50#ms(>1.
5s)0+9795Bl06Iβ+74NiT:average98Fr15=900(200)98Am04=540(160)G.
Audietal.
/NuclearPhysicsA729(2003)3–12847NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)75Co29500#800#40#ms(>300ns)7/2#9997Be70Iβ75Ni43900#400#600ms2007/2+#9985Re01Dβ=100;βn=1.
6#75Cu541209801.
224s0.
0033/2#99β=100;βn=3.
5675Zn624707010.
2s0.
27/2+#99β=10075Ga68464.
62.
4126s2(3/2)99β=10075Ge71856.
41.
682.
78m0.
041/299β=10075Gem71716.
71.
6139.
690.
0347.
7s0.
57/2+99IT≈100;β=0.
030675As73032.
41.
8STABLE3/299IS=100.
75Asm72728.
51.
8303.
92410.
000717.
62ms0.
239/2+99IT=10075Se72169.
01.
7119.
779d0.
0045/2+99ε=10075Br691391496.
7m1.
33/299β+=10075Kr6432484.
29m0.
175/2+99β+=10075Rb57222719.
0s1.
2(3/2)99β+=10075Sr4662022088ms3(3/2)9903Hu01TJDβ+=100;β+p=5.
2975NiD:βn=1.
6%#estimatedby85Re0176Ni41610#900#470ms3900+9798Am04Tβ=100;βn76Cu509767641ms6(3,5)9590Wi12Jβ=100;βn=3276Cum50980#200#0#200#1.
27s0.
30(1,3)9590Wi12Jβ=10076Zn62140805.
7s0.
30+95β=10076Ga66296.
62.
032.
6s0.
6(2+,3+)95β=10076Ge73213.
01.
71.
58Zy0.
170+9501Kl11TIS=7.
6138;2β=10076As72289.
51.
81.
0778d0.
0020295β≈100;ε99.
4;β+170ns)00We.
AIβ+;p76GeT: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=15Yynottrusted.
Seealso02Aa.
1and02Zd0276YI:also01Ki13>200ns,samegroup77Ni36750#500#300#ms(>300ns)9/2+#9797Be70Iβ77Cu48580#400#469ms83/2#97β=10077Zn587201202.
08s0.
057/2+#97β=10077Znm57950120772.
390.
121.
05s0.
101/2#97IT>50;β300ns)0+9797Be70Iβ78Cu44750#400#342ms119791Kr15Tβ=10078Zn57340901.
47s0.
150+91β=10078Znm546709026731319ns9(8+)00Da07ETIT=10078Ga63706.
62.
45.
09s0.
05(3+)91β=10078Ge71862488m10+91β=10078As728171090.
7m0.
2291β=10078Se77026.
11.
7STABLE0+91IS=23.
772878Br7345246.
46m0.
041+91β+≈100;β110Ey)0+9194Sa31TIS=0.
351;2β+78Rb66936717.
66m0.
080(+)91β+=10078Rbm668257111.
200.
105.
74m0.
054()9191Mc.
AEβ+=902;IT=10278Rbx66862147412R=2.
00.
5spmix78Sr631747159s80+9192Gr09Tβ+=10078Y52530#400#54ms5(0+)9701Ga24TJDβ+=100;β+p78Ym52530#640#0#500#5.
8s0.
55+#01Ki13TDβ+=100;β+p78Zr41700#500#50#ms(>170ns)0+00We.
AIβ+;β+p78BrD:βbranchisuncertain.
SeeENSDF78KrT:limitgivenhereisfortheK-e+decay(theoreticallyfaster)78YT:average01Ga24=50(8)01Ki13=55(+9–6)78YmT:average01Ki13=5.
7(0.
7)98Uu01=5.
8(0.
6)78ZrI:also01Ki13>200nssamegroup79Cu42330#500#188ms253/2#02β=100;βn=551779Zn53420#260#995ms19(9/2+)02β=100;βn=1.
3479Ga625101002.
847s0.
0033/2#02β=100;βn=0.
0891979Ge694909018.
98s0.
03(1/2)02β=10079Gem6930090185.
950.
0439.
0s1.
07/2+#02β=961;IT=4179As7363769.
01m0.
153/202β=10079Asm728646772.
810.
061.
21s0.
01(9/2)+0298Gr14TIT=10079Se75917.
61.
7295ky387/2+02β=10079Sem75821.
81.
795.
770.
033.
92m0.
011/202IT≈100;β=0.
0561179Br76068.
52.
0STABLE3/202IS=50.
69779Brm75860.
92.
0207.
610.
094.
86s0.
04(9/2+)02IT=10079Kr74443435.
04h0.
101/202β+=10079Krm743134129.
770.
0550s37/2+02IT=10079Krn742964147.
060.
0678.
7ns1.
0(5/2)02IT=10079Rb70803622.
9m0.
55/2+02β+=10079Sr6547782.
25m0.
103/2()02β+=10079Y5836045014.
8s0.
65/2+#02β+=100;β+p79Zr47360#400#56ms305/2+#02β+=100;β+p79AsmT:98Ho15=0.
87(0.
06)outweighed,notused80Cu36450#600#100#ms(>300ns)9797Be70Iβ80Zn51840170545ms160+92β=100;βn=1.
0580Ga591401201.
697s0.
011(3)9293Ru01Dβ=100;βn=0.
89680Ge695152829.
5s0.
40+92β=10080As721592315.
2s0.
21+92β=10080Se77759.
92.
0STABLE0+92IS=49.
6141;2β80Br75889.
52.
017.
68m0.
021+92β=91.
72;β+=8.
3280Brm75803.
72.
085.
8430.
0044.
4205h0.
0008592IT=10080Kr77892.
51.
5STABLE0+92IS=2.
28680Rb72173733.
4s0.
71+9293Al03Tβ+=10080Rbm716797494.
40.
51.
6s0.
026+92Do10E80Sr703087106.
3m1.
50+99β+=10080Y6122018030.
1s0.
549298Do04TJβ+=10080Ym60990180228.
50.
14.
8s0.
3(1)98Do04ETJIT=812;β+=19280Yn60910180312.
51.
04.
7s0.
3(2+)00Ch07ETJIT=100.
.
.
A-groupiscontinuedonnextpage.
.
.
G.
Audietal.
/NuclearPhysicsA729(2003)3–12849NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
80Zr5552014904.
6s0.
60+9201Ki13Tβ+=100;β+p80YT:differenceswith82De36=38(1)81Li12=33.
8(0.
6)explainedin98Do0480YmT:average01No07=5.
0(0.
5)98Do04=4.
7(0.
3)D:from98Do0480YnE:00Ch07=84(1)above228.
5level80ZrT:average01Ki13=5.
3(+1.
1–0.
9)00Re03=4.
1(+0.
8–0.
6)81Zn46130#300#290ms505/2+#97β=100;βn=7.
53081Ga579801901.
217s0.
005(5/2)97β=100;βn=11.
9781Ge663001208s29/2+#97β=10081Gem65620120679.
130.
048s2(1/2+)97β≈100;IT300ns)0+0397Be70Iβ82Ga53100#300#599ms2(1,2,3)0393Ru01Dβ=100;βn=21.
31382Ge656202404.
55s0.
050+03β=10082As7032020019.
1s0.
5(1+)03β=10082Asm7007525250200BD13.
6s0.
4(5)03β=10082Se77594.
02.
097Ey50+0399Pi08TIS=8.
7322;2β=10082Br77496.
51.
935.
282h0.
007503β=10082Brm77450.
61.
945.
94920.
00106.
13m0.
05203IT=97.
63;β=2.
4382Kr80589.
51.
8STABLE0+03IS=11.
581482Rb76188.
22.
81.
273m0.
0021+03β+=10082Rbm76119.
12.
469.
11.
5MD6.
472h0.
006503β+≈100;IT300ns)5/2+#0197Be70Iβ83Ga49390#300#308ms13/2#01β=100;βn=371783Ge60900#200#1.
85s0.
065/2+#01β=10083As6988022013.
4s0.
33/2#01β=10083Se75341422.
3m0.
39/2+01β=10083Sem751134228.
500.
2070.
1s0.
41/201β=10083Br7900942.
40h0.
023/201β=10083Brm7594043068.
80.
6700ns100(19/2)01IT=10083Kr79981.
72.
8STABLE9/2+01IS=11.
49683Krm79972.
32.
89.
40530.
0008154.
4ns1.
17/2+01IT=10083Krn79940.
12.
841.
55690.
00101.
83h0.
021/201IT=100.
.
.
A-groupiscontinuedonnextpage.
.
.
50G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
83Rb79075686.
2d0.
15/201ε=10083Rbm79033642.
110.
047.
8ms0.
79/2+0168Et01TIT=10083Sr767951032.
41h0.
037/2+01β+=10083Srm7653610259.
150.
094.
95s0.
121/201IT=10083Y72330407.
08m0.
069/2+0192Bu10Jβ+=10083Ym722704061.
980.
112.
85m0.
02(3/2)01β+=605;IT=40583Zr6646010041.
6s2.
41/2#01β+=100;β+p=83Zrm6641010052.
720.
05530ns0.
12(5/2)01IT=10083ZrnnonexistentRN8s1high0187Ra06Iβ+=100;β+p=83Nb589603104.
1s0.
3(5/2+)01β+=10083Mo47750#500#23ms193/2#0101Ki13TDβ+=100;β+p83ZrnD:6(4)%oftotalβ+pgotorstexcitedstatein82Sr83ZrnI:misassigned:absenceofradiationssuggestsnoisomerwithE>18keV84Ga44110#400#85ms1097β=100;βn=701584Ge58250#300#954ms140+9793Ru01Tβ=100;βn=10.
8684As66080#300#4.
02s0.
03(3)(+#)9793Ru01Tβ=100;βn=0.
28484Asm66080#320#0#100#650ms15097β=10084Se75952153.
1m0.
10+97β=10084Br777991531.
80m0.
08297β=10084Brm77460100340100BD6.
0m0.
2(6)97β=10084Brn7739115408.
20.
4300ns)3/2#9797Be70Iβ85Ge53070#400#540ms505/2+#97β=100;βn=14385As63320#200#2.
021s0.
0103/2#97β=100;βn=59.
42485Se724283031.
7s0.
95/2+#97β=10085Br78610192.
90m0.
063/291β=10085Kr81480.
31.
910.
776y0.
0039/2+9102Un02Tβ=10085Krm81175.
41.
9304.
8710.
0204.
480h0.
0081/291β=78.
64;IT=21.
4485Krn79488.
52.
31991.
81.
31.
6s0.
7(17/2+)91IT=10085Rb82167.
3310.
011STABLE5/291IS=72.
17285Sr81102.
62.
864.
853d0.
0089/2+9102Un02Tε=10085Srm80863.
92.
8238.
660.
0667.
63m0.
041/291IT=86.
64;β+=13.
4485Y77842192.
68h0.
05(1/2)94β+=10085Ym778221919.
80.
54.
86h0.
139/2+94β+≈100;IT885Nb6715022020.
9s0.
7(9/2+)91β+=10085Nbm66390220759.
01.
012s5(1/2)9198Oi.
AETJβ+=10085Mo59100#280#3.
2s0.
21/2#9797Hu15TDβ+=100;β+p=85Tc47670#400#300ns)0197Be70Iβ86Ge49840#500#300#ms(>300ns)0+0194Be24Iβ;βn86As59150#300#945ms801β=100;βn=33486Se705411615.
3s0.
90+01β=10086Br756401155.
1s0.
4(2)01β=10086Kr83265.
570.
10STABLE0+01IS=17.
3022;2β86Rb82747.
020.
2018.
642d0.
018201β≈100;ε=0.
0052586Rbm82190.
970.
27556.
050.
181.
017m0.
003601IT≈100;β300ns)5/2+#0297Be70Iβ;βn87As55980#300#610ms1203/2#0293Ru01Tβ=100;βn=15.
42287Se66580405.
50s0.
125/2+#02β=100;βn=0.
20487Br738571855.
65s0.
133/202β=100;βn=2.
60487Kr80709.
430.
2776.
3m0.
55/2+02β=10087Rb84597.
7950.
01249.
23Gy0.
223/20282Mi14TIS=27.
832;β=10087Sr84880.
41.
1STABLE9/2+02IS=7.
00187Srm84491.
91.
1388.
5330.
0032.
815h0.
0121/202IT≈100;ε=0.
30887Y83018.
71.
679.
8h0.
31/202β+=10087Ym82637.
91.
6380.
820.
0713.
37h0.
039/2+02IT=98.
4310;β+=1.
571087Zr7934881.
68h0.
01(9/2)+02β+=10087Zrm790128335.
840.
1914.
0s0.
2(1/2)02IT=10087Nb74180603.
75m0.
09(1/2)02β+=10087Nbm74180603.
840.
142.
6m0.
19/2+#02β+=10087Mo6769022014.
05s0.
237/2+#0297Hu07TDβ+=100;β+p=15587Tc59120#300#2.
18s0.
161/2#0200We.
ATDβ+=100;β+p87Tcm59100#310#20#60#2#s9/2+#β+;IT87Ru47340#600#50#ms(>1.
5s)1/2#0295Ry03Iβ+87AsT:unweighedaverage93Ru01=485(40)78Cr03=730(60)(BirgeratioB=3.
4)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+state52G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)88Ge40140#700#80#ms(>300ns)0+9797Be70Iβ88As51290#500#300#ms(>300ns)9794Be24Iβ;βn88Se63880501.
53s0.
060+97β=100;βn=0.
991088Br707304016.
36s0.
07(2,1+)9893Ru01Tβ=100;βn=6.
581888Brm7046040272.
70.
35.
4s0.
798IT=10088Kr79692132.
84h0.
030+88β=10088Rb82609.
000.
1617.
78m0.
11288β=10088Sr87921.
71.
1STABLE0+88IS=82.
58188Y84299.
11.
9106.
65d0.
04488β+=10088Ym83624.
61.
9674.
550.
0413.
9ms0.
2(8)+88IT=10088Yn83906.
21.
9392.
860.
09300s31+8888Zr836231083.
4d0.
30+88ε=10088Nb7607010014.
5m0.
1(8+)88β+=10088Nbm7603010040140BD7.
8m0.
1(4)88β+=10088Mo72700208.
0m0.
20+97β+=10088Tc62710#200#5.
8s0.
2(2,3)97β+=10088Tcm62710#360#0#300#6.
4s0.
8(6,7,8)97β+=10088Ru55650#400#1.
3s0.
30+9701Ki13TDβ+=100;β+p88BrT:average93Ru01=16.
34(0.
08)74Gr29=16.
5(0.
2)J:systematicsprefers(2)89Ge33690#900#50#ms(>300ns)3/2+#9897Be70Iβ89As47140#500#200#ms(>300ns)3/2#9894Be24Iβ89Se59200#300#410ms405/2+#98β=100;βn=7.
82589Br68570604.
40s0.
03(3/2,5/2)98β=100;βn=13.
8489Kr76730503.
15m0.
043/2(+#)9895Ke04Jβ=10089Rb81713515.
15m0.
123/298β=10089Sr86209.
11.
150.
53d0.
075/2+98β=10089Y87701.
72.
6STABLE1/298IS=100.
89Ym86792.
72.
6908.
970.
0315.
663s0.
0059/2+9894It.
ATIT=10089Zr84869478.
41h0.
129/2+98β+=10089Zrm842814587.
820.
104.
161m0.
0171/298IT=93.
7712;89Nb80650272.
03h0.
07(9/2+)98β+=10089Nbm80650#40#0#30#1.
10h0.
03(1/2)98β+=10089Mo75004152.
11m0.
10(9/2+)98β+=10089Mom7461715387.
50.
2190ms15(1/2)98IT=10089Tc67840#200#12.
8s0.
9(9/2+)98β+=10089Tcm67780#200#62.
60.
512.
9s0.
8(1/2)98β+≈100;IT1.
5s)7/2+#9895Ry03Iβ+89BrT:ENSDFaverages8values.
Also93Ru01=4.
348(0.
022)89ZrmDβ+=6.
231289RuT:average00We.
A=1.
45(0.
13)99Li33=1.
2(0.
2);samegroup01Ki13=1.
5(0.
2)89RhI:unobservedin00We.
A,atdetectionlimitG.
Audietal.
/NuclearPhysicsA729(2003)3–12853NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)90As41450#800#80#ms(>300ns)97Be70Iβ90Se55930#400#300#ms(>300ns)0+94Be24Iβ;βn90Br64620801.
910s0.
0109893Ru01Tβ=100;βn=25.
2990Kr749701932.
32s0.
090+98β=10090Rb793627158s5098β=10090Rbm792557106.
900.
03258s4398β=97.
44;IT=2.
6490Rbx79291147112R=21fsmix90Sr85941.
62.
928.
79y0.
060+98β=10090Y86487.
52.
664.
00h0.
21298β=10090Ym85805.
82.
6681.
670.
103.
19h0.
067+98IT≈100;β=0.
0018290Zr88767.
32.
4STABLE0+98IS=51.
454090Zrm86448.
32.
42319.
0000.
010809.
2ms2.
0598IT=10090Zrn85177.
92.
43589.
4190.
016131ns48+98IT=10090Nb82656514.
60h0.
058+98β+=10090Nbm825345122.
3700.
02263s26+98IT=10090Nbn825315124.
670.
2518.
81s0.
06498IT=10090Nbp824855171.
100.
10300ns)3/2#9997Be70Iβ91Se50340#500#270ms501/2+#99β=100;βn=211091Br6151070541ms53/2#99β=100;βn=20391Kr71310608.
57s0.
045/2(+)01β=10091Rb77745858.
4s0.
43/2()99β=10091Sr8364559.
63h0.
055/2+01β=10091Srx83599114711R=6mix91Y86345.
02.
958.
51d0.
061/299β=10091Ym85789.
42.
9555.
580.
0549.
71m0.
049/2+99IT>98.
5;β99;IT1.
5s)7/2+#9995Ry03Iβ+91NbmDe+=0.
0028254G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)92As30930#900#30#ms(>300ns)0197Be70Iβ92Se46650#600#100#ms(>300ns)0+0197Be70Iβ92Br5658050343ms15(2)01β=100;βn=33.
12592Kr68785121.
840s0.
0080+01β=100;βn=0.
03322592Rb7477264.
492s0.
020001β=100;βn=0.
0107592Sr8286832.
66h0.
040+03β=10092Y8481393.
54h0.
01201β=10092Zr88453.
92.
3STABLE0+01IS=17.
15892Nb86448.
32.
834.
7My2.
4(7)+01β+≈100;β190Ey)0+0197Ba35TIS=14.
8435;2β+92Mom8404542760.
460.
16190ns38+01IT=10092Tc78935264.
25m0.
15(8)+01β+=10092Tcm7866526270.
150.
111.
03s0.
07(4+)01IT=10092Ru74410#300#3.
65m0.
050+01β+=10092Rh63360#400#4.
3s1.
3(6+)0101Xu05TJDβ+=100;β+p=92Pd55500#500#1.
1s0.
30+0101Ki13TDβ+=100;β+p92MoT:T>190Ey(2σ)92RhT:unweighedaverage01Xu05=3.
0(0.
8)01Ki13=5.
6(0.
5)(BirgeratioB=2.
76)92RhJ:from97Ka07;01Xu05>493Se40720#800#50#ms(>300ns)1/2+#9797Be70Iβ93Br53050#300#102ms103/2#01β=100;βn=68793Kr640201001.
286s0.
0101/2+01β=100;βn=1.
951193Rb7261885.
84s0.
025/297β=100;βn=1.
39793Rbm723658253.
380.
0357s15(3/2,5/2)97IT=10093Sr8008587.
423m0.
0245/2+97β=10093Y842231110.
18h0.
081/297β=10093Ym8346411758.
7190.
021820ms407/2+97IT=10093Zr87117.
02.
31.
53My0.
105/2+97β=10093Nb87208.
32.
4STABLE9/2+97IS=100.
93Nbm87177.
52.
430.
770.
