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Building dwarf galaxies out of merged young star clusters

来源:世旅网
1002 nJu 22 1v6146010/hp-ortsa:viXraBuildingdwarfgalaxiesoutofmergedyoungstar

clusters

MichaelFellhauer

Inst.f¨urTheor.Phys.&Astrophys.Univ.Kiel,Leibnizstr.15,

24098Kiel,Germany

Abstract

Youngstarclustersininteractinggalaxiesareoftenfoundingroupsorclustersofstarclusterscontainingupto100singleclusters.Inourprojectwestudythefuturefateoftheseclustersofstarclusters.Wefindthatthestarclustersmergeontimescalesofafewdynamicalcrossingtimesofthesuper-cluster.Theresultingmergerobjecthassimilaritieswithobserveddwarfellipticals(dE).Furthermore,ifde-structiveprocessesliketidalheating,dynamicalfrictionorinteractionwithdiscorbulgeoftheparentgalaxyaretakenintoaccountourmergerobjectsmayevolveintoobjectsresemblingdwarfspheroidalgalaxies(dSph),withouttheneedofahighdarkmattercontent.

1Introduction

Systemsofinteractinggalaxies(likeTheAntennaeorStephan’sQuintet)showintensestarformation.Inthetidaltailsonefindsespeciallyyoungmassivestarclusters(Reff≈2−10pc;M≈104−107M⊙;seee.g.Whitmoreetal.(1999)).Thesestarclustersarenotdistributeduniformlybutareclusteredintogroups,somecontainingmorethanahundredclusters.Withthisprojectweinvestigatethefuturefateoftheseclustersofstarclusters(whatwecall“super-cluster”).FollowingtheargumentsofKroupa(1998)thesesuper-clustersmaybeboundentities,meaningthatthestarclustersinthesuper-clusterarenotonlyboundtothetidalfieldoftheparentgalaxybutalsoboundtoeachother.Therefore,thestarclustersareverylikelytomergewitheachotheronafewdynamicaltimesofthesuper-cluster.Thismergingprocessandtheresultingmergerobjectarethemajortopicofthisproject.

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2M.Fellhauer

2Setup

Wesimulatesuper-clusterscontainingN0=20starclusters.EachofthemisrepresentedbyaPlummersphere,containing100,000particles,atotalmassof106M⊙,ascale-length(Plummerradius)ofRpl=6pcandacrossingtimeof1.4Myr.AllstarclustersaredistributedintoanencompassingPlummer

sc=50,75,150,300pc,andthissuper-spherewithvariedscale-length,Rpl

clusterisplacedonacircularorbitatdistanceD=5,10,20,30,50,100kpcaroundananalyticgalacticpotentialwithanasymptoticallyflatrotationcurvewithvc=220km/sandRgal=4kpc.Forthediscussionoftheresults

sc=wedefinetwodimensionlessparametersforoursystems.α=Rpl/Rpl

0.02,0.04,0.08,0.12istheratiobetweenthescale-lengthofthesingleclus-sc/Rterandthescale-lengthofthesuper-cluster.β=Rcuttidal=0.2–2.7is

theratiobetweenthesizeandthetidalradiusofthesuper-cluster.Sev-eralrandomrealizationsofeachparametercombinationareperformedtoreducestochasticerrors.ThesimulationsarecarriedoutwiththeparticlemeshcodeSuperbox(Fellhaueretal.2000)whichhastheabilitytotracemanyobjectswithdifferentlevelsofhighresolutionsub-grids.Whiletheoutermostgridcoversthewholeorbitaroundthegalacticcentrewiththelowestresolution,themediumsizedgridsofeachstarclustercoverthesizeofthesuper-clusterandallintermediateinteractionsbetweentheclustersinmediumresolution(10–50pc),andtheinnermosthighresolution(1pc)gridscovereachsinglecluster.Bothmediumandhighresolutiongridsstayfocusedonthesimulatedobjectsandtravelwiththemthroughthesimula-tionarea.

3CompactMergerObjects

Adetaileddescriptionofthemergingtime-scalesandtheefficiencyofthemergerprocesswillappearinFellhaueretal.(2001).

