ComPASSsolved

solved  时间:2021-01-17  阅读:()
eScholarshipprovidesopenaccess,scholarlypublishingservicestotheUniversityofCaliforniaanddeliversadynamicresearchplatformtoscholarsworldwide.
LawrenceBerkeleyNationalLaboratoryLawrenceBerkeleyNationalLaboratoryTitle:UpdateonElectron-CloudSimulationsUsingthePackageWARP-POSINSTAuthor:Penn,G.
PublicationDate:10-09-2009PublicationInfo:LawrenceBerkeleyNationalLaboratoryPermalink:http://escholarship.
org/uc/item/0vp975ckUpdateonElectron-CloudSimulationsUsingthePackageWARP-POSINSTJ.
-L.
Vay,C.
M.
Celata,M.
A.
Furman,G.
Penn,M.
Venturini,LBNL,Berkeley,USAD.
P.
Grote,LLNL,Livermore,USA;K.
G.
Sonnad,U.
ofKarlsruhe,GermanyINTRODUCTIONAtPAC05[1]andPAC07[2],wepresentedthepackageWARP-POSINSTforthemodelingoftheeffectofelec-troncloudsonhigh-energybeams.
Wepresentherethelatestdevelopmentsinthepackage.
Threenewmodesofoperationswereimplemented:1)abuild-upmodewhere,similarlytoPOSINST(LBNL)orECLOUD(CERN),thebuild-upofelectroncloudsdrivenbyalegislatedbunchtrainismodeledinoneregionofanaccelerator;2)aquasi-staticmodewhere,similarlytoHEADTAIL(CERN)orQuickPIC(USC/UCLA),thefrozenbeamapproximationisusedtosplitthemodelingofthebeamandtheelec-tronsintotwocomponentsevolvingontheirrespectivetimescales;and3)aLorentzboostedmodewherethesim-ulationisperformedinamovingframewherethespaceandtimescalesrelatedtothebeamandelectrondynamicsfallinthesamerange.
Theimplementationofmodes(1)and(2)wasprimarymotivatedbytheneedforbenchmark-ingwithothercodes,whiletheimplementationofmode(3)fulllsthedrivetowardfullyself-consistentsimulationsofe-cloudeffectsonthebeamincludingthebuild-upphase.
BUILD-UPMODEFigure1:Sketchofthebuild-upmode.
Thedynamicsofelectronsisfollowedforathin(2-D)orthick(3-D)slicelocatedatagivenlocationinthelattice,undertheinuenceofalegislatedparticlebeampassingthroughtheslice.
Inordertofacilitatedirectcomparisonwithbuild-upcodeslikePOSINST[4,5,6,7],ECLOUD(CERN)orCloudland(SLAC),abuild-upmodeclasswasimple-mentedinWarp.
Inthismode,thedynamicsofelectronsisfollowedforathin(2-D)orthick(3-D)slicelocatedatagivenlocationinthelattice,undertheinuenceofalegis-latedparticlebeampassingthroughtheslice(Fig.
1).
RunsWorksupportedbytheUS-DOEunderContractDE-AC02-05CH11231,theUS-LHCLARP,andtheUS-DOESciDACprogramComPASS.
ThisworkusedresourcesofNERSC,supportedbytheUS-DOEunderContractDE-AC02-05CH11231.
jlvay@lbl.
govwereperformedwithWarpandPOSINSTfortheevolu-tionofanelectroncloudsliceinthemiddleofadipole.
TheaverageelectrondensityhistoryisgiveninFig.
2foraPOSINSTrunandthreeWarprunsin:(a)2-D,(b)3-Dwith4cellslongitudinallyandalengthof0.
2σz,and(c)3-Dwith16cellslongitudinallyandalengthof0.
8σz,whereσzisthebeamRMSlength.
Forthe3-Druns,pe-riodicboundaryconditionswereappliedlongitudinallyforeldsandparticles.
SnapshotsofcoloredelectrondensityplotsandverticalphasespacearegiveninFig.
3,takenatt=130ns.
TheseresultsdemonstrateaverygooddegreeofagreementforelectroncloudbuildsimulationsbetweenPOSINST,Warpin2-D,andWarpin3-D.
Figure2:AverageelectrondensityversustimefromPOSINSTandWarpinbuild-upmodesimulations.
QUASISTATICMODEWehaveimplementedaquasistatic[8]modeinWarp.
Inthismode,a2-Dslabofelectronmacroparticlesissteppedbackward(withsmalltimesteps)throughthebeameld(seeFig.
4).
The2-Delectronelds(solvedateachstep)arestackedina3-Darray,thatisusedtogiveakicktothebeam.
Finally,thebeamparticlesarepushedforward(withlargertimesteps)tothenextstationofelectrons,us-ingeithermapsoraLeap-Frogpusher.
Therstimple-mentationwasforacceleratorlatticestreatedinthesmoothapproximation.
Amoredetailedlatticedescriptionwasimplementedlater(seebelow).
Thismodeallowsfordi-rectcomparisonwiththequasistaticcodesHEADTAIL[9],QuickPIC[10],PEHTS[11]orCMAD[12].
Theparal-lelizationismono-dimensional(alongs)usingpipelining,similarlytoQuickPIC(seeFig.
5).
Wehavesimulatedane-clouddriveninstabilityinanLHC-likeringwithWarpinaquasistaticmode,andHEADTAIL.
Weusedthepa-rametersfromtable1inadrift(Fig.
6)andinadipole(Fig.
7).
SomeoftheparameterswerepurposelychosentoFigure3:Snapshotsofelectrondensityandverticalphasespacefrombuild-upsimulationsusing(left)POSINST,(middle)Warpin2-D,(right)Warpin3-D.
beunphysicallylarge,soastomagnifytheireffects.