0216.
13y0.
141/297IT=10093Mo8680344.
0ky0.
85/2+97ε=10093Mom8437842424.
890.
036.
85h0.
0721/2+97IT≈100;β+=0.
12193Tc8360342.
75h0.
059/2+01β+=10093Tcm832114391.
840.
0843.
5m1.
01/201IT=76.
611;β+=23.
41193Tcn8141842185.
160.
1510.
2s0.
3(17/2)0193Ru772709059.
7s0.
6(9/2)+97β+=10093Rum7654090734.
400.
1010.
8s0.
3(1/2)9783Ay01Dβ+=78.
023;93Run75190902082.
60.
92.
20s0.
17(21/2)+97IT=10093Rh69170#400#13.
9s1.
69/2+#0101Ki13TDβ+=100;β+p93Pd59700#400#1.
07s0.
12(9/2+)0101Ki13TJDβ+=100;β+p=93Ag46780#600#5#ms(>1.
5s)9/2+#9795Ry03Ip;β+93RumDIT=22.
023;β+p=0.
027593PdT:average01Ki13=1000(200)01Xu05=1300(200)00Sc31=900(200)D:β+p=1.
7#93AgI:thefeweventsreportedin94He28arenottrustedbyNUBASE93AgT:estimatedhalf-lifeisforβ+decay;p-decaywouldbemuchshorterG.
Audietal.
/NuclearPhysicsA729(2003)3–12855NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)94Se36800#800#20#ms(>300ns)0+9797Be70Iβ94Br47800#400#70ms2092β=100;βn=701594Kr61140#300#210ms40+0103Be05TDβ=100;βn=1.
11794Rb6855382.
702s0.
0053()9293Ru01Dβ=100;βn=10.
012394Sr78840775.
3s0.
20+92β=10094Y82348718.
7m0.
1292β=10094Zr87266.
82.
4STABLE(>110Py)0+9299Ar25TIS=17.
3828;2β94Nb86364.
52.
420.
3ky1.
6(6)+92β=10094Nbm86323.
62.
440.
9020.
0126.
263m0.
0043+92IT=99.
506;β=0.
50694Mo88409.
71.
9STABLE0+97IS=9.
251294Tc841544293m17+92β+=10094Tcm84079475.
51.
952.
0m1.
0(2)+92β+≈100;IT300ns)3/2#9797Be70Iβ95Kr56040#400#114ms31/2(+)9503Be05TDβ=100;βn=2.
871895Rb6585421377.
5ms0.
85/295β=100;βn=8.
732095Sr75117723.
90s0.
141/2+94β=10095Y81207710.
3m0.
11/294β=10095Zr85657.
82.
464.
032d0.
0065/2+00β=10095Nb86781.
92.
034.
991d0.
0069/2+00β=10095Nbm86546.
22.
0235.
6900.
0203.
61d0.
031/200IT=94.
46;β=5.
6695Mo87707.
51.
9STABLE5/2+00IS=15.
921395Tc86017520.
0h0.
19/2+95β+=10095Tcm85978538.
890.
0561d21/295β+=96.
1232;IT=3.
883295Ru83450121.
643h0.
0145/2+94β+=10095Rh783401505.
02m0.
10(9/2)+94β+=10095Rhm77800150543.
30.
31.
96m0.
04(1/2)94IT=885;β+=12595Pd70150#400#10#s9/2+#9597Sc30TDβ+=10095Pdm682903001860#500#13.
3s0.
3(21/2+)95β+=;IT=5#95Ag60100#400#1.
74s0.
13(9/2+)9594Sc35TJDβ+=100;β+p=95Agm59760#400#344.
20.
3300ns)9797Be70Iβ96Kr53030#500#80ms70+9703Be05TDβ=100;βn=3.
7496Rb6122529203ms32+9593Ru01Dβ=100;βn=13.
4496Rbm61230#200#0#200#200#ms(>1ms)1(#)81Bo30JIβ;IT;βn96Sr72939271.
07s0.
010+93β=10096Y78347235.
34s0.
05093β=10096Ym7720621114030BD9.
6s0.
2(8)+93β=10096Zr85442.
82.
824Ey60+9899Ar25TIS=2.
809;2β=10096Nb85604423.
35h0.
056+93β=10096Mo88790.
51.
9STABLE0+93IS=16.
68296Tc8581754.
28d0.
077+93β+=10096Tcm85783534.
280.
0751.
5m1.
04+93IT=98.
05;β+=2.
0596Ru860728STABLE(>67Py)0+0185No03TIS=5.
5414;2β+96Rh79679139.
90m0.
10(6+)93β+=10096Rhm796271352.
00.
11.
51m0.
02(3+)93IT=605;β+=40596Pd76230150122s20+93β+=10096Pdm737001502530.
80.
11.
81s0.
018+9398Gr.
BTDIT=10096Ag64570#400#4.
45s0.
04(8+)9303Ba39TJβ+=100;β+p=9.
71796Agm64570#400#0#50#6.
9s0.
6(2+)03Ba39TJDβ+=100;β+p=18596Agn64570#400#700ns20097Gr02TIT96Cd56100#500#1#s0+β+96RbT:ENSDFaverageof8values.
Thereisalso93Ru01=201(1)96RbmI:non-observationby81Th04isnotincontradictionwith81Bo30experiment96RbmI:existenceofthisisomerisdiscussedinENSDF96ZrT:from21(+8–4statistics+2systematics);other93Ka12=39(9)ingeochemical96ZrT:experiment,notused:observationof2βdecayquestionnedby96Ba3796PdmT:supersedes97Gr02=1.
7(0.
1);other83Gr01=2.
2(0.
3)outweighed96AgT:average03Ba39=4.
40(0.
06)97Sc30=4.
50(0.
06)96AgD:averageβ+p97Sc30=11.
9(2.
6)82Ku15=8.
0(2.
3);96He25=3.
7(0.
9)notused97Br34650#800#10#ms(>300ns)3/2#9797Be70Iβ97Kr47920#500#63ms43/2+#03Be05TDβ=100;βn=6.
7697Rb5836030169.
9ms0.
73/2+9393Ru01Dβ=100;βn=25.
7897Sr6878819429ms51/2+93β=100;βn99.
3;IT100Ty)0+0352Fr23TIS=24.
1331;2β98Tc8642844.
2My0.
3(6)+03β=100;β+=098Tcm86337490.
760.
1614.
7s3(2)03IT=10098Ru882246STABLE0+03IS=1.
87398Rh83175128.
72m0.
12(2)+03β+=10098Rhm83120#50#60#50#3.
6m0.
2(5+)03IT=895;β+=11598Pd813002117.
7m0.
30+03β+=10098Ag730607047.
5s0.
3(5+)03ABBW03Jβ+=100;β+p=0.
0012598Agm7289070167.
830.
15220ns20(3+)0398Gr.
BETDIT=10098Cd67630809.
2s0.
30+03β+=100;β+p300ns)0+9797Be70Iβ100Rb46700#300#51ms8(3+)9793Ru01Dβ=100;βn=5.
612;.
.
.
100Sr60220130202ms30+97β=100;βn=0.
7813100Y6729080735ms71,297β=100;βn=0.
928100Ym67090#220#200#200#940ms30(3,4,5)+#97β=100100Zr76600407.
1s0.
40+97β=100100Nb79939261.
5s0.
21+97β=100100Nbm794712847040BD2.
99s0.
11(4+,5+)97β=100100Mo8618468.
5Ey0.
50+9797Al02TIS=9.
6323;2β=100100Tc86016.
22.
215.
8s0.
11+97β≈100;ε=0.
00189100Tcm85815.
52.
2200.
670.
048.
32s0.
14(4)+97100Tcn85772.
22.
2243.
960.
043.
2s0.
2(6)+97100Ru89219.
02.
0STABLE0+97IS=12.
607100Rh855841820.
8h0.
1197β+=100100Rhm8547618107.
60.
24.
6m0.
2(5+)97IT≈98.
3;β+≈1.
7100Pd85226113.
63d0.
090+97ε=100100Ag78150802.
01m0.
09(5)+97β+=100100Agm781308015.
520.
162.
24m0.
13(2)+97β+=;IT100Cd7425010049.
1s0.
50+97β+=100100Cdm717001002548.
60.
560ns3(8)+97IT=100100In641702505.
9s0.
2(6,7)+9702Pl03TJβ+=100;β+p>3.
9100Sn567807101.
1s0.
40+97β+=100;β+p300ns)0197Be70Iβ103Y58940#300#224ms195/2+#0196Me09Tβ=100;βn=83103Zr683701101.
3s0.
1(5/2)01β=100103Nb75320701.
5s0.
2(5/2+)01β=100103Mo808506067.
5s1.
5(3/2+)01β=100103Tc845971054.
2s0.
85/2+01β=100103Ru87258.
82.
039.
26d0.
023/2+01β=100103Rum87020.
62.
1238.
20.
71.
69ms0.
0711/201IT=100103Rh88022.
22.
8STABLE1/201IS=100.
103Rhm87982.
42.
839.
7560.
00656.
114m0.
0097/2+01IT=100103Pd87479.
12.
916.
991d0.
0195/2+01ε=100103Pdm86694.
32.
9784.
790.
1025ns211/201IT=100103Ag847911765.
7m0.
77/2+01β+=100103Agm8465717134.
450.
045.
7s0.
31/201IT=100103Cd80649157.
3m0.
15/2+01β+=100103In745992560s19/2+#0197Sz04Tβ+=100103Inm7396725631.
70.
134s21/2#0197Sz04ETDβ+=67;IT=33103Sn66970#300#7s35/2+#01β+=100;β+p=103Sb56180#300#100#ms(>1.
5s)5/2+#0195Ry03Iβ+103YT:average96Me09=230(20)96Lh04=190(50)60G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)104Sr44400#700#30#ms(>300ns)0+0097Be70Iβ104Y54910#400#180ms600099Wa09Dβ=100;βn=104Zr66340#400#1.
2s0.
30+00β=100104Nb722201004.
9s0.
3(1+)00β=100;βn=0.
063104Nbm72010100220120BD940ms40high00β=100;βn=0.
053104Mo803305060s20+00β=100104Tc824905018.
3m0.
33+#00β=100104Tcm824205069.
70.
23.
5s0.
32(+)00IT=100104Ru880893STABLE0+00IS=18.
6227;2β104Rh86949.
82.
842.
3s0.
41+00β≈100;β+=0.
4510104Rhm86820.
82.
8128.
9670.
0044.
34m0.
035+00IT≈100;β=0.
131104Pd893904STABLE0+00IS=11.
148104Ag85111669.
2m1.
05+00β+=100104Agm8510466.
90.
433.
5m2.
02+00β+≈100;IT300ns)9797Be70Iβ105Y51350#500#60#ms(>300ns)5/2+#9794Be24Iβ105Zr62360#400#600ms10097β=100;βn105Nb708501002.
95s0.
065/2+#9496Me09Dβ=100;βn=1.
79105Mo773407035.
6s1.
6(5/2)93β=100105Tc82290607.
6m0.
1(3/2)93β=100105Ru8592834.
44h0.
023/2+93β=100105Rh87846435.
36h0.
067/2+93β=100105Rhm877164129.
7810.
00445s1/293IT=100105Pd884134STABLE5/2+93IS=22.
338105Ag870681141.
29d0.
071/293β+=100105Agm870431125.
4650.
0127.
23m0.
167/2+93IT≈100;β+=0.
347105Cd843301255.
5m0.
45/2+93β+=100105In79481175.
07m0.
079/2+9387Eb02Jβ+=100105Inm7880717674.
10.
348s6(1/2)93IT=;β+=25#105Sn732608034s1(5/2+)9395Pf01Tβ+=100;β+p=105Sb638201001.
12s0.
16(5/2+)02β+;p≈1;β+p105Te52500#500#1#s5/2+#α;β+105RhmT:noerrorgiven;othervalue:30s(seeENSDF:remeasurementrecommended)105SnJ:from85De08105TeI:the3eventsreportedin95Ry03arenottrustedbyNUBASE106Y46770#700#50#ms(>300ns)9797Be70Iβ106Zr59700#500#200#ms(>300ns)0+9794Be24Iβ106Nb67100#200#920ms402+#9496Me09TDβ=100;βn=4.
53106Mo76255188.
73s0.
120+9495Jo02Tβ=100106Tc797751335.
6s0.
6(1,2)94β=100106Ru863228373.
59d0.
150+94β=100106Rh86361829.
80s0.
081+94β=100106Rhm862251113612BD131m2(6)+94β=100106Pd899024STABLE0+94IS=27.
333106Ag86937523.
96m0.
041+94β+=;β≈0.
5106Agm86847589.
660.
078.
28d0.
026+94β+=100;IT≤4.
2e–6.
.
.
A-groupiscontinuedonnextpage.
.
.
G.
Audietal.
/NuclearPhysicsA729(2003)3–12861NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
106Cd871326STABLE(>410Ey)0+9402Tr04TIS=1.
256;2β+106In80606126.
2m0.
17+94β+=100106Inm805771228.
60.
35.
2m0.
1(3+)94β+=100106Sn77430501.
92m0.
080+94β+=100106Sb66330#310#600ms200(4+)9794Se01Jβ+=100106Sbm65330#590#1000#500#220ns2098Li50TIT=100106Te5821013070s200+9494Pa11Tα=100106ZrI:andT>240nsin97So07106NbT:average96Me09=900(20)83Sh06=1020(50)106SbT:from95Le.
C,Fig.
4,preliminary106TeT:average94Pa11=60(+40–20)81Sc17=60(+30–10)107Y42720#500#30#ms(>300ns)5/2+#0097Be70Iβ107Zr55190#300#150#ms(>300ns)0094Be24Iβ107Nb64920#400#300ms95/2+#0096Me09TDβ=100;βn=6.
015107Mo729401603.
5s0.
5(7/2)00β=100107Mom7287016066.
30.
2470ns30(5/2)00IT=100107Tc7910015021.
2s0.
2(3/2)00β=100107Tcm7903015065.
71.
0184ns3(5/2)00IT=100107Ru839201203.
75m0.
05(5/2)+00β=100107Rh868631221.
7m0.
47/2+00β=100107Rhm8659512268.
360.
04>10s1/200IT=100107Pd8836846.
5My0.
35/2+00β=100107Pdm881534214.
60.
321.
3s0.
511/200IT=100107Ag884024STABLE1/200IS=51.
8398107Agm88309493.
1250.
01944.
3s0.
27/2+00IT=100107Cd8698566.
50h0.
025/2+00β+=100107In835601132.
4m0.
39/2+00β+=100107Inm8288211678.
50.
350.
4s0.
61/200IT=100107Sn78580802.
90m0.
05(5/2+)00β+=100107Sb70650#300#4.
6s0.
85/2+#00β+=100107Te60540#300#3.
1ms0.
15/2+#00α=7030;β+=3030107ZrI:andT>240nsin97So07107NbT:average96Me09=300(30)91Hi02=300(10)108Y37740#800#20#ms(>300ns)0095Cz.
AIβ;βn108Zr52200#600#80#ms(>300ns)0+0097Be70Iβ;βn108Nb60700#300#193ms17(2+)00β=100;βn=6.
25108Mo71300#200#1.
09s0.
020+00β=100108Tc759501305.
17s0.
07(2)+00β=100108Ru836701204.
55m0.
050+00β=100108Rh8502011016.
8s0.
51+00β=100108Rhm850804060110BD6.
0m0.
3(5)(+#)00β=100108Pd895243STABLE0+00IS=26.
469108Ag8760242.
37m0.
011+00β=97.
1520;β+=2.
8520108Agm874934109.
4400.
007418y216+00β+=91.
39;IT=8.
79108Cd892526STABLE(>410Py)0+0295Ge14TIS=0.
893;2β+108In841161058.
0m1.
27+00β+=100108Inm840861029.
750.
0539.
6m0.
72+00β+=100108Sn820412010.
30m0.
080+00β+=100108Sb72510#210#7.
4s0.
3(4+)00β+=100;β+p108Te657201002.
1s0.
10+0085Ti02Dβ+=514;α=494;108I52650#360#36ms61+#0094Pa12Dα=;β+=9#;p300ns)9997Be70Iβ109Nb58100#500#190ms305/2+#99β=100;βn=315109Mo67250#300#530ms607/2#99β=100109Tc74540100860ms403/2#99β=100;βn=0.
082109Ru808507034.
5s1.
05/2+#99β=100109Rh850111280s27/2+99β=100109Pd87607313.
7012h0.
00245/2+99β=100109Pdm874183188.
9900.
0104.
696m0.
00311/299IT=100109Ag88722.
72.
9STABLE1/299IS=48.
1618109Agm88634.
72.
988.
03410.
001139.
6s0.
27/2+99IT=100109Cd885084461.
4d1.
25/2+99ε=100109Cdm88448459.
60.
412s21/2+99IT=100109Cdn880454463.
00.
510.
9s0.
511/299IT=100109In8648964.
2h0.
19/2+99β+=100109Inm858396650.
10.
31.
34m0.
071/299IT=100109Inn8438762101.
80.
2209ms6(19/2+)99IT=100109Sn826391018.
0m0.
25/2(+)99β+=100109Sb762591917.
0s0.
75/2+#99β+=100109Te67610604.
6s0.
3(5/2+)99β+=;α=3.
913;109I57610100103s5(5/2+)0287Gi02Jp=100109TeDβ+p=9.
431;β+α300ns)0+0097Be70Iβ110Nb53620#500#170ms202+#00β=100;βn=408110Mo65460#400#300ms400+00β=100;βn110Tc7096080920ms30(2+)0096Me09Dβ=100;βn=0.
042110Ru799805011.
6s0.
60+00β=100110Rh827805028.
5s1.
5(>3)(+#)00β=100110Rhm82839226050BD3.
2s0.
21+00β=100110Pd8834911STABLE(>600Py)0+0052Wi26TIS=11.
729;2β110Ag87460.
62.
924.
6s0.
21+00β≈100;ε=0.
306110Agm87343.
02.
9117.
590.
05249.
950d0.
0246+0002Un02Tβ=98.
646;IT=1.
366110Cd90353.
02.
7STABLE0+00IS=12.
4918110In86475124.
9h0.
17+00β+=100110Inm864131262.
10.
569.
1m0.
52+00β+=100110Sn85844144.
11h0.
100+00ε=100110Sb77540#200#23.
0s0.
4(4+)0097La13Jβ+=100110Te722805018.
6s0.
80+00β+≈100;α=0.
003#110I60320#310#650ms201+#00β+=834;α=174;110Xe51900130310ms1900+0002Ma19TDα=6435;β+110IDβ+p=113;β+α=1.
13G.
Audietal.
/NuclearPhysicsA729(2003)3–12863NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)111Nb50630#500#80#ms(>300ns)5/2+#9797Be70Iβ111Mo61100#400#200#ms(>300ns)9794Be24Iβ111Tc69220110290ms203/2#9696Me09TDβ=100;βn=0.
8520111Ru76670702.
12s0.
07(5/2+)9698Lh02Jβ=100111Rh823573011s1(7/2+)96β=100111Pd860041123.
4m0.
25/2+96β=100111Pdm8583211172.
180.
085.
5h0.
111/296IT=733;β=273111Ag8822137.
45d0.
011/296β=100111Agm88161359.
820.
0464.
8s0.
87/2+96IT=99.
32;β=0.
72111Cd89257.
52.
7STABLE1/2+00IS=12.
8012111Cdm88861.
32.
7396.
2140.
02148.
50m0.
0911/200IT=100111In8839652.
8047d0.
00049/2+00ε=100111Inm878595536.
950.
067.
7m0.
21/200IT=100111Sn85945735.
3m0.
67/2+96β+=100111Snm856907254.
720.
0812.
5s1.
01/2+111Sb808882875s1(5/2+)96β+=100111Te734807019.
3s0.
45/2+#97β+=100;β+p=111I64950#300#2.
5s0.
25/2+#96β+≈100;α=0.