Theresultingmergerobjectsarecompact,sphericalanddenseobjects.Theyhavehalf-massradiifrom40–150pcandsizesof120–1,000pc.Themassoftheseobjectsresemblesbetween75and95%ofthetotalmassoftheinitialsuper-cluster.Centraldensitiesarederivedbyfittingexponentialpro-filestotheinnerparts.Therangeofcentraldensitiesis100–1,000M⊙/pc3withexponentialscalelengthsofabout10pc.Intheouterpartsasteeppowerlaw(r−3.5)fitsthedensitybest.Thesurface-densitycanbewellfittedwithade-Vaucouleurprofile.Thevelocitydispersioninthecentralregionis

Buildingdwarfgalaxies3

about30km/sbutmeasuredalongtheline-of-sightthroughthecentreonederivesabout20km/s.Allthisdatasuggeststhatourmergerobjectshavesimilarpropertiestonucleateddwarfgalaxies(dE,N).Becausethemergerprocesslastsforaboutadozencrossingtimesofthesuper-cluster(forsmallα’sthiscansumuptomorethan1Gyr)themergerobjectissurroundedbyseveralstarclusterswhicharestillintheprocessofmergingorareonnear-circularorbitsaroundthesuper-clusterandslowlydecayingthroughdynamicalfriction.Therefore,ourmodelcanaccountforhighspecificclus-terfrequencies(SN),whicharefoundfordE,N-galaxies.

Furthermore,oursimplemodelsdonotaccountfordestructiveprocessesliketidalheatingoneccentricorbits,dynamicalfrictionintheparentgalaxyanddecayoforbit,shocksduetodiscorbulgepassages.Alltheseprocesseswouldleadtoamass-lossofthemergerobjectandadecreaseinitscen-traldensity.Translatedtoobservations,ourobjectswouldtransformintodE,noNwithtime,whilethenumberofremainingclustersisalsodecreasing.ObservationsshowthatdE,NhavehigherSNthandE,noN.

Ourobjectsalsoshowextendedtidaltailsalongthewholeorbitaroundthegalacticcentre.Escapedstarclustersarefoundinthesetidalfeatures.

4DissolvedMergerObject

Intwotestcalculationsthesuper-clusterwassetuponaneccentricorbit(Dapo=60kpc,Dperi=30kpc)sothattidalheatingcouldactonthemergerobjects.Themergerobjectsgetdissolvedwithtime(mass-loss≈5%perperigalacticonpassage).Duetoadisruptiveinteractionwithasecondobjectthecentraldensitiesdropdownfromseveralhundredto0.3–0.002M⊙/pc3,butcanstillbefittedwithanexponentialintheinnermostpart.Butintheouterpartsthematerialisnotboundtotheobjectanymore.Ithasa“fluffy”structureextendingafewkpc.Thesurface-densitycannotbefittedwithade-Vaucouleurprofileanymore.Themeasuredcentralvelocitydispersionsareintheorderof1–3km/s,butmeasuredalongtheline-of-sightthroughthecentreandtheouterunboundpartsonederivesabout10km/s.Comparedwithobservationstheseobjectslooklikedwarfspheroidalgalaxies(c.f.Klessen&Kroupa1998).StarclustersremainingaroundtheseobjectscanaccountfortheveryhighSNofsomedSph-galaxies.

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5Conclusions

Withoursimulationsweareabletoshow,thatthestarclustersinasuper-clustermergeefficiently.Comparingourparameterswithobservationswepredictanexponentialdecreasewithtimeofthenumberofclustersiftheobservedsuper-clustersareboundentities.

TheresultingmergerobjecthassimilarpropertieslikedE,N-galaxies,andifdestructiveprocessesaretakenintoaccountthenextstepintheevo-lutionofourobjectswouldbedE,noN.ThisalsogivesanaturalexplanationwhydE,NhavehigherSNthandE,noN.

ThefinalstageoftheevolutionwouldbeadSph-galaxy,suggestingthatatleastsomeoftheseobjectsmaynothaveapredictedhighdarkmattercontent.

References:

Fellhauer,M.,Kroupa,P.,Baumgardt,H.,Bien,R.,Boily,C.M.,Spurzem,R.,&Wassmer,N.2000,NewA,5,305

Fellhauer,M.,&KroupaP.2000,ASPConf.Ser.,211,2411

Fellhauer,M.,Baumgardt,H.,Kroupa,P.,&Spurzem,R.2001,Cel.Mech.&Dyn.Astron.inpress;astro-ph/0103052

Gallagher,S.C.,Hunsberger,S.D.,Charlton,J.C.,&Zaritsky,D.2000,ASPConf.Ser.,211,2471

Grebel,E.K.2000,ASPConf.Ser.,211,2621

Hunsberger,S.D.,Gallagher,S.D.,Charlton,J.C.,&Zaritsky,D.2000,ASPConf.Ser.,211,2541

Klessen,R.S.,&Kroupa,P.1998,ApJ,498,143Kroupa,P.1998,MNRAS,300,200Mateo,M.1998,ARAA,36,435

Whitmore,B.C.,Zhang,Q.,Leitherer,C.,&Fall,S.M.1999,AJ,118,1551Zhang,Q.,&Fall,S.M.1999,ApJL,527,81L

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ASPConf.Ser.211:Proceedingsoftheworkshop‘MassiveStellarClus-ters’heldinStrasbourgNov.1999;eds.A.Lancon,C.M.Boily

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