Thetwocodespredictsimilaremittancegrowthunderthevar-iousconditions,withexcellentqualitativeagreementandgoodtoverygoodquantitativeagreement.
Wetentativelyattributethequantitativediscrepanciestodifferencesinim-plementationsincluding:adaptiveversusxedgridsizes,differenteldsolversandparticlepushers,differenteldinterpolationproceduresnearinternalconductors,slightlydifferentvaluesofphysicalconstants,etc.
Table1:Parametersusedforsimulationsofe-clouddriveninstabilitystudiesintheLHC.
circumferenceC26.
659kmbeamenergyEb450GeVbunchpopulationNb1.
1*1011rmsbunchlengthσz0.
13mrmsbeamsizesσx,y0.
884,0.
884mmbetafunctionsβx,y66.
,71.
54mbetatrontunesQx,y64.
28,59.
31chromaticitiesQx,y1000.
,1000.
synchrotrontuneν0.
59momentumcompactionfactorα0.
347*103rmsmomentumspreadδrms4.
68*102BOOSTEDFRAMEAPPROACHItwasshownin[13]thatitwaspossibletoperformsim-ulationsofelectron-driveninstabilitiesfromrstprinciples(e.
g.
usingstandardParticle-In-Cellmethods),atmuchre-ducedcomputingcostbyperformingthecalculationinaFigure4:Sketchofthequasistaticmode.
A2-Dslabofelectronmacroparticlesissteppedbackward(withsmalltimesteps)throughthebeameld.
The2-Delectronelds(solvedateachstep)arestackedina3-Darray,thatisusedtogiveakicktothebeam.
Finally,thebeamparticlesarepushedforward(withlargertimesteps)tothenextstationofelectrons.
Figure5:Sketchoftheparalleldecompositionforthequa-sistaticmode.
Thebeamisdistributedamongnslices,thatareuniformlyspreadamongNprocessors.
Usingapipeliningalgorithm,slicesonagivenprocessorarepushedfromonestationtothenext,withoutwaitingfortheslicesofthepreviousprocessorstoreachthesamestation.
suitableLorentzboostedframe.
Numericaldevelopmentsthatwereneededhavebeenimplemented,includinganewparticlepusherandeldsolver,andaredescribedin[14].
Specialhandlingofinputsandoutputsbetweentheboostedframeandthelaboratoryframearedescribedin[15].
TwoWarpcalculationsofanelectronclouddriveninstabilityFigure6:FractionalemittancegrowthfromWarp(red)andHEADTAIL(black)simulationsofane-clouddriveninsta-bilityindriftsofanLHC-likeringforanelectronback-grounddensityof1014m3for(top)ν=α=δrms=Qx=Qy=0,(middle)Qx=Qy=0,(bottom)parame-tersfromtable1.
showedverygoodagreement[14]betweenafullPICcal-culationinaboostedframeandacalculationusingthequa-sistaticmode,forsimilarcomputationalcost.
FURTHERDEVELOPMENTSWehaverecentlyaddedthecapabilitytouselinearmapstopushparticlesinacceleratorlattices,withinthequa-sistaticmodeandthefullPICmodeinaLorentzboostedframe.
GoodquantitativeagreementwasobtainedbetweenWarpusingthequasistaticmodeandCMAD[12].
SimilarcalculationswiththefullPICmethodinaboostedframeareinprogress.
Figure7:FractionalverticalemittancegrowthfromWarpandHEADTAILsimulationsindipolesofanLHC-likeringforthreeassumedinitialelectrondensities.
ACKNOWLEDGMENTSWethankG.
Rumoloforprovidingthesourceandin-valuablesupportforusingthecodeHEADTAIL.
REFERENCES[1]JLVayetal,ParticleAcceleratorConference,Knoxville,TN(2005),papersROPB006andFPAP016[2]M.
A.
Furmanetal,ParticleAcceleratorConference,Albu-querque,NM(2007),paperTUXAB03[3]D.
P.
Grote,A.
Friedman,J.
-L.
Vay.
I.
Haber,AIPConf.
Proc.
749(2005)55.
[4]M.
A.
FurmanandG.
R.
Lambertson,LBNL-41123/CBPNote-246,PEP-IIAPNoteAP97.
27(Nov.
25,1997).
Proc.
Intl.
WorkshoponMultibunchInstabilitiesinFutureElectronandPositronAccelerators"MBI-97"(KEK,15-18July1997;Y.
H.
Chin,ed.
),KEKProceedings97-17,Dec.
1997,p.
170.
[5]M.
A.
FurmanandM.
T.
F.
Pivi,LBNL-49771/CBPNote-415(Nov.
6,2002).
PRST-AB5,124404(2003),http://prst-ab.
aps.
org/pdf/PRSTAB/v5/i12/e124404.
[6]M.
A.
FurmanandM.
T.
F.
Pivi,LBNL-52807/SLAC-PUB-9912(June2,2003).
[7]M.
A.
Furman,LBNL-41482/CBPNote247/LHCProjectReport180(May20,1998).
[8]P.
Sprangle,E.
Esarey,andA.
Ting,Phys.
Rev.
Letters64,2011-2014(1990).
[9]G.
RumoloandF.
Zimmermann,PRST-AB5121002(2002).
[10]C.
Huang,V.
K.
Decyk,C.
Ren,M.
Zhou,W.
Lu,W.
B.
Mori,J.
H.
Cooley,T.
M.
Antonsen,Jr.
andT.
Katsouleas,J.
ofCom-put.
Phys.
217,658-679(2006).
[11]K.
Ohmi,SingleBunchElectronCloudInstabilityforaRoundBeam(Memo),19.
Nov.
2002.
[12]M.
Pivi,TheseproceedingsWE1PBI01.
[13]J.
-L.
Vay,Phys.
Rev.
Lett.
,98(2007)130405.
[14]J.
-L.
Vay,Phys.
Plas.
,15(2008)056701.
[15]J.
-L.
Vayetal,TheseproceedingsTU1PBI04.