088111Im63550#300#1398121ns2(11/2)111Xe54400#300#740ms2005/2+#9694Pa11Dβ+;α=107111XemnonexistentRN900ms20090Tu.
AT111MoI:andT>240nsin97So07111TcT:supersedes88Pe13=300(30)fromsamegroup111XemI:fromassigningαdecaytoisomerinolderversionofENSDF112Nb45800#700#60#ms(>300ns)2+#9797Be70Iβ112Mo58830#600#150#ms(>300ns)0+9794Be24Iβ112Tc66000120290ms202+#9799Wa09TDβ=100;βn=1.
52112Ru75480701.
75s0.
070+97β=100112Rh79740503.
4s0.
41+9799Lh01Tβ=100112Rhm794106033070BD6.
73s0.
15>39799Lh01Tβ=100112Pd863361821.
03h0.
050+97β=100112Ag86624173.
130h0.
0092()97β=100112Cd90580.
52.
7STABLE0+97IS=24.
1321112In87996514.
97m0.
101+97β+=563;β=443112Inm878395156.
590.
0520.
56m0.
064+97IT=100112Inn876455350.
760.
09690ns507+97IT=100112Inp873825613.
690.
142.
81s0.
0389787Eb02JIT=100112Sn886614STABLE0+97IS=0.
971;2β+112Sb816011851.
4s1.
03+97β+=100112Te773001702.
0m0.
20+97β+=100112I67100#210#3.
42s0.
111+#9778Ro19Dβ+≈100;α=0.
0012;112Xe599701002.
7s0.
80+9794Pa11Dβ+≈100;α=0.
98112Cs46290#300#500s1001+#02p=100112RhT:supersedes91Jo11=2.
1(0.
3)and88Ay02=3.
8(0.
6)ofsamegroup112RhmT:supersedes88Ay02=6.
8(0.
2)112IDβ+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%64G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)113Nb42200#800#30#ms(>300ns)5/2+#9897Be70Iβ113Mo54140#600#100#ms(>300ns)9894Be24Iβ113Tc63720#300#170ms203/2#9899Wa09TDβ=100;βn=2.
13113Ru7220070800ms50(5/2+)9898Ku17Jβ=100113Rum720707013018510ms30(11/2)98Ku17ETJIT=;β=113Rh78680502.
80s0.
12(7/2+)9893Pe11Jβ=100113Pd836904093s5(5/2+)98β=100113Pdm836104081.
10.
3300ms100(9/2)98IT=100113PdnnonexistentRN>100s9881Me17I113Ag87033175.
37h0.
051/298β=100113Agm869901743.
500.
1068.
7s1.
67/2+98IT=647;β=367113Cd89049.
32.
77.
7Py0.
31/2+98IS=12.
2212;β=100113Cdm88785.
82.
7263.
540.
0314.
1y0.
511/298β≈100;IT=0.
14113In893703STABLE9/2+99IS=4.
295113Inm889783391.
6990.
0031.
6579h0.
00041/299IT=100113Sn883334115.
09d0.
031/2+00β+=100113Snm88256477.
3860.
01921.
4m0.
47/2+00IT=91.
123;β+=8.
923113Sb84420186.
67m0.
075/2+98β+=100113Te78347281.
7m0.
2(7/2+)98β+=100113I71130506.
6s0.
25/2+#98β+=100;α=3.
31e–7;113Xe62090802.
74s0.
085/2+#9885Ti02Dβ+≈100;α=0.
0115;113Cs5170010016.
7s0.
75/2+#02p=100;α=0113TcT:98Ku17=110(30)and92Ay02=130(50)arefromsameauthors113RumE:abovethe99keVlevelandbelow160keV113PdnI:existenceisnotpossiblesincediscoveryof113Pdmby93Pe11113IDβ+α113XeDβ+p=74;β+α≈0.
0074113XeD:α=0.
0024-0.
0204%fromestimatedlimitforthereducedwidth,see85Ti02113XeD:β+pandβ+αderivedfromβ+p/α=605(35)andβ+p/β+α=500-1500in85Ti02114Mo51310#700#80#ms(>300ns)0+0397Be70Iβ114Tc59730#600#150ms302+#03β=100;βn=114Ru70530#230#530ms600+03β=100;βn114Rh756301101.
85s0.
051+03β=100;βn114Rhm75430#190#200#150#1.
85s0.
05(4,5)03β=100114Pd83497242.
42m0.
060+03β=100114Ag84949254.
6s0.
11+03β=100114Agm847502519951.
50ms0.
05(92Py)0+0395Ge14TIS=28.
7342;2β114In88572371.
9s0.
11+03β=99.
5015;β+=0.
5015114Inm883823190.
290.
0349.
51d0.
015+03IT=96.
7524;β+=3.
2524114Inn880703501.
940.
0343.
1ms0.
6(8)03IT=100114Inp879303641.
720.
034.
3s0.
4(7+)03IT=100114Sn905613STABLE0+03IS=0.
661114Snm8747433087.
370.
07733ns14703IT=100114Sb84515283.
49m0.
03(3+)03β+=100114Sbm8402028495.
50.
07219s12(8)03IT=100114Te818892815.
2m0.
70+03β+=100114I72800#300#2.
1s0.
21+03β+=100;β+p114Im72530#300#265.
90.
56.
2s0.
5(7)03ABBW96Dβ+=912;IT=92114Xe670861110.
0s0.
40+03β+=100114Cs54540#310#570ms20(1+)03β+≈100;α=0.
0186;114Ba45950140530ms2300+0302Ma19Dβ+≈100;β+p=2010;114ImD:evaluatedforNUBASEbyJ.
Blachot,basedon114IITdecay114CsDβ+p=8.
713;β+α=0.
193114BaDα=0.
93;12C300ns)99β;βn115Tc57110#700#100#ms(>300ns)3/2#99β;βn115Ru66430130740ms8099β=100;βn115Rh7421080990ms507/2+#99β=100115Pd804006025s25/2+#99β=100115Pdm803106089.
180.
2550s311/2#99β=92.
020;IT=8.
020115Ag849903020.
0m0.
51/299β=100115Agm849503041.
160.
1018.
0s0.
77/2+99β=79.
03;IT=21.
03115Cd88090.
52.
753.
46h0.
101/2+99β=100115Cdm87909.
52.
7181.
00.
544.
56d0.
24(11/2)99β≈100;IT15115PdmJ:E3transitiontoground-state115TemE:lessthan20keV,fromENSDF115XeDβ+α=0.
00031116Tc52750#700#90#ms(>300ns)2+#0197Be70Iβ116Ru64450#700#400#ms(>300ns)0+0194Be24Iβ116Rh70740140680ms601+01β=100;βn116Rhm70540#210#200#150#570ms50(6)01β=100116Pd799606011.
8s0.
40+01β=100116Ag82570502.
68m0.
10(2)01β=100116Agm824905081.
900.
208.
6s0.
3(5+)01β=94.
015;IT=6.
015116Cd88719330Ey40+0103Da09TIS=7.
4918;2β=100116In88250414.
10s0.
031+0198Bh04Dβ≈100;ε=0.
236116Inm881234127.
2670.
00654.
29m0.
175+01β=100116Inn879604289.
6600.
0062.
18s0.
04801IT=100116Sn91528.
12.
9STABLE0+01IS=14.
549116Sb86821615.
8m0.
83+01β+=100116Sbm864404038040BD60.
3m0.
6801β+=100116Te85269282.
49h0.
040+01β+=100116I774901002.
91s0.
151+01β+=100116Im77090#110#400#50#3.
27s0.
16(7)01IT=100116Xe730471359s20+01β+=100116Cs62070#100#700ms40(1+)01β+=100;β+p=0.
287;.
.
.
116Csm61970#120#100#60#3.
85s0.
134+,5,601β+=100;β+p=0.
5115;.
.
.
116Ba54600#400#1.
3s0.
20+01β+=100;β+p=31116RuI:andT>240nsin97So07116CdT:from29(1statistics+4–3systematics);supersedes00Da27=26(1statistics+7–4systematics)116CsDβ+α=0.
04925116CsmDβ+α=0.
008266G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)117Tc49850#700#40#ms(>300ns)3/2#0297Be70Iβ117Ru60010#700#300#ms(>300ns)0294Be24Iβ117Rh68950#500#440ms407/2+#02β=100117Pd76530604.
3s0.
3(5/2+)02β=100117Pdm7633060203.
20.
319.
1ms0.
711/2#02IT=100117Ag822705073.
6s1.
41/2#02β=100117Agm822405028.
60.
25.
34s0.
05(7/2+)02β=94.
015;IT=6.
015117Cd8642532.
49h0.
041/2+02β=100117Cdm862893136.
40.
23.
36h0.
05(11/2)02β≈100;IT≈0117In88945643.
2m0.
39/2+02β=100117Inm886306315.
3020.
012116.
2m0.
31/202β=52.
915;IT=47.
115117Sn90400.
02.
9STABLE1/2+02IS=7.
687117Snm90085.
42.
9314.
580.
0413.
76d0.
0411/202IT=100117Sb8864592.
80h0.
015/2+02β+=100117Te850971362m21/2+02β+=100;e+=251117Tem8480113296.
10.
5103ms3(11/2)0299Mo30JIT117Ten8482313274.
40.
119.
9ns0.
45/2+02IT=100117I80435282.
22m0.
04(5/2)+02β+=100;e+≈77117Xe741851061s25/2(+)02β+=100;β+p=0.
00296117Cs66440608.
4s0.
69/2+#02β+=100117Csm66290#100#150#80#6.
5s0.
43/2+#02β+=100117Csx66390805050R=spmix117Ba57290#300#1.
75s0.
07(3/2)(+#)0297Ja12Dβ+=100;β+p=133;117La46510#400#23.
5ms2.
6(3/2+,3/2)02p=;β+=6#117Lam46370#400#13815p10ms5(9/2+)02p=;β+=3#117RuI:andT>240nsin97So07117BaDβ+α=0.
0248117BaD:β+pfrom97Ja12.
β+p/β+α=350-1200from85Ti02yieldsβ+α=0.
011-0.
037118Tc45200#900#30#ms(>300ns)2+#9795Cz.
AIβ118Ru57920#800#200#ms(>300ns)0+94Be24Iβ118Rh65140#500#310ms30(410)(+#)9700Jo18TJDβ=100118Pd754702101.
9s0.
10+95β=100118Ag79570603.
76s0.
1519593Ja03Jβ=100118Agm7944060127.
490.
052.
0s0.
24(+)9595Ap.
AEβ=59;IT=41118Cd867092050.
3m0.
20+95β=100118In8723085.
0s0.
51+95β=100118Inm87130#50#100#50#4.
364m0.
0075+9594It.
ATβ=100118Inn86990#50#240#50#8.
5s0.
3895IT=98.
63;β=1.
43118Sn91656.
12.
9STABLE0+95IS=24.
229118Sb8799943.
6m0.
11+95β+=100118Sbm8774962506BD5.
00h0.
02895β+=100118Sbn87948450.
8140.
02120.
6s0.
6(3)+118Te87721156.
00d0.
020+95ε=100118I809712013.
7m0.
5295β+=100118Im8078120190.
11.
08.
5m0.
5(7)9594Ka39Eβ+≈100;IT=118Xe78079103.
8m0.
90+95β+=100118Cs684091314s2295β+=100;β+p=0.
02114;.
.
.
118Csm68310#60#100#60#17s3(7)9593Be46Jβ+=100;β+p=0.
02114;.
.
.
118Csx684041254R300ns)97Be70Iβ119Rh63240#600#300#ms(>300ns)7/2+#94Be24Iβ119Pd71620#300#920ms13000β=100119Ag7856090&6.
0s0.
51/2#00β=100119Agm78540#90#20#20#&2.
1s0.
17/2+#00β=100119Cd83910802.
69m0.
02(3/2+)00β=100119Cdm8376080146.
540.
112.
20m0.
0211/2#00β=100119In8770482.
4m0.
19/2+00β=100119Inm873938311.
370.
0318.
0m0.
31/200β=94.
415;IT=5.
615119Sn90068.
42.
9STABLE1/2+00IS=8.
594119Snm89978.
92.
989.
5310.
013293.
1d0.
711/200IT=100119Sb89477838.
19h0.
225/2+00ε=100119Sbm866251128527850ms9027/2+#00ABBWEIT=100119Te87184816.
05h0.
051/2+00β+=100119Tem869238260.
960.
054.
70d0.
0411/200ε=99.
594;e+=0.
414;119I837662819.
1m0.
45/2+00β+=100119Xe78794105.
8m0.
35/2(+)0090Ne.
AJe+=795;ε=215119Cs723051443.
0s0.
29/2+00β+=100;β+α300ns)0+0295Cz.
AIβ120Rh59230#600#200#ms(>300ns)94Be24Iβ120Pd70150120500ms1000+02β=100120Ag75650701.
23s0.
043(+#)0293Ru01Dβ=100;βn300ns)7/2+#94Be24Iβ121Pd66260#500#400#ms(>300ns)0094Be24Iβ121Ag74660150790ms207/2+#00β=100;βn=0.
08013121Cd810608013.
5s0.
3(3/2+)00β=100121Cdm8085080214.
860.
158.
3s0.
8(11/2)00β=100121In858412723.
1s0.
69/2+00β=100121Inm8552827312.
980.
083.
88m0.
101/200β=98.
82;IT=1.
22121Sn89204.
12.
527.
03h0.
043/2+00β=100121Snm89197.
82.
56.
300.
0643.
9y0.
511/20002Re18TIT=77.
620;β=22.
420121Snn87205.
32.
71998.
80.
95.
3s0.
519/2+#00IT=100121Sb89595.
12.
2STABLE5/2+00IS=57.
215121Te885512619.
16d0.
051/2+00β+=100121Tem8825726293.
9910.
022154d711/200IT=88.
611;β+=11.
411121I86287102.
12h0.
015/2+00β+=100121Im83910102376.
90.
49.
0s1.
500IT=100121Xe824731140.
1m2.
0(5/2+)00β+=100121Cs7710014155s43/2(+)00β+=100121Csm770321468.
50.
3122s39/2(+)00β+=83;IT=17121Ba7074014029.
7s1.
55/2(+)00β+=100;β+p=0.
021121La62400#500#5.
3s0.
211/2#00β+=100;β+p121Ce52700#500#1.
1s0.
1(5/2)(+#)0099Li46Jβ+=100;β+p≈1121Pr41580#700#600ms300(3/2)0090Bo39TJDp=;β+;β+p121PdI:andT>240nsin97So07121PrT:T=1.
4(0.
8)sinENSDF:nottrustedtobelongtothisnuclide122Rh52900#700#50#ms(>300ns)97Be70Iβ122Pd64690#400#300#ms(>300ns)0+9894Be24Iβ122Ag71230#210#520ms14(3+)9495Fe12Tβ=100;βn=0.
18610122Agm71150#220#80#50#1.
5s0.
58#94β=100;βn122Cd80730405.
24s0.
030+94β=100122In83580501.
5s0.
31+94β=100122Inm83540#80#40#60#10.
3s0.
65+94β=100122Inn83290130290140BD10.
8s0.
4894β=100122Sn89945.
92.
7STABLE0+94IS=4.
633;2β122Sb88330.
22.
22.
7238d0.
0002294β=97.
5912;122Sbm88166.
62.
2163.
55910.
00174.
191m0.
003(8)94IT=100122Sbn88192.
72.
2137.
4720.
001530s5+122Te90314.
01.
5STABLE0+94IS=2.
5512122I8608053.
63m0.
061+94β+=100122Xe853551120.
1h0.
10+94ε=100122Cs781403021.
18s0.
191+9693Al03Tβ+=100;β+α240nsin97So07122AgD:βnintensityisfrom93Ru01122SbDβ+=2.
4112122CsT:average93Al03=21.
2(0.
2)69Ch18=21.
0(0.
7)122CsD:β+αintensityupperlimitisfrom75Ho09122CeI:T=8.
7(0.
7)sinNDS71(1994)wasmisprintfor122La;correctedinENSDFG.
Audietal.
/NuclearPhysicsA729(2003)3–12869NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)123Pd60610#600#200#ms(>300ns)94Be24Iβ123Ag69960#210#296ms6(7/2+)9495Fe12Tβ=100;βn=0.
555123Cd77310402.
10s0.
02(3/2)+94β=100123Cdm7699040316.
520.
231.
82s0.
03(11/2)94β=;IT=123In83426245.
98s0.
069/2+94β=100123Inm8309924327.
210.
0447.
8s0.
51/294β=100123Sn87820.
52.
7129.
2d0.
411/294β=100123Snm87795.
92.
724.
60.
440.
06m0.
013/2+94β=100123Sb89224.
12.
1STABLE7/2+94IS=42.
795123Te89171.
91.
5>600Ty1/2+9496Al30TIS=0.
893;ε=100123Tem88924.
31.
5247.
550.
04119.
25d0.
1511/294IT=100123I87943413.
2235h0.
00195/2+9402Un02Tβ+=100123Xe85249102.
08h0.
021/2+9490Ne.
AJβ+=100123Xem8506410185.
180.
225.
49s0.
267/2()123Cs81044125.
87m0.
041/2+9493Al03Tβ+=100123Csm8088712156.
740.
211.
64s0.
12(11/2)94IT=100123Csx810371374R300ns)0+97Be70Iβ124Ag66470#200#172ms53+#97β=100;βn>0.
1124Agm66470#220#0#100#200#ms8#95Kr.
AIβ;IT124Cd76710601.
25s0.
020+97β=100124In80880503.
11s0.
103+97β=100124Inm80900502070BD3.
7s0.
2(8)(#)97β≈100;IT124Sn88236.
81.
4STABLE(>100Py)0+9752Ka41TIS=5.
795;2β124Snm85911.
81.
42325.
010.
043.
1s0.
5797IT=100124Snn85580.
21.
52656.
60.
545s510+#97IT=100124Sb87620.
32.
160.
20d0.
03398β=100124Sbm87609.
42.
110.
86270.
000893s55+97IT=755;β=255124Sbn87583.
52.
136.
84400.
001420.
2m0.
2(8)97IT=100124Sbp87579.
52.
140.
80380.
00073.
2s0.
3(3+,4+)97IT=100124Te90524.
51.
5STABLE0+97IS=4.
7414124I87365.
02.
44.
1760d0.
0003297β+=100124Xe87660.
11.
8STABLE(>48Py)0+9789Ba22TIS=0.
091;2β+124Cs81731830.
9s0.
41+9793Al03Tβ+=100124Csm812688462.
550.
176.
3s0.
2(7)+97IT=100124Csx81701223020R=spmix124Ba790901211.
0m0.
50+97β+=100124La702606029.
21s0.
17(7,8)9797As05Tβ+=100124Lam70160#120#100#100#21s4low(+#)9797As05Tβ+=100124Ce64820#300#9.
1s1.
20+9897As05Tβ+=100124Pr53130#600#1.
2s0.
297β+=100;β+p=124Nd44500#600#500#ms0+β+124AgmI:"Thereissomeevidenceforalow-spinandahigh-spinisomerin124Ag"124CsT:average93Al03=30.
9(0.
5)78Ek05=30.
8(0.
5)124LaJ:for124Laand124Lamarefrom92Id01124CeT:average97As05=10.
8(1.
5)78Bo32=6(2)70G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)125Ag64800#300#166ms77/2+#99β=100;βn=125Cd7336070650ms203/2+#99β=100125Cdm73310505070BD570ms9011/2#9989Hu03Tβ=100125In80480302.
36s0.
049/2+99β=100125Inm8012030360.
120.
0912.
2s0.
21/2()99β=100125Sn85898.
51.
59.
64d0.
0311/299β=100125Snm85871.
01.
527.
500.
149.
52m0.
053/2+99β=100125Sb88255.
52.
62.
75856y0.
000257/2+99β=100125Te89022.
21.
5STABLE1/2+99IS=7.
0715125Tem88877.
41.
5144.
7720.
00957.
40d0.
1511/299IT=100125I88836.
41.
559.
400d0.
0105/2+99ε=100125Xe87192.
11.
916.
9h0.
21/2(+)99β+=100125Xem86939.
51.
9252.
600.
1456.
9s0.
99/2()99IT=100125Cs84088845m11/2(+)99β+=100125Csm838218266.
61.
1900ms30(11/2)9998Su16TJIT=100125Ba79668113.
5m0.
41/2(+#)99β+=100125La737592664.
8s1.
2(11/2)99β+=100125Lam7365226107.
00.
1390ms40(3/2+)9999Ca21ETJIT=100125Ce66660#200#9.
3s0.
3(7/2)9902Pe15Jβ+=100;β+p=125Pr57910#400#3.
3s0.
73/2+#02β+=100;β+p125Nd47620#400#600ms1505/2(+#)02β+=100125CdmT:unweighedaverage89Hu03=480(30)86Ma42=660(30)(BirgeratioB=4.
24)125LaJ:ENSDF'99saysground-statespinunknown;a(11/2)levelliesat8-9keVaboveground-state125LamJ:3/2+#fromsystematics;lowspinandeven-parityfrom99Ca21125CeT:average99Ca21=9.
6(0.
4)86Wi15=9.
2(1.
0)83Ni05=8.
9(0.
5)126Ag61010#300#107ms123+#03β=100;βn=126Cd7233050515ms170+03β=100126In77810401.
53s0.
013(+#)03β=100126Inm777105010060BD1.
64s0.
058(#)0379Fo10Jβ=100126Sn8602011230ky140+03β=100126Snm83801112218.
990.
086.
6s1.
4703IT=100126Snn83456112564.
50.
57.
7s0.
510+#03IT=100126Sb864003012.
35d0.
06(8)03β=100126Sbm863803017.
70.
319.
15m0.
08(5+)03β=864;IT=144126Sbn863603040.
40.
311s(3)03IT=100126Sbp8630030104.
60.
3553ns5(3+)03IT=100126Te90064.
61.
5STABLE0+03IS=18.
8425126I87911412.
93d0.
05203β+=52.
75;β=47.
35126Xe891696STABLE0+03IS=0.
091;2β+126Cs84345121.
64m0.
021+03β+=100126Csm8407212273.
00.
7>1s03IT=100126Csn8374912596.
11.
1171s1403IT=100126Ba8267012100m20+03β+=100126La749709054s2(5)(+#)03β+=100126Lam74760400210410BD20s20(0,1,2)03β+=100126Ce708212851.
0s0.
30+03β+=100126Pr60260#200#3.
12s0.
18(4,5,6)0388Ba42Tβ+=100;β+p=126Nd52890#400#1#s(>200ns)0+0300So11Iβ+126Pm39570#500#500#msβ+126LamT:97As05:"byfarshorterthan50s"126PrT:average95Os03=3.
14(0.
22)88Ba42=3.
0(0.
4)and83Ni05=3.
2(0.
6)G.
Audietal.
/NuclearPhysicsA729(2003)3–12871NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)127Ag58900#300#79ms37/2+#9896Wo.
ATDβ=100;βn=127Cd6852070370ms70(3/2+)96β=100127In76990401.
09s0.
019/2(+)9687Eb02Jβ=100;βn≤0.
03127Inm765207046070BD3.
67s0.
04(1/2)96β=100;βn=0.
694127Sn83499252.
10h0.
04(11/2)96β=100127Snm83494254.
70.
34.
13m0.
03(3/2+)96β=100127Sb8670053.
85d0.
057/2+96β=100127Te88281.
11.
59.
35h0.
073/2+96β=100127Tem88192.
81.
588.
260.
08109d211/296IT=97.
62;β=2.
42127I889834STABLE5/2+96IS=100.
127Xe88321436.
345d0.
0031/2+9602Un02Tε=100127Xem880244297.
100.
0869.
2s0.
99/296IT=100127Cs8624066.
25h0.
101/2+96β+=100127Csm857886452.
230.
2155s3(11/2)96IT=100127Ba828161112.
7m0.
41/2+96β+=100127Bam827361180.
330.
121.
9s0.
27/296IT=100127La77896265.
1m0.
1(11/2)96β+=100127Lam778812614.
81.
23.
7m0.
4(3/2+)96β+≈100;IT127Ce719806029s25/2+#9896Ge07Tβ+=100127Cem71980#120#0#100#34s2(1/2+)96Ge07TJDβ+=100127Pr64430#200#4.
2s0.
33/2+#98β+=100127Prm63830#280#600#200#50#ms11/298Mo30Jβ+;IT127Nd55420#400#1.
8s0.
45/2+#96β+=100;β+p=127Pm45060#600#1#s5/2+#β+;p127AgT:supersedes95Fe12=109(25)fromsamegroup128Ag54800#300#58ms501β=100;βn=128Cd67290290280ms400+01β=100128In7436050840ms60(3)+0193Ru01Dβ=100;βn=0.
0383128Inm7411050247.
870.
1010ms7(1)01IT=100128Inn740405032060BD720ms100(8)01β=100128Sn833352759.
07m0.
140+01β=100128Snm81244272091.
500.
116.
5s0.
5(7)01IT=100128Sb84609259.
01h0.
04801β=100128Sbm845992410710.
4m0.
25+01β=96.
410;IT=3.
610128Te88992.
11.
72.
2Yy0.
30+0196Ta04TIS=31.
748;2β=100128Tem86201.
41.
72790.
70.
4370ns3010+01IT=100128I87738424.
99m0.
021+01β=93.
18;β+=6.
98128Im876004137.
8500.
004845ns20401IT=100128In875714167.
3670.
005175ns15(6)01IT=100128Xe89860.
01.
4STABLE0+01IS=1.
923128Xem87072.
71.
52787.
30.
483ns2801IT=100128Cs8593153.
640m0.
0141+0193Al03Tβ+=100128Ba85402102.
43d0.
050+01ε=100128La78630505.
18m0.
14(5+)01β+=100128Lam78530#110#100#100#2s(15/2)96IT=100129Sbp82489212138.
90.
51.
1s0.
1(23/2+)03Ge04ETJIT=100129Te87003.
21.
869.
6m0.
33/2+96β=100129Tem86897.
71.
8105.
500.
0533.
6d0.
111/296IT=6317;β=3717129I88503315.
7My0.
47/2+96β=100129Xe88697.
40.
7STABLE1/2+96IS=26.
4424129Xem88461.
30.
7236.
140.
058.
88d0.
0211/296IT=100129Cs87500532.
06h0.
061/2+96β+=100129Ba85065112.
23h0.
111/2+96β+=100129Bam85057118.
420.
062.
16h0.
027/2+#96β+≈100;IT=129La813262111.
6m0.
23/2+96β+=100129Lam8115421172.
10.
4560ms5011/296IT=100129Ce76287283.
5m0.
3(5/2+)9793Al03Tβ+=100129Cem7617928107.
60.
162ns5(7/2)96IT=100129Pr6977430&30s4(3/2+)9696Gi08Jβ+=100129Prm6939030382.
70.
5&1#ms(11/2)97Gi07EJDIT=100129Nd62240#200#4.
9s0.
25/2+#96β+=100;β+p=129Pm52950#400#3#s(>200ns)5/2+#00So11Iβ+129Sm42250#500#550ms1005/2+#99Xu05TDβ+=100129AgI:theevaluatorsarenotconvincedbytheidenticationarguments129InT:average93Ru01=611(5)86Wa17=610(10)129InmDβn=2.
55129CeJ:from96Gi08(5/2+inENSDFwasfromtheory)130Ag46160#330#50ms0+01β=100;βn130Cd61570280162ms70+0101Ha39TDβ=100;βn=3.
510130In6989040290ms20(1)01β=100;βn=0.
9313130Inm69840405050BD538ms510#0193Ru01Tβ=100;βn=1.
6515130Inn694905040060BD540ms10(5+)01β=100;βn=1.
6515130Sn80139113.
72m0.
070+01β=100130Snm78192111946.
880.
101.
7m0.
17#01β=100130Sb822921739.
5m0.
88#01β=100130Sbm82287174.
800.
206.
3m0.
2(4,5)+01β=100130Te87351.
41.
9790Ey1000+0196Ta04TDIS=34.
0862;2β=100130Tem85205.
01.
92146.
410.
04115ns8(7)01IT=100130Ten846907266171.
90s0.
08(10+)01IT=100130Tep82976.
02.
64375.
41.
8261ns3301IT=100130I86932312.
36h0.
015+01β=100130Im86892339.
95250.
00138.
84m0.
062+01IT=842;β=162130Xe89881.
70.
7STABLE0+01IS=4.
082130Cs86900829.
21m0.
041+01β+=98.
4;β=1.
6130Csm867378163.
250.
113.
46m0.
06501IT≈100;β+=0.
162130Csx86873172715R=.
2.
1fsmix130Ba87261.
62.
8STABLE(>4.
0Zy)0+0196Ba24TIS=0.
1061;2β+130Bam84786.
52.
82475.
120.
189.
54ms0.
1480102Mo31TIT=100.
.
.
A-groupiscontinuedonnextpage.
.
.
G.
Audietal.
/NuclearPhysicsA729(2003)3–12873NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
130La81628268.
7m0.
13(+)01β+=100130Ce794232822.
9m0.
50+01β+=100130Cem76969282453.
60.
3100ns8(7)01IT=100130Pr711806040.
0s0.
4(6,7)(+#)0188Ba42Jβ+=100130Prm71080#120#100#100#10#s2+#0188Ba42Jβ+130Nd665962821s30+0101Gi17Tβ+=100130Pm55470#300#2.
6s0.
2(5+,6+,4+)0199Xi03Jβ+=100;β+p=130Sm47580#400#1#s0+01β+130Eu33940#500#1.
1ms0.
52+#02Ma61TDp=;β+=1#130InmT:average93Ru01=542(9)85Re.
A=532(6)and86Wa17=550(10)130InmT:76Lu02=580(10)atvariance,notused130TeT:seealsonumerous(notused)resultsin95Tr07130TeT:treatedbyENSDF'01asalowerlimit(notacceptedbyNUBASE)130TenE:lessthan25keVabove2648.
57(0.
22)(8+)level,seeENSDF'01130BamT:others66Br14=8.
8(0.
2)69Wa.
A=13.
5(1.
0)notused130PrmJ:88Ba42:thereisalsoalow-spincomponentin130Practivity130PrmJ:seealsothediscussionin01Gi17onthreeisomericstatesin130Pr130NdT:otherconictingdata,notused:00Xu08=13(3)77Bo02=28(3)131Cd55270#300#68ms37/2#00Ha55TDβ=100;βn=3.
510131In6813728280ms30(9/2+)9493Ru01Dβ=100;βn=2.
23131Inm677904035040BD350ms50(1/2)94β≈100;131Inn6404070410070BD320ms60(19.
.
23/2+)94β>99;131Sn773142156.
0s0.
5(3/2+)94β=100131Snm77230#40#80#30#58.
4s0.
5(11/2)9401Si.
AEβ=100;IT300Ey)0+9496Ba24TIS=0.
1011;2β+132La83740404.
8h0.
2294β+=100132Lam8355040188.
180.
1124.
3m0.
5694IT=76;β+=24132Ce82474213.
51h0.
110+99β+=100132Cem80133212340.
80.
59.
4ms0.
3(8)9901Mo05TJIT=100132Pr75210601.
49m0.
11(2+)0194Bu18TJβ+=100132Prm75210#120#0#100#20#s(5+)90Ko25Jβ+132Nd71426241.
56m0.
100+9795Bu11Tβ+=100132Pm61710#200#6.
3s0.
7(3+)92β+=100;β+p≈5e–5132Sm55250#300#4.
0s0.
30+92β+=100;β+p132Eu42500#400#100#ms93Li40Dβ+;p=0132PrT:average94Bu18=1.
47(0.
12)74Ar27=1.
6(0.
3)132NdT:average95Bu11=1.
47(0.
12)77Bo02=1.
75(0.
17)133In57930#300#165ms3(9/2+)0296Ho16Jβ=100;βn=8510133Inm57600#300#330#40#180#ms(1/2)96Ho16JIT133Sn70950401.
45s0.
037/2#9893Ru01Dβ=100;βn=0.
029424133Sb78943252.
5m0.
1(7/2+)95β=100133Te829452412.
5m0.
3(3/2+)95β=100133Tem8261124334.
260.
0455.
4m0.
4(11/2)95β=82.
530;IT=17.
530133I85887520.
8h0.
17/2+95β=100133Im8425351634.
1740.
0179s2(19/2)95IT=100133Xe87643.
62.
45.
2475d0.
00053/2+9502Un02Tβ=100133Xem87410.
42.
4233.
2210.
0182.
19d0.
0111/295IT=100133Cs88070.
9580.
022STABLE7/2+95IS=100.
133Ba87553.
51.
010.
51y0.
051/2+95ε=100133Bam87265.
31.
0288.
2470.
00938.
9h0.
111/295IT≈100;ε=0.
009611133La85494283.
912h0.
0085/2+95β+=100133Lam8495828535.
600.
0262ns311/2133Ce824231697m41/2+97β+=100133Cem823861637.
10.
84.
9h0.
49/297β+=100133Pr77938126.
5m0.
3(3/2+)97β+=100133Prm7774612192.
050.
141.
1s0.
2(11/2)9701Xu04TIT=100133Nd723305070s10(7/2+)97β+=100133Ndm7220050127.
970.
1170s(1/2)+9795Br24Dβ+≈100;IT=133Ndn7215050176.
100.
10300ns(9/2)97IT=100133Pm6541050&15s3(3/2+)9596Ga17Jβ+=100133Pmm6528050130.
41.
0&10#s(11/2)96Ga17EJβ+;IT133Sm57130#200#2.
90s0.
17(5/2+)0101Xu04Tβ+=100;β+p=133Eu47280#300#200#ms11/2#β+133InD:βnintensityisfrom93Ru01133PmmE:combiningγsfromTable1:214.
7+357.
7+453.
8–252.
8–643(1)133SmT:average01Xu04=3.
1(0.
5)85Wi07=2.
8(0.
2)77Bo02=3.
2(0.
4)G.
Audietal.
/NuclearPhysicsA729(2003)3–12875NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)134In52020#400#140ms4high0296Ho16Jβ=100;βn=65;134Sn668001001.
12s0.
080+94β=100;βn=1713134Sb7417040780ms60(0)95β=100134Sbm7409010080110BD10.
22s0.
09(7)95β=100;βn=0.
0918134Te825591141.
8m0.
80+98β=100134Tem80868111691.
240.
17164ns16+98IT=100134I84072852.
5m0.
2(4)+94β=100134Im837568316.
490.
223.
60m0.
10(8)94IT=97.
710;β=2.
310134Xe88124.
50.
8STABLE(>11Py)0+9489Ba22TIS=10.
4410;2β134Xem86159.
00.
91965.
50.
5290ms17794IT=100134Cs86891.
1810.
0262.
0648y0.
00104+94β=100;ε=0.
00031134Csm86752.
4370.
026138.
74410.
00262.
903h0.
008894IT=100134Ba88949.
90.
4STABLE0+95IS=2.
41718134La85219206.
45m0.
161+94β+=100134Ce84836203.
16d0.
040+94ε=100134Pr7851040&11m(5)94β+=100134Prm78510#110#0#100#&17m2294β+=100134Nd75646128.
5m1.
50+99β+=100134Ndm73353122293.
10.
4410s30(8)99IT=100134Pm667406022s1(5+)94β+=100134Pmm66740#120#0#100#5s(2+)94β+=100134Sm61510#200#10s10+94β+=100134Eu49830#200#500ms20094β+=100;β+p=134Gd41570#400#400#ms0+β+134InDβ2n99.
97;IT10Zy)0+0202Be74TIS=8.
8716;2β136Xem8453371891.
7030.
0142.
95s0.
096+02IT=100136Cs86338.
71.
913.
16d0.
035+02β=100136Csm858215518519s280283We07EIT=;β136Ba88886.
90.
4STABLE0+02IS=7.
85424136Bam86856.
40.
42030.
4660.
018308.
4ms1.
9702IT=100136La86040509.
87m0.
031+02β+=100136Lam85790502559114ms3(8)(#)02ABBWEIT=100136Ce8646813STABLE(>38Py)0+0201Da22TIS=0.
1852;2β+136Cem83373133095.
50.
42.
2s0.
210+02IT=100136Pr813271213.
1m0.
12+02β+=100136Prm8073212594.
620.
2291.
7ns0.
9(6)+02IT=100136Nd791991250.
7m0.
30+02β+=100136Pm7120080&107s6(5)02β+=100136Pmm7107090130120BD&47s2(2+)02β+=100136Sm668111247s20+02β+=100136Smm64546122264.
71.
115s1(8)02IT=100136Eu56260#200#3.
3s0.
3(7+)0289Vi04Dβ+=100;β+p=0.
093136Eum56260#540#0#500#3.
8s0.
3(3+)0289Vi04Dβ+=100;β+p=0.
093136Gd49050#400#1#s(>200ns)0+0200So11Iβ+136Tb35970#600#200#ms02β+136SbDβ2n=0.
28#136LamE:approx.
10-40keVabove230.
1level,fromENSDF'02,thus230.
1+25(9)137Sn50310#600#190ms605/2#02β=100;βn=5815137Sb60260#400#450ms507/2+#9402Sh08TDβ=100;βn=4910137Te695601202.
49s0.
053/2#9493Ru01Dβ=100;βn=2.
9916137I765032824.
13s0.
12(7/2+)9493Ru01TDβ=100;βn=7.
1423137Xe8237973.
818m0.
0137/294β=100137Cs86545.
60.
530.
1671y0.
00137/2+0102Un02Tβ=100137Ba87721.
20.
4STABLE3/2+97IS=11.
23224137Bam87059.
50.
4661.
6590.
0032.
552m0.
00111/297IT=100137La871011360ky207/2+94ε=100137Ce85879139.
0h0.
33/2+94β+=100137Cem8562513254.
290.
0534.
4h0.
311/294IT=99.
223;β+=0.
783137Pr83177121.
28h0.
035/2+94β+=100137Prm8261612561.
220.
232.
66s11/2137Nd795801138.
5m1.
51/2+01β+=100137Ndm7906111519.
430.
171.
60s0.
15(11/2)01IT=100137Pm7407313&2#m5/2+#β+137Pmm739205015050BD&2.
4m0.
111/294β+=100137Sm680304045s1(9/2)94β+=100137Smm67850#60#180#50#20#s1/2+#β+137Eu60020#200#8.
4s0.
511/2#9488Be.
ATβ+=100137Gd51210#400#2.
2s0.
27/2+#9499Xu05Tβ+=100;β+p=137Tb41000#600#600#ms11/2#96p;β+137IT:supersedes74Ru08=24.
5(0.
2)fromsamegroupG.
Audietal.
/NuclearPhysicsA729(2003)3–12877NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)138Sb55150#300#500#ms(>300ns)2#0394Be24Iβ;βn138Te65930#210#1.
4s0.
40+03β=100;βn=6.
321138I72330806.
23s0.
03(2)0393Ru01Dβ=100;βn=5.
4618138Xe801504014.
08m0.
080+03β=100138Cs82887933.
41m0.
18303β=100138Csm82807979.
90.
32.
91m0.
08603IT=812;β=192138Csx82847254023R=fsmix138Ba88261.
60.
4STABLE0+03IS=71.
69842138Bam86171.
10.
42090.
540.
06800ns1006+03IT=100138La865254102Gy15+03IS=0.
0901;138Lam86452472.
570.
03116ns5(3)+03IT=100138Ce8756910STABLE(>150Ty)0+0301Da22TIS=0.
2512;2β+138Cem85440102129.
170.
128.
65ms0.
20703IT=100138Pr83132141.
45m0.
051+03β+=100138Prm827831734823BD2.
12h0.
04703β+=100138Nd82018125.
04h0.
090+03β+=100138Ndm78843123174.
90.