器安装环境和运维管理工具推荐

今天看到一个网友从原来虚拟主机准备转移至服务器管理自己的业务。这里问到虚拟主机和服务器到底有什么不同,需要用到哪些工具软件。那准备在下班之间稍微摸鱼一下整理我们服务器安装环境和运维管理中常见需要用到的软件工具推荐。第一、系统镜像软件一般来说,我们云服务器或者独立服务器都是有自带镜像的。我们只需要选择镜像安装就可以,比如有 Windows和Linux。但是有些时候我们可能需要自定义镜像的高级玩法,这...

华纳云-618大促3折起,18元/月买CN2 GIA 2M 香港云,物理机高防同享,10M带宽独享三网直连,无限流量!

官方网站:点击访问华纳云活动官网活动方案:一、香港云服务器此次推出八种配置的香港云服务器,满足不同行业不同业务规模的客户需求,同时每种配置的云服务都有不同的带宽选择,灵活性更高,可用性更强,性价比更优质。配置带宽月付6折季付5.5折半年付5折年付4.5折2年付4折3年付3折购买1H1G2M/99180324576648直达购买5M/17331556710081134直达购买2H2G2M892444...

LOCVPS全场8折,香港云地/邦联VPS带宽升级不加价

LOCVPS发布了7月份促销信息,全场VPS主机8折优惠码,续费同价,同时香港云地/邦联机房带宽免费升级不加价,原来3M升级至6M,2GB内存套餐优惠后每月44元起。这是成立较久的一家国人VPS服务商,提供美国洛杉矶(MC/C3)、和中国香港(邦联、沙田电信、大埔)、日本(东京、大阪)、新加坡、德国和荷兰等机房VPS主机,基于XEN或者KVM虚拟架构,均选择国内访问线路不错的机房,适合建站和远程办...

solved为你推荐
域名查询我的电脑域名怎么查电信主机租用租用电信服务器要注意什么?域名备案域名怎么进行备案?免备案虚拟空间免备案的虚拟主机空间,买了以后会强制备案不?php虚拟空间普通网站需要多大空间?本人新手php学习者,想买个虚拟空间用来放自己做的一些企业站,只是练习用途重庆虚拟空间重庆那里可以租用VSP主机什么是虚拟主机什么是“虚拟主机”?请解释祥细些!最好的虚拟主机哪家的虚拟主机比较好?广西虚拟主机虚拟主机哪里的好?shopex虚拟主机我有一个PHP1G的虚拟主机,请问做什么站比较合适?
最便宜的vps raksmart mediafire 免费个人博客 网站实时监控 论坛空间 cpanel空间 福建天翼加速 bgp双线 asp免费空间申请 速度云 泉州移动 isp服务商 超级服务器 美国独立日 双线asp空间 免费ftp 电信网络测速器 新加坡空间 中国电信测速网站 更多