4410ns50(10+)03IT=100138Pm749402710s21+#03β+=100138Pmm74911133030BD3.
24m0.
055#03β+=100138PmnnonexistentEU3.
24m0.
05(3+)81De38Iβ+=100138Sm71498123.
1m0.
20+03β+=100138Eu617502812.
1s0.
6(6)03β+=100138Gd55780#200#4.
7s0.
90+03β+=100138Gdm53550#200#2232.
71.
16s1(8)03138Tb43630#400#800#ms(>200ns)0300So11Iβ+;p=0138Dy34940#600#200#ms0+β+138LaDβ+=65.
65;β=34.
45138PmnD:argumentsforasecondisomer,ofintermediatespin,arenotconvincing138TbD:from93Li40139Sb50320#500#300#ms(>300ns)7/2+#0194Be24Iβ139Te60800#400#500#ms(>300ns)5/2#0194Be24Iβ;βn139I68840302.
282s0.
0107/2+#0193Ru01Tβ=100;βn=10.
03139Xe756442139.
68s0.
143/201β=100139Cs8070139.
27m0.
057/2+01β=100139Ba84913.
70.
483.
1m0.
3(7/2)01β=100139La87231.
42.
4STABLE7/2+01IS=99.
9101139Ce869527137.
641d0.
0203/2+01ε=100139Cem861987754.
240.
0856.
54s0.
1311/20194It.
ATIT=100139Pr8482384.
41h0.
045/2+01β+=100139Nd819922629.
7m0.
53/2+01β+=100139Ndm8176126231.
150.
055.
50h0.
2011/201β+=88.
24;IT=11.
84139Pm77496134.
15m0.
05(5/2)+01β+=100139Pmm7730713188.
70.
3180ms20(11/2)01IT≈100;β+=0.
16#139Sm72380112.
57m0.
101/2+01β+=100139Smm7192311457.
400.
2210.
7s0.
611/201IT=93.
75;β+=6.
35139Eu653981317.
9s0.
6(11/2)01β+=100139Gd57530#200#5.
7s0.
39/2#0199Xi04Tβ+=100;β+p=139Gdm57280#250#250#150#4.
8s0.
91/2+#01β+=100;β+p=139Tb48170#300#1.
6s0.
211/2#01β+=100;β+p139Dy37690#500#600ms2007/2+#01β+=100;β+p139IT:average93Ru01=2.
280(0.
011)80Al15=2.
29(0.
02)139GdT:average99Xi04=5.
8(0.
9)88Be.
A=5.
8(0.
4);other83Ni05=4.
9(1.
0)notused139GdT:sinceitcorrespondstoamixtureofground-stateandisomer139GdmD:assumingthatthedelayedprotonsreportedby83Ni05arefrombothstates78G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)140Te56960#300#300#ms(>300ns)0+9894Be24Iβ;βn140I64270#200#860ms40(3)(#)95β=100;βn=9.
310140Xe729906013.
60s0.
100+02β=100140Cs77051863.
7s0.
3195β=100140Ba83271812.
752d0.
0030+98β=100140La84321.
02.
41.
6781d0.
0003395β=100140Ce88083.
32.
5STABLE0+95IS=88.
45051140Cem85975.
52.
52107.
850.
037.
3s1.
56+140Pr8469563.
39m0.
011+95β+=100140Prm839326763.
30.
73.
05s0.
20(8)140Nd84252283.
37d0.
020+95ε=100140Ndm82031282221.
40.
1600s50795IT=100140Pm78210409.
2s0.
21+95β+=100140Pmm777831342040BD5.
95m0.
05895β+=100140Sm754561214.
82m0.
120+95β+=100140Eu66990501.
51s0.
021+95β+=100140Eum667805021015125ms25#95ABBWEIT≈100;β+300ns)5/2#0194Be24Iβ;βn141I60520#200#430ms207/2+#01β=100;βn=213141Xe68330901.
73s0.
015/2(#)01β=100;βn=0.
0445141Cs744771124.
84s0.
167/2+01β=100;βn=0.
0353141Ba79726818.
27m0.
073/201β=100141La8293853.
92h0.
03(7/2+)01β=100141Ce85440.
12.
532.
508d0.
0137/201β=100141Pr86020.
92.
5STABLE5/2+01IS=100.
141Nd8419842.
49h0.
033/2+01β+=100141Ndm834414756.
510.
0562.
0s0.
811/20170Ab05DIT≈100;β+=0.
0328141Pm805231420.
90m0.
055/2+01β+=100141Pmm7989514628.
400.
10630ns2011/201IT=100141Sm75939910.
2m0.
21/2+01β+=100141Smm757639176.
00.
322.
6m0.
211/201β+≈100;IT=0.
313141Eu699271340.
7s0.
75/2+01β+=100141Eum698311396.
450.
072.
7s0.
311/201IT=863;β+=143141Gd632242014s4(1/2+)01β+=100;β+p=0.
031141Gdm6284620377.
80.
224.
5s0.
5(11/2)01β+=892;IT=112141Tb545401103.
5s0.
2(5/2)01β+=100141Tbm54540#230#0#200#EU7.
9s0.
611/2#0188Be.
AIβ+=100141Dy45320#300#900ms200(9/2)01β+=100;β+p=141Ho34370#500#4.
1ms0.
3(7/2)02p=;β+=1#141Hom34300#500#6626.
4s0.
8(1/2+)0201Se03ETp=100141TbmI:existencediscussedin88Be.
A.
Provisionallyaccepted141HomT:from01Se03=6.
5(+0.
7–0.
9)G.
Audietal.
/NuclearPhysicsA729(2003)3–12879NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)142Te47430#600#50#ms(>300ns)0+0094Be24Iβ142I55720#400#200ms2#00β=100;βn=25#142Xe654801001.
22s0.
020+0003Be05TDβ=100;βn=0.
363142Cs70515111.
689s0.
01100093Ru01Tβ=100;βn=0.
0904142Ba77823610.
6m0.
20+00β=100142La80035691.
1m0.
5200β=100142Ce84538.
53.
0STABLE(>50Py)0+00IS=11.
11451;α;2β142Pr83792.
72.
519.
12h0.
04200β≈100;ε=0.
01648142Prm83789.
02.
53.
6940.
00314.
6m0.
5500IT=100142Nd85955.
22.
3STABLE0+00IS=27.
25142Pm811572540.
5s0.
51+00β+=100142Pmm8027425883.
170.
162.
0ms0.
2(8)00IT=100142Sm78993672.
49m0.
050+00β+=100142Eu71320302.
36s0.
101+0091Fi03Tβ+=100142Eum708561246030BD1.
223m0.
008800β+=100142Gd669602870.
2s0.
60+00β+=100142Tb57060#300#597ms171+00β+=100;β+p=0.
002211142Tbm56780#300#280.
21.
0303ms17(5)00IT≈100;β+260Py142EuT:average91Fi03=2.
34(0.
12)75Ke08=2.
4(0.
2)143I51640#400#100#ms(>300ns)7/2+#0294Be24Iβ;βn=40#143Xe60450#200#511ms65/20203Be05TDβ=100;βn=1.
0015143Cs67671241.
791s0.
0073/2+02β=100;βn=1.
647143Ba739361314.
5s0.
35/202β=100143La781871514.
2m0.
1(7/2)+02β=100143Ce81612.
03.
033.
039h0.
0063/202β=100143Pr83073.
52.
613.
57d0.
027/2+02β=100143Nd84007.
42.
3STABLE7/202IS=12.
22143Pm829663265d75/2+02ε=100;e+200ns)11/2#0100So11Iβ+143Er31350#600#200#ms9/2#β+143GdD:78Fi02:β+pand/orβ+αfor143Gd+143Gdm=0.
001%,39particlesdetected143DyT:others:84Ni03=3.
2(0.
6)83Ni05=4.
1(0.
3)intwodifferentexperiments80G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)144I46580#500#50#ms(>300ns)1#0194Be24Iβ;βn=40#144Xe57280#300#388ms70+0103Be05TDβ=100;βn=3.
03144Cs6327026994ms41(#)01β=100;βn=3.
2021144Csm62970#200#300#200#3)01β=;IT144Ba717691311.
5s0.
20+01β=100144La748905040.
8s0.
4(3)01β=100144Ce804373284.
91d0.
050+01β=100144Pr80756317.
28m0.
05001β=100144Prm80697359.
030.
037.
2m0.
3301IT≈100;β=0.
07144Nd83753.
22.
32.
29Py0.
160+01IS=23.
83;α=100144Pm814213363d1450194Hi05Dε=100;e+200ns)0+0100So11Iβ+144BaD:βn=3.
67inENSDF'01belongsinfactto144Cs145Xe52100#300#188ms43/2#9703Be05TDβ=100;βn=5.
06145Cs6005711582ms63/2+9393Ru01TDβ=100;βn=14.
38145Ba67410704.
31s0.
165/298β=100145La729909024.
8s2.
0(5/2+)9896Ur02Jβ=100145Ce77100403.
01m0.
06(3/2)93β=100145Pr7963275.
984h0.
0107/2+93β=100145Nd81437.
12.
3STABLE7/293IS=8.
31145Pm81274317.
7y0.
45/2+93ε=100;α=2.
8e–7145Sm80657.
72.
8340d37/202ε=100145Smm71871.
52.
98786.
20.
7990ns170(49/2+)02IT=100145Eu7799845.
93d0.
045/2+93β+=100145Eum772824716.
00.
3490ns11/293IT=100145Gd729271923.
0m0.
41/2+01β+=100145Gdm7217819749.
10.
285s311/201IT=94.
35;β+=5.
75145Tb658806020#m(3/2+)9693To04Jβ+145Tbm65880#120#0#100#30.
9s0.
7(11/2)9693Al03Tβ+=100145Dy58290509.
5s1.
0(1/2+)9393Al03Tβ+=100;β+p=145Dym5817050118.
20.
214.
1s0.
7(11/2)9393To04Tβ+=100145Ho49180#300#2.
4s0.
1(11/2)93β+=100145Hom49080#320#100#100#100#ms5/2+#β+;IT145Er39690#400#900ms3001/2+#98β+=100;β+p=145Tm27880#400#3.
1s0.
3(11/2)0298Ba13TJp=100145CsT:average93Ru01=579(6)82Ra13=594(13)145TbmT:average93Al03=31.
6(0.
6)82No08=29.
5(1.
0)and82Al07=29.
5(1.
5)145DyT:average93Al03=10.
5(1.
5)93To04=6(2)and84Sc.
C=10(1)145DymT:average93To04=14.
5(1.
0)82No08=13.
6(1.
0)145TmT:average03Ka04=3.
1(0.
3)98Ba13=3.
5(1.
0)J:notadoptedbyENSDF'02G.
Audietal.
/NuclearPhysicsA729(2003)3–12881NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)146Xe48670#400#146ms60+9703Be05TDβ=100;βn=6.
915146Cs5562070323ms619793Ru01Tβ=100;βn=14.
25146Ba65000702.
22s0.
070+9793Ru01Dβ=100146La69120706.
27s0.
1029793Ru01Dβ=100146Lam6899015013013010.
0s0.
1(6)9779Ke02Eβ=100146Ce756807013.
52m0.
130+97β=100146Pr767106024.
15m0.
18(2)97β=100146Nd80931.
12.
3STABLE0+97IS=17.
23;2β;α146Pm7946055.
53y0.
05399ε=66.
013;β=34.
013146Sm810024103My50+97α=100146Eu7712264.
61d0.
03497β+=100146Eum764566666.
370.
16235s39+97IT=100146Gd76093548.
27d0.
100+01ε=100146Tb67770508s41+97β+=100146Tbm67620#110#150#100#24.
1s0.
559793Al03Tβ+=100146Tbn66840#110#930#100#1.
18ms0.
02(10+)97IT=100146Dy625542733.
2s0.
70+9793Al03Tβ+=100146Dym59618272935.
70.
6150ms2010+#97IT=100146Ho51570#200#3.
6s0.
3(10+)97β+=100;β+p=146Er44710#300#1.
7s0.
60+9793To05Dβ+=100;β+p=146Tm31280#400#240ms30(6)02p≈100;β+146Tmm31200#400#716p72ms23(10+)02p=;β+=16#146CsT:average93Ru01=321(2)76Lu02=343(7)146BaD:93Ru01βn3.
0Ey)0+0082Be20TIS=5.
71;2β;α148Pm7687265.
368d0.
002100β=100148Pmm767346137.
90.
341.
29d0.
115,600β=95.
86;IT=4.
26148Sm79342.
22.
47Py30+00IS=11.
2410;α=100148Eu763021054.
5d0.
5500β+=100;α=9.
4e–728148Gd76275.
82.
874.
6y3.
00+00α=100;2β+148Tb705401460m1200β+=100148Tbm704501490.
10.
32.
20m0.
05(9)+00β+=100148Tbn61921148618.
61.
01.
310s0.
007(27+)00IT=100148Dy67859113.
3m0.
20+00β+=100148Ho580201302.
2s1.
1(1+)00β+=100148Hom57620#160#400#100#9.
49s0.
12(6)0093Al03Tβ+=100;β+p=0.
081148Hon57330#160#690#100#2.
35ms0.
04(10+)00IT=100148Er51650#200#4.
6s0.
20+00β+=100;β+p≈0.
15148Tm39270#400#700ms200(10+)00β+=100148Yb30350#600#250#ms0+β+148PrmE:derivedfromENSDFestimateE50ms)3/2+#9587Ra12Iβ;βn149Ba53490#200#344ms73/2#95β=100;βn=0.
4312149La60800#320#1.
05s0.
035/2+#9593Ru01Dβ=100;βn=1.
43149Ce667001005.
3s0.
23/2#98β=100149Pr71060802.
26m0.
07(5/2+)95β=100149Nd74380.
92.
81.
728h0.
0015/295β=100149Pm76071453.
08h0.
057/2+95β=100149Pmm758314240.
2140.
00735s311/2149Sm77141.
92.
4STABLE(>2Py)7/295IS=13.
827;α149Eu76447493.
1d0.
45/2+95ε=100149Gd7513349.
28d0.
107/201β+=100;α=4.
3e–410149Tb7149644.
118h0.
0251/2+99β+=83.
317;α=16.
717149Tbm71460435.
780.
134.
16m0.
0411/299β+≈100;α=0.
0223149Dy6771594.
20m0.
147/2()9588Ah02Jβ+=100149Dym6505492661.
10.
4490ms15(27/2)95IT=99.
33;β+=0.
73149Dyn602303074903028ns2(47/2+)95IT=100149Ho616881821.
1s0.
2(11/2)95β+=100149Hom616391848.
800.
2056s3(1/2+)95β+=100149Er53742284s2(1/2+)95β+=100;β+p=72149Erm5300028741.
80.
28.
9s0.
2(11/2)95β+=96.
57;IT=3.
57;.
.
.
149Tm44040#300#900ms200(11/2)95β+=100;β+p=0.
2615149Yb33500#500#700ms200(1/2+,3/2+)9501Xu06TDβ+=100;β+p=149DynE:7409.
9abovelevelat≈80keV149ErmDβ+p=0.
187150Cs38960#300#100#ms(>50ms)9787Ra12Iβ;βn150Ba50600#400#300ms0+95β=100;βn150La57040#400#510ms30(3+)9795Ok02TJβ=100;βn=2.
73150Ce64820504.
0s0.
60+95β=100150Pr68304266.
19s0.
16(1)96β=100150Nd7369036.
7Ey0.
70+9697De40TDIS=5.
62;2β=100150Pm73603202.
68h0.
02(1)95β=100.
.
.
A-groupiscontinuedonnextpage.
.
.
G.
Audietal.
/NuclearPhysicsA729(2003)3–12883NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
150Sm77057.
32.
4STABLE0+96IS=7.
381150Eu74797636.
9y0.
95()95β+=100150Eum74755642.
10.
512.
8h0.
1095β=892;β+=112;150Gd7576961.
79My0.
080+96α=100;2β+150Tb7111183.
48h0.
16(2)96β+≈100;α200ns)0+9700So11Iβ+150Lu24940#500#46ms6(5,6)0200Gi01Jp=;β+=30#150Lum24900#500#3415p80s60(1+,2+)0200Gi01Jp≈100;β+150NdT:from6.
75(+0.
37–0.
68statistics+0.
68systematics)150EumDIT≤5e–8150HoT:average93Al03=78(2)82No08=72(4)150TmmT:average96Ga24=2.
22(0.
07)88Ni02=2.
15(0.
10)and87To05=2.
2(0.
2)150TmmT:82No08=3.
5(0.
6)atvariance,notusedD:from88Ni02150TmnE:671.
6keVabove150Tmm,fromENSDF151Cs35220#500#60#ms(>50ms)3/2+#9787Ra12Iβ;βn151Ba45820#400#200#ms(>300ns)3/2#9794Be24Iβ151La54290#400#300#ms(>300ns)5/2+#9794Be24Iβ151Ce615001001.
02s0.
063/2#97β=100151Pr667712318.
90s0.
07(3/2)(#)97β=100151Nd70953312.
44m0.
073/2+97β=100151Pm73395528.
40h0.
045/2+97β=100151Sm74582.
52.
490y85/297β=100151Smm74321.
42.
4261.
130.
041.
4s0.
1(11/2)97IT=100151Eu74659.
12.
5STABLE5/2+97IS=47.
813151Eum74462.
92.
5196.
2450.
01058.
9s0.
511/297151Gd741954124d17/297ε=100;α=1.
0e–66151Tb71630517.
609h0.
0011/2(+)99β+≈100;α=0.
009515151Tbm71530599.
540.
0625s3(11/2)99IT=93.
84;β+=6.
24151Dy68759417.
9m0.
37/2()99β+=;α=5.
64151Ho636321235.
2s0.
111/2()9787Ne.
AJβ+=;α=223151Hom635911241.
00.
247.
2s1.
01/2(+)9787Ne.
AJα=7718;β+151Er582661623.
5s1.
3(7/2)97β+=100151Erm55681162585.
50.
6580ms20(27/2)97IT=95.
33;β+=4.
73151Tm5078220&4.
17s0.
10(11/2)97β+=100151Tmm5069021927AD&6.
6s1.
4(1/2+)97β+=100151Tmn48126202655.
670.
22451ns24(27/2)97IT=100151Yb415403001.
6s0.
5(1/2+)9786To12Tβ+=100;β+p=151Ybm40790#320#750#100#1.
6s0.
5(11/2)9786To12TDβ+≈100;β+p=;IT=0.
4#151Ybn39750#580#1790#500#2.
6s0.
719/2#97IT=100151Ybp39090#580#2450#500#20s127/2#97IT=100151Lu30200#400#80.
6ms1.
9(11/2)0293Se04Dp=;β+=37#151Lum30130#400#775p16s1(3/2+)02p=;β+151YbT:derivedfrom1.
6(0.
1),formixtureofground-stateandisomerwithalmostsamehalf-life151YbmE:740#estimatedby90Ak01(seeENSDF'97)151YbnE:1791.
2keVabove151Ybm(seeENSDF'97)151YbpE:2448keVabove151Ybm(seeENSDF'97)151LuD:p=63.
4(0.
9)%inENSDF'02,basedonpredictedbeta-decayhalf-life≈220ms84G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)152Ba42600#500#100#ms0+97β152La50070#400#200#ms(>300ns)9794Be24Iβ152Ce59110#200#1.
1s0.
30+9790Ta07Tβ=100152Pr638101203.
63s0.
124+9799To04Jβ=100152Nd701582511.
4m0.
20+97β=100152Pm71262264.
12m0.
081+97β=100152Pmm711208014090BD7.
52m0.
08497β=100152Pmn71010#150#250#150#13.
8m0.
2(8)97β≈100;IT=152Sm74768.
82.
5STABLE0+97IS=26.
7516152Eu72894.
52.
513.
537y0.
006397β+=72.
13;β=27.
93152Eum72848.
92.
545.
59980.
00049.
3116h0.
0013097β=724;β+=284152Eun72746.
62.
5147.
860.
1096m1897IT=100152Gd74714.
22.
5108Ty80+97IS=0.
201;α=100;2β+152Tb707204017.
5h0.
1298β+=100;α300ns)5/2+#9894Be24Iβ153Ce55350#400#500#ms(>300ns)3/2#9894Be24Iβ153Pr616301004.
28s0.
115/2#98β=100153Nd673492731.
6s1.
0(3/2)98β=100153Pm70685115.
25m0.
025/298β=100153Sm72565.
82.
546.
284h0.
0043/2+98β=100153Smm72467.
42.
598.
370.
1010.
6ms0.
311/298IT=100153Eu73373.
52.
5STABLE5/2+98IS=52.
193153Gd72889.
82.
5240.
4d1.
03/298ε=100153Gdm72794.
62.
595.
17370.
00123.
5s0.
4(9/2+)98IT=100153Gdn72718.
62.
5171.
1890.
00576.
0s1.
4(11/2)98IT=100153Tb7132042.
34d0.
015/2+98β+=100153Tbm711574163.
1750.
005186s411/298IT=100153Dy6915056.
4h0.
17/2()99β+≈100;α=0.
009414153Ho6501962.
01m0.
0311/298β+≈100;α=0.
05125153Hom64950668.
70.
39.
3m0.
51/2+98β+≈100;α=0.
188153Er60488937.
1s0.
27/2()9885Ah.
1Jα=533;β+=473153Tm54015181.
48s0.
01(11/2)98α=913;β+=93153Tmm539721843.
20.
22.
5s0.
2(1/2+)98α=923;β+=153Yb47060#200#4.
2s0.
27/2#9888Wi05Dβ+=;α=50#153Ybm44360#220#270010015s1(27/2)98153Lu38410210900ms20011/29897Ir01Dα=70#;β+=;p=0153Lum383302108051#s1/2+9897Ir01EDβ+;α;p=0153Lun357802102632.
90.
515s327/298153Hf27300#500#400#ms(>200ns)1/2+#00So11Iβ+153Hfm26550#510#750#100#500#ms11/2#β+;IT153SmT:seealso99Sc12=46.
274(7)153ErJ:and89Ot.
A153YbDβ+p=0.
0082153YbmE:inENSDF2578.
2+x153LuD:pdecayisfrom97Ir01G.
Audietal.
/NuclearPhysicsA729(2003)3–12885NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)154La42380#600#100#msβ154Ce52700#500#300#ms(>300ns)0+9894Be24Iβ154Pr582001502.
3s0.
1(3+,2+)98β=100154Nd6569011025.
9s0.
20+98β=100154Ndm65210#190#480#150#1.
3s0.
598154Ndn64340110134910>1s(5)98154Pm6850040&1.
73m0.
10(0,1)98β=100154Pmm68380110120120BD&2.
68m0.
07(3,4)98β=100154Sm72461.
62.
5STABLE(>2.
3Ey)0+98IS=22.
7529;2β154Eu71744.
42.
58.
593y0.
004398β≈100;ε=0.
021154Eum71599.
12.
5145.
30.
346.
3m0.
4(8)98IT=100154Gd73713.
22.
5STABLE0+98IS=2.
183154Tb701605021.
5h0.
40(+#)98β+≈100;β256235s3(17+)98IT=100154Hf32730#500#2s10+98β+≈100;α≈0154TbmDβ300ns)5/2#9794Be24Iβ155Pr55780#300#1#s(>300ns)5/2#9795Cz.
AIβ155Nd62470#150#8.
9s0.
23/2#94β=100155Pm669703041.
5s0.
2(5/2)94β=100155Sm70197.
22.
622.
3m0.
23/294β=100155Eu71824.
52.
54.
7611y0.
00135/2+94β=100155Gd72077.
12.
5STABLE3/297IS=14.
8012155Gdm71956.
12.
5121.
050.
1932.
0ms0.
311/297IT=100155Tb71254125.
32d0.
063/2+94ε=100155Dy69160129.
9h0.
23/299β+=100155Dym6892612234.
330.
036s11/299IT=100155Ho660401848m15/2+94β+=100155Hom6589818141.
970.
11880s8011/294IT=100155Er6221575.
3m0.
37/294β+≈100;α=0.
0227155Tm566351321.
6s0.
2(11/2)95β+=98.
13;α=1.
93155Tmm565941441645s3(1/2+)95β+>92;α300ns)95Cz.
AIβ156Nd605302005.
49s0.
070+03β=100156Ndm5910020014325135ns503IT=100156Pm642203026.
70s0.
10403β=100156Sm69370109.
4h0.
20+03β=100156Smm67972101397.
550.
09185ns7503IT=100156Eu70093615.
19d0.
080+03β=100156Gd72542.
22.
5STABLE0+03IS=20.
479156Gdm70404.
62.
52137.
600.
051.
3s0.
1703IT=100156Tb7009845.
35d0.
10303β+≈100;β156Tbm70044554324.
4h1.
0(7)03IT=100156Tbn70010488.
40.
25.
3h0.
2(0+)03IT=;β+=156Dy705307STABLE(>1Ey)0+0358Ri23TIS=0.
061;α;2β+156Ho653504056m1403β+=100156Hom653004052.
40.
59.
5s1.
5103IT=;β+156Hon65250#60#100#50#7.
8m0.
3(9+)03β+=75;IT156Er642132419.
5m1.
00+03β+=100;α=17e–64156Tm568401683.
8s1.
8203β+≈100;α=0.
06410156Tmm5663616203.
60.
5400ns(11)03IT=100156TmnnonexistentRN19s39+0391To08I156Yb532641126.
1s0.
70+03β+=902;α=102156Lu4375070494ms12(2)03α=;β+=5#156Lum43530#110#220#80#198ms2(9)+0396Pa01Dα=946;β+156Hf3785021023ms10+0396Pa01Dα=973;β+156Hfm358902101959.
01.
0AD480s408+0396Pa01Tα=100156Ta25800#400#144ms24(2)03p≈100;β+156Tam25700#400#1008AD360ms40(9+)03β+=95.
89;p=4.
29156TbmE:derivedfromE324hto4+49.
630levelandE(IT)300ns)5/2#9795Cz.
AIβ157Pm6237011010.
56s0.
10(5/2)96β=100157Sm66730508.
03m0.
07(3/2)96β=100157Eu69467515.
18h0.
035/2+96β=100157Gd70830.
72.
5STABLE3/296IS=15.
652157Tb70770.
62.
571y73/2+96ε=100157Dy6942878.
14h0.
043/297β+=100157Dym692297199.
380.
0721.
6ms1.
611/297IT=100157Ho668292412.
6m0.
27/296β+=100157Er634202818.
65m0.
103/296β+=100157Erm6326528155.
40.
376ms6(9/2+)96IT=100157Tm58709283.
63m0.
091/2+97β+=100157Yb534421038.
6s1.
07/296β+=99.
5;α=0.
5157Lu46483196.
8s1.
8(1/2+,3/2+)96β+;α=157Lum464621921.
02.
0AD4.
79s0.
12(11/2)96β+=;α=62157Hf38750#200#115ms17/29696Pa01Tα=869;β+=149157Ta2963021010.
1ms0.
41/2+02α=;p=3.
412;157Tam296102102254.
3ms0.
111/202α=;β+=1#;p=0157Tan2804021015939AD1.
7ms0.
1(25/2)02α=100157DymT:asadoptedbyENSDFevaluatorfrom3inconsistentresults157LuT:ENSDF'96averageofverydiscrepant91To09=5.
7(0.
5)91Le15,92Po14=9.
6(8)157TaDβ+=1#G.
Audietal.
/NuclearPhysicsA729(2003)3–12887NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)158Pr44730#600#200#msβ158Nd54400#400#700#ms(>300ns)0+9795Cz.
AIβ158Pm590901304.
8s0.
596β=100158Sm65210805.
30m0.
030+96β=100158Eu672108045.
9m0.
2(1)96β=100158Gd70696.
82.
5STABLE0+96IS=24.
847158Tb69477.
22.
6180y11396β+=83.
47;β=16.
67158Tbm69366.
92.
9110.
31.
210.
70s0.
17096IT≈100;β81;β+93;IT31Ey)0+9701Da22TIS=21.
8619;2β160Tb67842.
92.
672.
3d0.
2397β=100160Dy69678.
12.
5STABLE0+97IS=2.
348160Ho663881525.
6m0.
35+97β+=100160Hom663281559.
980.
035.
02h0.
05297IT=653;β+=353160Hon6619122197163s(9+)97ABBWEIT=100160Er660582428.
58h0.
090+97ε=100160Tm60300309.
4m0.
3197β+=100160Tmm6023040702074.
5s1.
55(+#)97IT=855;β+=155160Yb58170174.
8m0.
20+97β+=100160Lu502706036.
1s0.
32#97β+=100;α140Ty)0+9956Po16TIS=0.
141;α;2β+162Tm614842621.
70m0.
19199β+=100162Tmm61350501304024.
3s1.
75+99ABBWEIT;β+=184162Yb598321618.
87m0.
190+99β+=100162Lu52840801.
37m0.
021()9998Ge13Jβ+=100162Lum52720#220#120#200#1.
5m4#99β+≈100;IT162Lun52540#220#300#200#1.
9m99β+≈100;IT162Hf491731039.
4s0.
90+99β+≈100;α=0.
0081162Ta39780503.
57s0.
123+#99β+≈100;α=0.
07410162W34002181.
36s0.
070+99β+;α=45.
216162Re22350#200#107ms13(2)99α=946;β+162Rem22180#200#17310AD77ms9(9+)99α=915;β+162Os14500#500#1.
87ms0.
180+9900Ma95Tα=100162HomE:about10keVabovelevelat96.
1(0.
1),fromENSDF;errorfromNUBASE162ErT:lowerlimitisforαdecay162TmmE:above66.
90levelandlessthan192keV,fromENSDF162OsT:average00Ma95=1.
9(0.
2)96Bi07=1.
5(+0.
7–0.
5)89Ho12=1.
9(0.
7)163Pm43150#800#200#ms5/2#β163Sm50900#700#1#s1/2#β163Eu56630#500#6#s5/2+#β163Gd61490#300#68s37/2+#00β=100163Tb64601519.
5m0.
33/2+00β=100163Dy66386.
52.
5STABLE5/200IS=24.
9016163Ho66383.
92.
54.
570ky0.
0257/200ε=100163Hom66086.
02.
5297.
880.
071.
09s0.
031/2+00IT=100163Er65174575.
0m0.
45/200β+=100163Erm647295445.
50.
6580ns100(11/2)00IT=100163Tm6273561.
810h0.
0051/2+00β+=100163Yb593041611.
05m0.
253/200β+=100163Lu54791283.
97m0.
131/2(+)01β+=100163Hf492862840.
0s0.
63/2#00β+=100;α60;β+80;IT1m1/2(#)00IT;β+167Hf53468282.
05m0.
05(5/2)00β+=100167Ta48351281.
33m0.
07(3/2+)00β+=100167W420891919.
9s0.
53/2#00β+=99.
961;α=0.
041167Re34840#50#&3.
4s0.
49/2#00α≈100;β+167Rem3471040130#40#&5.
9s0.
31/2+#00β+≈99;α≈1167Os2650070810ms603/2#00α=578;β+=438167Ir170791935.
2ms2.
01/2+02α=486;p=324;β+167Irm1690319175.
32.
2p30.
0ms0.
611/202α=8010;β+167Pt6540#410#700s2007/2#00α=100167WJ:lowestobservedstateby92Th06is13/2+167IrmDp=0.
4192G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)168Gd48100#700#300#ms0+85Si25Iβ168Tb52500#500#8.
2s1.
34#99β=100168Dy585601408.
7m0.
30+99β=100168Ho60070302.
99m0.
073+94β=100168Hom6001030591132s4(6+)9490Ch37EIT≈100;β130Ty)0+9456Po16TIS=0.
131;α;2β+168Lu57060505.
5m0.
16()9498Ge13Jβ+=100168Lum56880100180110BD6.
7m0.
43+94β+>95;IT320Py)0+0296De60TIS=14.
9327;170Tm59800.
62.
5128.
6d0.
3102β≈100;ε=0.
13110170Tmm59617.
42.
5183.
1970.
0044.
12s0.
13(3)+02IT=100170Yb60769.
02.
4STABLE0+02IS=3.
0415170Ybm59510.
52.
41258.
460.
14370ns15402IT=100170Lu57310172.
012d0.
0200+02β+=100170Lum572171792.
910.
09670ms100(4)02IT=100170Hf562542816.
01h0.
130+02ε=100170Ta50138286.
76m0.
06(3)(+#)02β+=100170W47293152.
42m0.
040+02β+≈100;α93;α160Py)0+9896De60TIS=12.
7641;176Ybm52444.
12.
61050.
00.
311.
4s0.
3(8)98IT=;β40178Hg1631713269ms30+9402Ro17Tα=;β+=30#178Tl4750#110#255ms1002Ro17TDα=;β+=47#178Pb356824230s1500+01Ro.
BTα≈100;β+178TanE:1470.
6keVabove178Tam,fromENSDF178TanT:average96Ko13=58(4)79Du02=60(5)178TapE:2902keVabovethe(7)178Tamisomer178HgT:others96Pa01=287(23)91Se01=250(25)and79Ha10=260(30)178PbT:twoeventsat202and147s179Tm41600#500#20#s1/2+#β179Yb46420#300#8.
0m0.
4(1/2)94β=100179Lu4906454.
59h0.
067/2(+)94β=100179Lum484725592.
40.
43.
1ms0.
91/2(+)94IT=100179Hf50471.
92.
1STABLE9/2+94IS=13.
622179Hfm50096.
92.
1375.
03670.
002518.
67s0.
041/294IT=100179Hfn49366.
12.
11105.
840.
1925.
05d0.
2525/294IT=100179Ta50366.
32.
21.
82y0.
037/2+00ε=100179Tam49049.
02.
21317.
30.
49.
0ms0.
2(25/2+)00IT=100179Tan47727.
02.
32639.
30.
554.
1ms1.
7(37/2+)00IT=100179W493041637.
05m0.
16(7/2)94β+=100179Wm4908216221.
9260.
0086.
40m0.
07(1/2)94IT≈100;β+=0.
283179Re465862419.
5m0.
1(5/2)+95β+=100179Rem465212465.
390.
0995s25(5/2)179Os43020186.
5m0.
3(1/2)94β+=100179Ir380771179s1(5/2)98β+=100179Pt32264921.
2s0.
41/294β+≈100;α=0.
243179Au24952177.
1s0.
35/2#94β+=78.
09;α=22.
09179Aup24853189916AD(11/2)179Hg16922271.
09s0.
045/2#9402Ro17Tα≈53;β+=;β+p≈0.
15179Tl830040270ms30(1/2+)01ABBWJα=;β+=30#179Tlm7440#50#860#30#1.
60ms0.
16(9/2)0102Ro17Tα≈100;IT;β+179Pb2000#200#3#ms5/2#α179HgT:average02Ro17=1.
08(0.
09)71Ha03=1.
09(0.
04)179TlT:average02Ro17=415(55)98To14=230(40)83Sc24=160(+90–40)179TlJ:fromαdecayto175Aum179TlmT:average02Ro17=1.
7(0.
2)98To14=1.
8(0.
4)96Pa01=0.
7(+6–4)83Sc24=1.
4(0.
5)98G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)180Yb44400#400#2.
4m0.
50+94β=100180Lu46690705.
7m0.
15+9495Me03Jβ=100180Lum466807013.
90.
31s395Me03EJTβ;IT180Hf49788.
42.
1STABLE0+94IS=35.
0816180Hfm48646.
92.
11141.
480.
045.
5h0.
1894IT≈100;β=0.
31180Ta48936.
22.
28.
152h0.
0061+94ε=863;β=143180Tam48860.
91.
875.
31.
3RQSTABLE(>1.
2Py)994IS=0.
0122;β180Tan47485.
22.
41451.
01.
045s21596Dr02TE180W496444STABLE(>700Py)0+9403Da05TIS=0.
121;α;2β+180Wm4811541529.
040.
035.
47ms0.
09894IT=100180Re45840212.
44m0.
06(1)94β+=100180Os443592021.
5m0.
40+94β+=100180Ir37978221.
5m0.
1(4,5)(+#)94β+=100180Pt344361152s30+94β+≈100;α≈0.
3180Au25596218.
1s0.
394β+≤98.
2;α≥1.
8180Hg20245142.
56s0.
020+9493Wa03Tβ+=524;α=484180Tl9400#120#1.
5s0.
29498To14TDβ+;α=73;180Pb1939215ms30+0096To08TDα=100180WT:lowerlimitisforαdecay,also03Ce01>270Py97Ge15>74Py180WT:indicationin03Da05for1.
1(+0.
8–0.
4)Ey,butimportantbackground180WT:03Da09>80Pyfor2βdecay180TlDβ+SF≈1.
0e–4180TlD:α=(2-12)%from02An.
A181Yb40850#400#1#m3/2#β181Lu44740#300#3.
5m0.
3(7/2+)91β=100181Hf47411.
92.
142.
39d0.
061/291β=100181Hfm468174595380s5(9/2+)01Sh36ETJIT=100181Hfn4637210104010100s(17/2+)01Sh36ETJIT=100181Hfp45674101738101.
5ms0.
5(27/2)01Sh36ETJIT=100181Ta48441.
61.
8STABLE7/2+92IS=99.
9882181Tam48435.
41.
86.
2380.
0206.
05s0.
129/292IT=100181Tan4695731485325s221/298Wh02ETJIT=100181Tap46212322303210s2029/298Wh02ETJIT=100181W482545121.
2d0.
29/2+91ε=100181Re465111319.
9h0.
75/2+91β+=100181Os4355030105m31/292β+=100181Osm435003048.
90.
22.
7m0.
1(7/2)9295Ro09Eβ+=100181Ir39472264.
90m0.
15(5/2)93β+=100181Pt343751552.
0s2.
21/29995Bi01Dβ+≈100;α=0.
07410181Au278712013.
7s1.
4(3/2)99β+=;α=2.
75181Hg20661153.
6s0.
11/2()99β+=695;α=315;181Hgp20460#40#210#40#13/2+181Tl1280193.
2s0.
31/2+#9198To14TDα=;β+181Tlm119442985729AD1.
7ms0.
49/2#98To14TDβ+;α=;IT181Pb314090&45ms205/2#96To01Tα=;β+=2#181PbmnonexistentRN&13/2+#9196To01I181HgDβ+p=0.
0164;β+α=11e–64181TlT:average98To14=3.
2(0.
3)92Bo.
D=3.
4(0.
6)181TlmT:average98To14=1.
4(0.
5)84Sc.
A=2.
7(1.
0)181PbT:supersedes89To01=50(+40–30)fromsamegroup181PbmI:provedby96To01nottoexistG.
Audietal.
/NuclearPhysicsA729(2003)3–12899NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)182Lu41880#200#2.
0m0.
2(0,1,2)95β=100182Hf4605969My20+95β=100182Hfm4488661172.
880.
1861.
5m1.
5895β=583;IT=423182Ta46433.
31.
8114.
43d0.
03395β=100182Tam46417.
01.
816.
2630.
003283ms35+95IT=100182Tan45913.
71.
8519.
5720.
01815.
84m0.
101095IT=100182W48247.
50.
8STABLE(>170Ey)0+9503Da05TIS=26.
5016;α182Re4545010064.
0h0.
57+95β+=100182Rem453882060100BD12.
7h0.
22+95β+=100182Os446092222.
10h0.
250+95ε=100182Ir390522115m1(3+)9595Sa42Jβ+=100182Pt36169162.
2m0.
10+95β+≈100;α=0.
0382182Au283012015.
5s0.
4(2+)9501Ib02Jβ+≈100;α=0.
135182Hg235761010.
83s0.
060+9597Ba21Dβ+=86.
29;α=13.
89;182Tl13350802.
0s0.
32#9592Bo.
DTβ+>96;α25Ey97Ge15>8.
3Ey182AuT:average95Bi01=14.
5(1.
3)(forβ+),15.
3(1.
0)(forα)and92Ro21=15.
6(0.
4)182HgDβ+p80Ey)1/20103Da05TIS=14.
314;α183Wm46057.
50.
8309.
4930.
0035.
2s0.
311/2+01IT=100183Re45811870.
0d1.
45/2+99ε=100183Rem4390381907.
60.
31.
04ms0.
04(25/2+)99IT=100183Os436605013.
0h0.
59/2+91β+=100183Osm4349050170.
710.
059.
9h0.
31/291β+=852;IT=152183Ir401972558m55/29161Di04Tβ+≈100;α=0.
05#183Pt35772166.
5m1.
01/29395Bi01Dβ+≈100;α=0.
00965183Ptm357381634.
500.
0843s5(7/2)93β+≈100;α1s(1/2)+99IT=100183Aup2995610230.
60.
613Ey97Ge15>1.
9Ey183IrT:average61Di04=55(7)61La05=60(6)183HgDβ+p=2.
6e–48183HgmI:2001Sc41=noisomerseenwithsamecharacteristicsas185Hgor187Hg183HgmI:noisomerinsameodd-N181Ptand179Os183TlnE:346.
8(0.
3)keVabove183Tlm100G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)184Lu36410#400#20s3(3+)9095Kr04TJβ=100184LumnonexistentRN20shigh95Kr04I184Hf41500404.
12h0.
050+90β=100184Hfm40230401272.
40.
448s10895Kr04TEβ=100184Ta42841268.
7h0.
1(5)90β=100184W45707.
30.
9STABLE(>180Ey)0+9003Da05TIS=30.
642;α184Re44227438.
0d0.
53()90β+=100184Rem440394188.
010.
04169d88(+)90IT=75.
411;ε=24.
611184Os44256.
11.
3STABLE(>56Ty)0+90IS=0.
021;α;2β+184Ir39611283.
09h0.
03590β+=100184Irm3938528225.
650.
11470s3+184Pt373321817.
3m0.
20+9095Bi01Dβ+≈100;α=0.
00177184Ptm35493181839.
41.
61.
01ms0.
05890IT=100184Au303192220.
6s0.
95+03β+≈100;α20ns(10)84Sc.
ATIT184Pb1104514490ms250+0302An.
ADα=8015;β+184Bi1050#130#6.
6ms1.
53+#02An.
ATα=184Bim1200#160#150#100#13ms210#02An.
ATα=184WT:also03Ce01>29Ey97Ge15>4.
0Ey184OsT:lowerlimitisforαdecay184TlnT:alphadecayfrom188BimnotcoincidentwithX(K)andγ184TlnI:identiedby02Sc.
A185Hf38360#200#3.
5m0.
63/2#95β=100185Ta413961449.
4m1.
57/2+#95β=100185Tam4009030130829>1ms(21/2)99Wh03TJDIT=100185W43389.
70.
975.
1d0.
33/295β=100185Wm43192.
30.
9197.
430.
051.
597m0.
00411/2+9594It.
ATIT=100185Re43822.
21.
2STABLE5/2+95IS=37.
402185Rem41698.
22.
321242123ns23(21/2)97Sh37TIT=100185Os42809.
41.
393.
6d0.
51/295ε=100185Osm42707.
11.
5102.
30.
73.
0s0.
47/2#95IT185Ir403362814.
4h0.
15/295β+=100185Pt366804070.
9m2.
4(9/2+)95β+≈100;α=0.
005020185Ptm3658040103.
40.
233.
0m0.
8(1/2)95β+=;IT4.
1Ey)0+0303Da09TIS=28.
4319;2β;α186Wm40992.
31.
81517.
20.
618s1(7)03IT=100186Wn38966.
72.
73542.
82.
1>3ms(16+)03IT=100186Re41930.
21.
23.
7183d0.
0011103β=92.
5310;ε=7.
4710186Rem4178171497200ky50(8+)03IT=;β170Ey03Ce01>27Ey97Ge15>6.
5Eyforαdecay186WnT:lowerlimitis3ms;upperlimit30s186RemT:uncertaintyestimatedbyENSDF'89evaluator186IrmT:average91Be25=1.
90(0.
05)70Fi.
A=2.
0(0.
1)186IrmE:Eispositiveandbelow1.
5keV186TlI:identiedasdecaylevelfrom190Biin91Va04186TlnE:374.
0(0.
2)keVabove186Tlm186BiT:average02An.
A=14.
8(0.
8)97Ba21=15.
0(1.
7)187Hf32980#400#30#s(>300ns)3/2#99Be63Iβ187Ta36770#200#2#m(>300ns)7/2+#99Be63Iβ187W39904.
81.
723.
72h0.
063/292β=100187Re41215.
71.
441.
2Gy0.
25/2+9101Ga01TIS=62.
602;β=100;187Os41218.
21.
4STABLE1/292IS=1.
962187Ir39716610.
5h0.
33/2+91β+=100187Irm395306186.
150.
0430.
3ms0.
69/291IT=100187Pt36713282.
35h0.
033/291β+=100187Au33005258.
4m0.
31/2+91β+≈100;α=0.
003#187Aum3288425120.
510.
162.
3s0.
19/291IT=100187Hg2811814&1.
9m0.
33/291β+=100;α>1.
2e–4187Hgm28059205916MD&2.
4m0.
313/2+91β+=100;α>2.
5e–4187Tl22444851s(1/2+)99β+50;β+187Bim62721810120AD320s701/2+#01α>50;β+187Bin61211525217s5(13/2+)02Hu14ETJIT=100187ReDα300ns)0+0299Be63Iβ188Ta33810#200#20#s(>300ns)0299Be63Iβ188W38667369.
78d0.
050+02β=100188Re39016.
11.
417.
0040h0.
0022102β=100188Rem38844.
01.
4172.
0690.
00918.
59m0.
04(6)02IT=100188Os41136.
41.
4STABLE0+02IS=13.
248188Ir38328741.
5h0.
5102β+=100188Irm3736030970304.
2ms0.
27+#02ABBWEIT≈100;β+188Pt37823510.
2d0.
30+02ε=100;α=2.
6e–53188Au32301208.
84m0.
061()02β+=100188Hg30202123.
25m0.
150+02β+=100;α=3.
7e–58188Hgm27478122724.
30.
4134ns15(12+)02IT=100188Tl223503071s2(2)02β+=100188Tlm22307104030MD71s1(7+)02β+=100188Tln220381031030MD41ms4(9)02IT≈100;β+188Pb178151125.
5s0.
10+02β+=;α=9.
38188Pbm15237112578.
20.
7830ns210(8)02IT=100188Pbn15102112713.
00.
694ns(11)02IT=100188Pbp1502050280050797ns2102IT=100188Bi720050&44ms33+#0297Wa05Tα=;β+188Bim7000#150#210#140#&220ms40(10)0297Wa05Tα=;β+188Po53819430s1800+02α=;β+188IrmE:lessthan100keVabove923.
5level,fromENSDF188TlnE:268.
8(0.
5)keVabove188Tlm,from91Va04188PbpE:2700.
5aboveunknownlevel,seeENSDF'02188BiT:average97Wa05=46(7)84Sc.
A=44(3)188BimT:average97Wa05=218(50)84Sc.
A=210(90)189Ta31830#300#3#s(>300ns)7/2+#99Be63Iβ189W3548020011.
6m0.
3(3/2)9197Ya03Tβ=100189Re37978824.
3h0.
45/2+91β=100189Os38985.
41.
5STABLE3/291IS=16.
155189Osm38954.
61.
530.
8140.
0185.
8h0.
19/291IT=100189Ir384531313.
2d0.
13/2+91ε=100189Irm3808113372.
180.
0413.
3ms0.
311/291IT=100189Irn36120132333.
30.
43.
7ms0.
2(25/2)+91IT=100189Pt364831110.
87h0.
123/292β+=100189Ptm3629111191.
60.
4143s(13/2+)189Au335822028.
7m0.
31/2+92β+=100;α99;α≈0.
4189Pbm17840#50#40#30#1#m(13/2+)ABBWJβ+;IT189Bi1006050674ms11(9/2)9895Ba75Jα>50;β+50;β+360(120)G.
Audietal.
/NuclearPhysicsA729(2003)3–128103NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)190Ta28660#400#300#msβ190W3430016030.
0m1.
50+03β=100190Wm31920160238152s(4)+03IT=100190Irq36433.
61.
7317.
560.
0490ns(5)03IT=100190Pt373236650Gy300+03IS=0.
0141;α=100;.
.
.
190Au328811642.
8m1.
0103β+=100;α1s90391Va04ETIT190Pb204171271s10+03β+;α=0.
404190Pbm17802122614.
80.
8150ns(10)+03IT=100190Pbn177992326182025s(12+)03IT190Pbp17759122658.
20.
87.
2s0.
6(11)03IT=100190Bi109001806.
3s0.
1(3+)0391Va04Jα=7721;β+=190Bim1048310420180MD6.
2s0.
1(10)0391Va04Jα=709;β+190Bin1021010690180MD>500ns1007+#0301An11ETIT=100190Po4563132.
46ms0.
050+03α≈100;β+=0.
1#190RemE:fromlowerlimit119.
12andcalculated173and220(seeENSDF'90)190RemE:210(290)fromdifferenceinbeta-decay190PtD2β+190HgDα300ns)3/2#99Be63Iβ191Re34349109.
8m0.
5(3/2+,1/2+)95β=100191Os36393.
71.
515.
4d0.
19/295β=100191Osm36319.
31.
574.
3820.
00313.
10h0.
053/295IT=100191Ir36706.
41.
7STABLE3/2+95IS=37.
32191Irm36535.
21.
7171.
240.
054.
94s0.
0311/295IT=100191Irn34590402120405.
5s0.
795ABBWEIT=100191Pt3569842.
802d0.
0253/296ε=100191Ptm355494149.
040.
0295s13/2+191Au33810403.
18h0.
083/2+99β+=100191Aum3354040266.
20.
5920ms110(11/2)99IT=100191Hg305932349m103/2()0086Ul02Jβ+=100;α300ns)0+99Be63Iβ192Re31710#200#16s198β=100192Os35880.
52.
6STABLE(>9.
8Ty)0+98IS=40.
7819;2β;α192Osm33865.
12.
62015.
400.
115.
9s0.
1(10)98IT>87;β300ns)5/2+#99Be63Iβ193Os33392.
62.
630.
11h0.
013/298β=100193Ir34533.
81.
7STABLE3/2+98IS=62.
72193Irm34453.
61.
780.
2400.
00610.
53d0.
0411/298IT=100193Pt34477.
01.
750y61/298ε=100193Ptm34327.
21.
7149.
780.
044.
33d0.
0313/2+98IT=100193Au333941117.
65h0.
153/2+98β+=100;α300ns)99Be63Iβ194Os32432.
72.
66.
0y0.
20+96β=100194Ir32529.
31.
719.
28h0.
13196β=100194Irm32382.
21.
7147.
0780.
00531.
85ms0.
24(4+)96IT=100194Irn321607037070BD171d11(10,11)(#)96β=100194Pt34763.
10.
9STABLE0+96IS=32.
96799194Au322621038.
02h0.
10196β+=100194Aum3215510107.
40.
5600ms8(5+)96IT=100194Aun3178610475.
80.
6420ms10(11)96IT=100194Hg3219313440y800+01ε=100.
.
.
A-groupiscontinuedonnextpage.
.
.
G.
Audietal.
/NuclearPhysicsA729(2003)3–128105NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
194Tl2683014033.
0m0.
5299β+=100;α2.
5Ey)0+9890Bu28TIS=0.
151;2β+196Tl27497121.
84h0.
03298β+=100196Tlm2710312394.
20.
51.
41h0.
02(7+)98β+=95.
5;IT=4.
5196Pb253611437m30+01β+=100;α≤3e–5196Pbm23623141738.
270.
12320Ty)0+0252Fr23TIS=7.
16355;2β;α198Au29582.
10.
62.
69517d0.
00021202β=100198Aum29269.
90.
6312.
22000.
0020124ns45+02IT=100198Aun28770.
41.
6811.
71.
52.
27d0.
02(12)02IT=100198Hg30954.
40.
3STABLE0+02IS=9.
9720198Tl27490805.
3h0.
5202β+=100198Tlm2695080543.
50.
41.
87h0.
037+02β+=542;IT=462198Tln2675080742.
30.
432.
1ms1.
010#02IT=100198Pb26050152.
4h0.
10+02β+=100198Pbm23909152141.
40.
44.
19s0.
10(7)02IT=100198Bi193692810.
3m0.
3(2+,3+)02β+=100198Bim190852828040MD11.
6m0.
3(7+)02β+=100198Bin188372853040MD7.
7s0.
51002IT=100198Po15473171.
77m0.
030+02α=572;β+=432198Pom13619171853.
630.
1829ns28+02IT=100198Pon12907172565.
920.
20200ns201102IT=100198Pop12781172691.
860.
20750ns5012+02IT198At6670504.
2s0.
3(3+)0295Bi.
ADα>94;β+198Atm6340#70#330#90#1.
0s0.
2(10)0295Bi.
ADα>86;β+198Rn12311365ms30+02α=;β+=1#198RnmnonexistentEU50ms9α=;β+=;IT=198PtT:lowerlimitisfor0ν-2βdecay198BinE:248.
5(0.
5)keVabove198Bim,from92Hu04198RnmI:αdecayassignedtoisomerbyENSDF'95,notacceptedbyNUBASE199Ir244004020#s3/2+#01β199Pt27392330.
80m0.
215/294β=100199Ptm269684424213.
6s0.
4(13/2)+94IT=100199Au29095.
00.
63.
139d0.
0073/2+94β=100199Aum28546.
10.
6548.
93680.
0021440s30(11/2)94IT=100199Hg29547.
10.
4STABLE1/294IS=16.
8722199Hgm29014.
60.
4532.
480.
1042.
66m0.
0813/2+9401Li17TIT=100.
.
.
A-groupiscontinuedonnextpage.
.
.
G.
Audietal.
/NuclearPhysicsA729(2003)3–128107NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
199Tl28059287.
42h0.
081/2+94β+=100199Tlm2730928749.
70.
328.
4ms0.
29/294IT=100199Pb252282690m103/201β+=100199Pbm2479926429.
52.
712.
2m0.
3(13/2+)01ABBWEIT=93;β+=7199Pbn22664262563.
82.
710.
1s0.
2(29/2)01ABBWEIT=100199Bi207981227m19/294β+=100199Bim2013112667424.
70m0.
15(1/2+)94β+=;IT90;IT99;β+200ns1197IT=100202At1059128184s1(2,3)+97β+=;α=183202Atm104012819040MD182s2(7+)97IT;β+;α=8.
715202Atn100102858040MD460ms50(10)9792Hu04EIT≈100;β+=0.
25#202Rn6275189.
94s0.
180+9796Ta18Tα=;β+=14#202Fr314050290ms30(3+)9796En01Tα=;β+=3#202Frm3470#70#330#90#340ms40(10)97α=;β+=3#202Ra9210602.
6ms2.
10+9896Le09TDα=100202HgD:lowerhalf-lifelimitfor24NedecayT>3.
7Zy,from90Bu28202BiJ:re-evaluationtoapossible6+isdiscussedin96Ca02202AtnDα=0.
09611202AtnE:391.
7(0.
5)keVabove202Atm202RnT:average96Ta18=10.
3(0.
4)71Ho01=9.
85(0.
20)202FrT:average96En01=230(+80–40)95Bi.
A=300(40)203Au23143353s23/2+93β=100203Hg25269.
11.
746.
612d0.
0185/293β=100203Hgm24336.
02.
0933.
11.
024s(13/2+)203Tl25761.
21.
3STABLE1/2+93IS=29.
52414203Tlm2236030034003007.
7s0.
5(25/2+)98Pf02TJIT=100203Pb24787751.
873h0.
0095/293ε=100203Pbm239627825.
200.
096.
3s0.
213/2+93IT=100203Pbn2183872949.
470.
22480ms2029/293IT=100203Bi215402211.
76h0.
059/293β+=100;α≈1e–5203Bim20442221098.
140.
07303ms51/2+93IT=100203Po173072636.
7m0.
55/293β+≈100;α=0.
112203Pom1666626641.
490.
1745s213/2+93IT≈100;α=0.
04#203At12163127.
4m0.
29/293β+=693;α=313203Rn61602443.
5s2.
1(3/2,5/2)9396Ta18Tα=669;β+=349203Rnm5798243634AD26.
7s0.
513/2(+)9387Bo29Jα=;β+=20#203Fr86116550ms209/2#98α=;β+=5#203Ra8640804ms3(3/2)9896Le09TJDα≈100;β+203Ram88604022090AD41ms17(13/2+)9896Le09TJDα≈100;β+203RnT:average96Ta18=42(3)71Ho01=45(3)203RnmT:from96Ta18204Au20750#200#39.
8s0.
9(2)94β=100204Hg24690.
20.
3STABLE0+94IS=6.
8715;2β204Tl24346.
01.
33.
78y0.
02294β=97.
1012;ε=2.
9012204Tlm23242.
01.
41104.
00.
463s2(7)+94IT=100204Tln2185050025005002.
6s0.
2(12)98Pf02TJIT=100204Tlp2085050035005001.
6s0.
2(20+)98Pf02TJIT=100204Pb25109.
71.
2STABLE(>140Py)0+94IS=1.
41;α204Pbm22923.
91.
22185.
790.
0567.
2m0.
3994IT=100204Bi206672611.
22h0.
106+94β+=100204Bim1986226805.
50.
313.
0ms0.
11094IT=100204Bin17834262833.
41.
11.
07ms0.
03(17+)94IT=100204Po18334113.
53h0.
020+94β+=99.
341;α=0.
661.
.
.
A-groupiscontinuedonnextpage.
.
.
G.
Audietal.
/NuclearPhysicsA729(2003)3–128109NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%).
.
.
A-groupcontinued.
.
.
204At11875249.
2m0.
27+94β+=96.
22;α=3.
82204Atm1128824587.
300.
20108ms10(10)94IT=100204Rn7984151.
24m0.
030+95α=731;β+204Fr608251.
7s0.
3(3+)9495Bi.
ADα=962;β+204Frm65825504AD2.
6s0.
3(7+)9495Bi.
ADα=902;β+204Frn934253264AD1.
7s0.
6(10)9494Le05Tα=748;IT=268204Ra60541560ms110+9895Le04Tα≈100;β+=0.
3#204FrnE:276.
1keVabove204Frm,from95Bi.
AD:αintensityisfrom95Bi.
A204RaT:average95Le04=45(+55–21)96Le09=59(+12–9)205Au18750#300#31s23/2+9794We02Tβ=100205Hg2228745.
2m0.
11/298β=100205Hgm2073041556.
530.
241.
10ms0.
04(13/2+)98IT=100205Tl23820.
61.
3STABLE1/2+93IS=70.
47614205Tlm20530.
01.
33290.
630.
172.
6s0.
225/2+93IT=100205Pb23770.
11.
215.
3My0.
75/293ε=100205Pbm22756.
31.
21013.
8390.
0135.
54ms0.
1013/2+93IT=100205Pbn20574.
51.
43195.
60.
8217ns525/293IT=100205Bi21062715.
31d0.
049/293β+=100205Po17509201.
66h0.
025/293β+≈100;α=0.
041205Pom16048201461.
200.
2158ms119/293IT=100205Pon1662920880.
300.
04645s13/2+205At129721526.
2m0.
59/293β+=902;α=102205Atm10909152062.
570.
2567.
9ns25/2+205Atn10632152339.
600.
257.
8s29/2+205Rn7710502.
8m0.
15/293β+=774;α=234205Fr131083.
85s0.
10(9/2)93α≈100;β+300ns)0+0398Pf02Iβ210Tl9246121.
30m0.
035+#03β=100;βn=0.
0096210Pb14728.
31.
522.
20y0.
220+03β=100;α=1.
9e–64210Pbm13450512785201ns178+03IT=100210Bi14791.
81.
45.
012d0.
005103β=100;α=13.
2e–510210Bim14520.
51.
4271.
310.
113.
04My0.
06903α=100210Bin14358.
31.
4433.
490.
1057.
5ns10703IT=100210Po15953.
11.
2138.
376d0.
0020+03α=100210Pom14396.
11.
21556.
960.
0398.
9ns2.
58+03IT=100210At1197288.
1h0.
4(5)+03β+≈100;α=0.
17520210Atm942282549.
60.
2482s6(15)03IT=100210Atn794484027.
70.
25.
66s0.
07(19)+03IT=100210Atp501386959.
30.
698ns2(26)03IT=100210Rn959892.
4h0.
10+03α=961;β+210Rnm790817169015644ns408+#03IT210Rnn5761173837151.
06s0.
05(17)03IT=100210Rnp3105176493151.
04s0.
07(22)+03IT=100210Fr3346223.
18m0.
066+03α=6030;β+=4030210Ra461153.
7s0.
20+03α=;β+=4#210Ram226020018002002.
24s(8+)0398Le.
AEJ210Ac879060350ms407+#0300He17Tα=;β+=9#210Th140432517ms110+03α=;β+=1#210RnmE:ENSDF2003:lessthan50keVabove1664.
6level210AcT:average00He17=335(+64–46)68Va04=350(50)211Tl6080#200#1#m(>300ns)1/2+#98Pf02Iβ211Pb10491.
42.
736.
1m0.
29/2+91β=100211Bi1185862.
14m0.
029/291α≈100;β=0.
2764211Bim1063161227.
20.
370ns5(21/2)91IT=100211Bin10601121257101.
4s0.
3(25/2)9198Pf02TIT=100211Po12432.
51.
3516ms39/2+91α=100211Pom10970514625AD25.
2s0.
6(25/2+)91α≈100;IT=0.
0164211Pon102985213550.
25s0.
07(31/2)98Fo04ETJIT≈100;α211Pop75595487452s1(43/2+)98Fo04ETJIT≈100;α211At11647.
12.
87.
214h0.
0079/296ε=58.
208;α=41.
808211Rn8756714.
6h0.
21/296β+=72.
617;α=27.
417211Fr4158213.
10m0.
029/291α>80;β+93;β+300ns)5+#98Pf02Iβ212Pb7547.
42.
210.
64h0.
010+92β=100212Pbm6212101335105s1(8+)9298Pf02TIT=100212Bi8117.
32.
060.
55m0.
061()9289Ha.
ADβ=64.
066;α=35.
946;212Bim78703025030AD25.
0m0.
2(9)92α=671;β=331;βα=301212Bin5920#200#2200#200#7.
0m0.
3>1592β≈100;IT212Po10369.
41.
2299ns20+92α=100212Pom745912291112AD45.
1s0.
6(18+)92α≈100;IT=0.
072212At86217314ms2(1)92α≈100;β+99;IT95;β300ns)7/2+#98Pf02Iβ;α219At10397456s35/2#01α≈97;β≈3219Rn8830.
82.
53.
96s0.
015/2+01α=100219Fr8618720ms29/201α=100219Ra9394810ms3(7/2)+01α=100219Ac115705011.
8s1.
59/201α=100;β+=1e–6#219Th14470501.
05s0.
039/2+#01α=100;β+=1e–7#219Pa185205053ns109/201α=100;β+=5e–9#219U232106055s259/2+#01α=100;β+=1.
4e–5#220Po15470#360#40#s(>300ns)0+98Pf02Iβ220At14350503.
71m0.
043(#)97β=922;α=82220Rn10613.
42.
255.
6s0.
10+97α=100;2β220Fr11483427.
4s0.
31+97α≈100;β=0.
355220Ra10273917.
9ms1.
40+9700He17Tα=100220Ac137521526.
36ms0.
19(3)9790An19Tα=100;β+=5e–4#220Th14669229.
7s0.
60+97α=100;ε=2e–7#220Pa2038060780ns1601#97α=100;β+=3e–7#220U23030#200#60#ns0+α;β+220RaT:average00He17=18(2)90An19=17(2)61Ru06=23(5)220AcT:average90An19=26.
4(0.
2)70Bo13=26.
1(0.
5)221At16810#200#2.
3m0.
23/2#90β=100221Rn14472625m27/2(+)90β=781;α=221221Fr1327854.
9m0.
25/29097Ch53Dα≈100;β=0.
004815;221Ra12964528s25/2+9094Bo28Dα=100;14C=1.
2e–109221Ac145205052ms29/2#90α=100221Th1693891.
68ms0.
06(7/2+)90α=100221Pa20380505.
9s1.
79/290α=100221U24590#100#700#ns9/2+#α;β+221FrD14C=8.
8e–1111221FrD:βintensityisfrom97Ch53;14Cintensityisfrom94Bo28221ThT:also00He17=2.
0(+0.
3–0.
2)222At20800#300#54s1096β=100222Rn16373.
62.
43.
8235d0.
00030+96α=100222Fr163492114.
2m0.
3296β=100222Ra14321538.
0s0.
50+96α=100;14C=3.
0e–810222Ac1662155.
0s0.
5196α=991;β+=11222Acm16820#150#200#150#1.
05m0.
07high96α=;IT≤10;β+=1.
44222Th17203122.
05ms0.
070+9600He17Tα=100;ε2s)9/2#9794Ye08IDα=100225UT:00He17=59(+5–2);others94An02=68(+45–20)92To02=95(15)and225UT:89He13=80(+40–10)outweighed,notused226Rn28770#400#7.
4m0.
10+96β=100226Fr2737010049s1196β=100226Ra23669.
12.
31.
600ky0.
0070+9690We01Dα=100;14C=2.
6e–96;2β226Ac24310329.
37h0.
12(1)(#)96β=833;ε=173;α=0.
0062226Th23197530.
57m0.
100+9601Bo11Dα=100;18O95;ε2s)0+9794An02IDα≈100;β+=0.
1#228NpD:β+SF=0.
020(9)%denedby94Kr13relativetoε,thus0.
012(6)%oftotal116G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)229Fr358204050.
2s0.
41/2+#9092Bo05Tβ=100229Ra32563194.
0m0.
25/2(+)90β=100229Ac307503062.
7m0.
5(3/2+)90β=100229Th29586.
52.
87.
34ky0.
165/2+90α=100229Thm29586.
52.
80.
00350.
001070h503/2+94He08TEJIT229Pa29898.
02.
71.
50d0.
05(5/2+)90ε≈100;α=0.
485229Pam29909.
62.
711.
60.
3420ns303/298Le15EJDIT=100229U31211658m3(3/2+)90β+≈80;α≈20229Np33780904.
0m0.
25/2+#90α>50;β+3233Cm47290701#m3/2+#01Ca.
BDα=;β+233UD24Ne=7.
2e–119;28Mg250ns(5/2+)03β=100239Un50707.
71.
9133.
79900.
0010780ns401/2+03IT=100239Np49312.
42.
12.
356d0.
0035/2+03β=100;α=5e–10#239Pu48589.
91.
824.
11ky0.
031/2+03α=100;SF=3.
1e–106239Pum48981.
51.
8391.
5840.
003193ns47/203IT=100239Am49392.
02.
411.
9h0.
1(5/2)03ε≈100;α=0.
0101239Amm518902002500200163ns12(7/2+)03SF≈100;IT239Cm51190#100#2.
9h(7/2)03β+≈100;α1.
1Ey,from92Mo25;thus2β10;SF=4.
513;246Md76280#330#1.
0s0.
498α=;β+;SF246Mdm76490#340#21070EU1.
0s0.
496Ni09TDα=;β+246EsDβ+SF≈0.
003246FmDβ+SF=105246MdmI:nolongerconsideredtoexist,seeENSDF'98247Pu69000#300#2.
27d0.
231/2+#93β=100247Am67150#100#23.
0m1.
35/2#93β=100247Cm65534415.
6My0.
59/293α=100247Bk6549161.
38ky0.
25(3/2)93α≈100;SF247Cf6613783.
11h0.
037/2+#93ε≈100;α=0.
0355247Es68610#30#4.
6m0.
37/2+#93β+≈93;α≈7;SF≈9e–5#247Esp68930#200#320#200#am247Fm71580#140#35s45/2+#93α≥50;β+≤50247FmmnonexistentEU9.
2s2.
39367Fl15Iα≈100;IT247Fmp71730#170#150#100#Nm(7/2+)247Fmq71980#210#400#150#247Md76040#320#270ms1601/2#9393Ho.
ATDSF=;α247Mdm76170#310#130#100#Nm1.
12s0.
22(7/2+)93Ho.
ATDα=100;SF=0.
0001#247FmmI:existenceofthisisomerisdiscussedinENSDFG.
Audietal.
/NuclearPhysicsA729(2003)3–128121NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)248Am70560#200#3#m99β248Cm673925348ky60+99α=91.
6116;SF=8.
3916;248Bk68080#70#>9y6+#99α248Bkm681102130#70#23.
7h0.
21()99β=705;ε=305;α=0.
001#248Bkp681305050#50#(5)248Cf672405334d30+99α≈100;SF=0.
00293248Es70300#50#27m52#,0+#99β+≈100;α≈0.
25;β+SF=3e–5248EsmnonexistentRN41m89Ha27I248Fm719061236s30+99α=937;β+=77;SF=0.
105248Md77150#240#7s399β+=8010;α=2010;248Mdp77250#250#100#70#248No80660#300#60;β+249Mdm77430#250#100#100#1.
9s0.
9(1/2)01He35TJDα=100249No81820#340#57s125/2+#9903Be18Tβ+;α249BkDSF=47e–92250Cm72989118300#y0+01SF≈74;α≈18;β≈8250Bk7295143.
212h0.
005201β=100250Bkm72987435.
590.
0529s1(4+)01IT=100250Bkn73036584.
12.
1AD213s8(7+)01IT250Cf71171.
82.
113.
08y0.
090+01α≈100;SF=0.
0773250Es73230#100#8.
6h0.
1(6+)01β+>97;α250Esm73430#180#200#150#2.
22h0.
051()01β+≈100;α250Fm740741230m30+01α>90;ε80;α50;α80;α254Lr89850#340#13s301α=7611;β+=2411;SF254Lrp89880#340#30#70#254Rf93320#290#23s30+0197He29TDSF=;α94;SF87;SF95;β+150000y,from86Lo16,thusSF82;SF70;SF263Sgm110320#100#100#70#Nm120ms3/2+#99α=;IT263Bh114610#370#200#ms99α263Hs119750#350#1#ms7/2+#99α=100263Hsp120250#360#500#100#amα;SF263RfT:average03Kr.
1=24(+19–7)m93Gr.
C=500(+300–200)s92Cz.
A=600(+300–200)s263DbD:SFfrom92Kr01=57(+13–15);β+average03Kr.
1=3(+4–1)93Gr.
C=8(2)263DbT:Possiblyacandidateforthe54(+98–21)sSFdecayobservedby98Ik02G.
Audietal.
/NuclearPhysicsA729(2003)3–128125NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)264No104650#640#1#m0+α;SF264Lr106230#440#10#hα;SF264Rf106180#450#1#h0+α264Db109360#230#3#mα264Sg110780#280#400#ms0+99α264Bh116070#280#1.
3s0.
59902Ho11Tα=;β+264Bhp116370#310#300#150#am264Hs11960040540s3000+9995Ho.
BTα≈50;SF≈50264BhT:meanlifetimeof6events1.
5s264HsT:95Ho.
B(2events76sand825s)87Mu15(1event80s).
Averageof264HsT:the3events:327(+448–120)s,see84Sc13265Lr107900#710#10#hα;SF265Rf108710#420#13h3/2+#0099Og.
ATDα265Db110480#280#15#mα265Sg112820608s33/2+#99α>50;SF265Sgp113120#120#300#100#11/2#265Bh116570#380#500#msα265Hs121170#140#2.
1ms0.
39/2+#99α≈100;SF<1265Hsm121480#140#30070AD780s1503/2+#99α≈100;IT265Mt126820#460#2#msα265RfT:onecaseonlyaftera1.
3hmeasurement266Lr111130#660#1#hα;SF266Rf109880#540#10#h0+α;SF266Db112740#360#20#mα;SF266Sg113700#290#21s60+0198Tu01Tα=349;SF=669266Bh118250#200#5s301α≈100;β+;SF266Hs121190#280#2.
7ms1.
00+0101Ho06TDα=;SF≈1.
4#266Mt127890#350#1.
2ms0.
40184Og03Dα=;SF<5.
5266Mtm129120#350#123080AD6ms30197Ho14TDα=100266SgT:average98Tu01=21(+20–12)94La22=10-30D:from18%<α<50%50%01(+0.
47–0.
24)266MtmT:3eventsat7.
8,2.
0and5.
0yield3.
4(+4.
7–1.
3)267Rf113200#580#5#hα;SF267Db113990#470#2#hα;SF267Sg115900#270#19ms99Og.
BTα=100267Bh118910#260#22s1000Wi15TDα=100267Hs122760#100#32ms153/2+#00α=100267HsmnonexistentEU200ms95Ho.
ATDIα=;IT267Mt127900#540#10#msα267Ea134450#370#10s89/2+#0095Gh04Tα=100267HsmI:tentativeonly267EaT:onesingleevent,lifetime4s,thusT=2.
8(+13.
0–1.
3),see84Sc13268Rf115170#710#1#h0+α;SF268Db116850#530#6#hα;SF268Sg117000#540#30#s0+α;SF268Bh120870#380#25#sα;SF268Hs123110#410#2#s0+α268Mt129220#320#53ms215+#,6+#0002Ho11Tα=100268Mtp129470#330#250#100#α;SF268Ea133940#500#100#s0+α268MtT:meanlifetimeof6events60ms126G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)269Db118730#770#3#hα;SF269Sg119930#660#35s2300α<100;SF269Bh121740#410#25#sα269Hs124870#120#27s170002Ho11Tα=100269Mt129530#550#200#msα269Ea135180#140#230s1103/2+#0095Ho03Tα=100269HsT:2eventsat19.
7and22.
0syield14(+26–6)270Db121760#720#1#hα;SF270Sg121400#620#10#m0+α;SF270Bh124460#470#30#sα;SF270Hs125430#290#30#s0+01Tu.
BDα=100270Mt131020#540#2#sα270Ea134810#290#160s1000+01Ho06TDα≈100;SF≈0.
2270Eam135940#290#11407010ms6(10)(#)01Ho06ETJα=;IT271Sg124330#650#2#hα;SF271Bh125920#560#40#sα;SF271Hs128230#340#40#sα;SF271Mt131470#570#5#sα271Ea136060#110#210ms17011/2#00α=100271Eam136090#110#2929AD1.
3ms0.
59/2+#00α=100272Sg125900#770#1#h0+α;SF272Bh128580#610#2#mα;SF272Hs129530#580#40#s0+α;SF272Mt133890#480#10#sα;SF272Ea136290#650#1#s0+SF272Eb143090#330#2.
0ms0.
85+#,6+#0002Ho11Tα=100272EbT:meanlifetimeof6events2.
3ms273Sg128750#660#1#mSF273Bh130050#830#90#mα;SF273Hs132260#830#RN50#s3/2+#0002Ni10Iα273Mt134990#510#20#sα;SF273Ea138670#130#360s28013/2#00α=100273Eam138870#130#19820EU120ms3/2+#00α=100273Eap138950#130#29040ADα;SF273Eb143150#610#5#msα273HsT:99Ni03=1.
2(+1.
7–0.
6)alphadecayretractedbyauthorsin02Ni10274Bh132680#780#90#mα;SF274Hs133330#650#1#m0+α;SF274Mt137390#560#20#sα;SF274Ea139250#490#2#s0+α;SF274Eb145050#620#5#msα275Bh134370#650#40#mSF275Hs135950#710#30#mα;SF275Mt138460#590#30#sα;SF275Ea141750#450#2#sα;SF275Eb145450#690#10#msαG.
Audietal.
/NuclearPhysicsA729(2003)3–128127NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)276Hs137120#820#1#h0+α;SF276Mt140800#680#40#sα;SF276Ea142550#610#5#s0+α;SF276Eb147640#630#100#msα;SF277Hs139580#730#40m303/2+#0099Og10TDSF=100277Mt141980#880#1#mα;SF277Ea144980#960#RN5#s11/2+#0002Ni10Iα277Eb148590#620#1#sα;SF277Ec152710#130#1.
1ms0.
73/2+#0002Ho11Tα=100277HsT:onesingleevent16.
5myields11(+55–5)277EaT:99Ni03=3.
0(+4.
7–1.
5)alphadecayretractedbyauthorsin02Ni10277EcT:twoeventsat0.
280msand1.
406ms278Mt144210#840#30#mα;SF278Ea145750#680#10#s0+α;SF278Eb150530#630#1#sα;SF278Ec153060#530#10#ms0+α;SF279Mt145490#720#6#mα;SF279Ea147980#740#10#sα;SF279Eb151340#660#3#sα;SF279Ec155140#490#100#msα;SF280Ea148850#850#11s60+01Og01TDSF=100280Eb153210#740#10#sα;SF280Ec155600#640#1#s0+α;SF280EaT:3eventsat6.
93,14.
3and7.
4yield6.
6(+9–2.
4)281Ea150960#730#4m33/2+#0099Og10TDα=100281Eb154040#930#1#mα;SF281Ec157690#990#RN10#s3/2+#0002Ni10Iα281EaT:onesingleevent1.
6myields1.
1(+5.
3–0.
5),see84Sc13281EcT:99Ni03=0.
89(+1.
30–0.
45)alphadecayretractedbyauthorsin02Ni10282Eb156010#890#4#mα;SF282Ec158140#710#30#s0+α;SF283Eb156880#780#10#mα;SF283Ec160020#770#4.
2m2.
199Og05TDSF=100283Ed164360#730#10#sα;SF283EcT:4eventsat99Og07=9.
3m,3.
8m,99Og05=3.
0mand0.
9myield3(+3–1)m284Ec160570#850#31s180+01Og01TDα=100284Ed165880#800#1#mα;SF285Ec162180#730#40m305/2+#0099Og10TDα=100285Ed166490#980#2#mα;SF285Ee171110#1030#RN5#s3/2+#0002Ni10Iα285EcT:onesingleevent15.
4syields11(+51–5),see84Sc13285EeT:99Ni03=580(+870–290)alphadecayretractedbyauthorsin02Ni10128G.
Audietal.
/NuclearPhysicsA729(2003)3–128NuclideMassexcessExcitationHalf-lifeJπEnsReferenceDecaymodesand(keV)energy(keV)intensities(%)286Ed168120#940#5#mα;SF286Ee171260#770#5#s0+α;SF287Ed168640#830#20#mα;SF287Ee172880#770#10s799Og07Tα=100287Ef178090#790#500#msα;SF287EeT:2eventsat1.
32sand14.
4syield5.
5(+10–2)288Ee172970#850#2.
8s1.
40+01Og01TDα=100288Ef179310#850#1#sα;SF289Ee174450#730#80s605/2+#0099Og10TDα=100289Ef179510#1020#10#sα;SF289Eg185240#1090#RN10#ms5/2+#0002Ni10Iα289EeT:onesingleeventat30.
4syields21(+101–10)289EgT:99Ni03=600(+860–300)alphadecayretractedbyauthorsin02Ni10290Ef180840#980#10#sα;SF290Eg184990#840#50#ms0+α;SF291Ef181070#890#1#mα;SF291Eg186310#850#100#msα;SF291Eh192410#880#10#msα;SF292Eg186100#850#120ms1000+01Og01TDα=100292Eh193330#940#50#msα;SF292EgT:onesingleeventat46.
9msyields33(+155–15)293Ei199960#1200#RN5#ms1/2+#0002Ni10Iα293EiT:99Ni03=120(+180–60)alphadecayretractedbyauthorsin02Ni10