youjun lu - university of california, los angeles
TRANSCRIPT
YoujunLuNa*onalAstronomicalObservatoryofChina
2016.02.08@Aspen
2/11/16 GCconference@Aspen 1
Collaborators:FupengZHANG(SYSU)QingjuanYU(KIAA)
Ø ConstrainingthespinofthemassiveblackholeattheGalac*ccenterviathemo*onofasurroundingstar(QingjuanYU)
Ø Ontes*ngtheKerrmetricintheGCviastarorbits:theeffectsofstellarperturba*ons(FupengZHANG)
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Outline
Ø Background:GCS-stars,andhypervelocitystars
Ø Dynamicalmodels:TidalbreakupofbinarystarsinthevicinityoftheGCMBH
Ø Confron*ngobserva*onswithmodelsØ Modelpredic*onsØ Summary
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Introduc*on:evidenceforanMBHintheGC
Velocities & Orbits of Stars ! Mass M • = rv
2 /G M • = 4 ×106M⊙
2/11/16 GCconference@Aspen 4Ghezetal;Genzel,etal.
Introduc*on:Galac*ccenterAuniquelaboratoryforstellardynamicsandblackholephysics
v StellarstructuresintheGalac*cCenter(GC)
Ø Youngstellardisk(s):0.04-0.5pcclockwiserota*ngstellardisk(CWS)+acounterclockwisedisk?
Ø S-stars:<4000AU(isotropic)theclosestonetotheMBH(<1000AU)(S0-2/S2,S0-102)
InterplaybetweenstarsandMBH
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Introduc*on:forma*onofS-stars
2/11/16 GCconference@Aspen 6Alexander+Antonini+Chen+Perets+manyothertalks
v Stellardisks:starswereformedinagaseousdisk(insitu)
v S-stars:<4000AU(Sdalforce)Ø Youthparadox:(Ghezetal.2003)
² RejuvenaSonofoldstars?² MigraSonofstarsfromthestellardisk?
(Madigan+ 2009; Baruteau+ 2011, Chen+ 2014)² Exchangecaptures?(Gould & Quillen 2003) Hills mechanism (tidal breakup of binaries)
v WhataretheoriginsoftheS-stars?ArethereanybrightstarsclosertothecentralMBHthantheknownS-stars?v CantheclosestonebeusedtoprobethemetricoftheGCMBHorthedistribuSonofbackgroundstars(stellarremnants)?
Hypervelocitystars(HVSs)intheGalac*chalo
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Brownetal.2014,2015
Ø EscapingawayfromtheMilkywayhalo(hypervelocity)Ø Distancefrom~40kpcto~120kpcfromtheGCØ MainlytypeBstars(3-4M")
Hypervelocitystars(HVSs)
HVSsasapredic*onofHillsmechanism(andothers)aredetectedbylaterobserva*ons!
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21EscapingawayfromMilkyWay
Brownetal.2014,2015
Tidalbreakupofbinarystars v TidalbreakupofbinarystarsinthevicinityoftheMBH
Ø capturedcomponent:S-star(<4000AU)
Ø ejectedcomponent:hypervelocitystar(>700km/s)
Injec*ngbinary
Captured“S-star”
Ejected“HVS”
(Gould&Quillen2003)
(Hills1988;Yu&Tremaine2003)
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HVSs as a prediction of the Hills mechanism (and others) are confirmed by later observations!
Tidalbreakupofbinarystars
180°-Θ≈10°
Weaklyboundbinaries
HVSscanwellmemorizetheinjec*ngdirec*onsoftheirprogenitors,i.e.,theejec*ngdirec*onofanHVSisalmostan*-paralleltotheinjec*ngdirec*onofitsprogenitor. Luetal.2010
Zhangetal.20102/11/16 10S-stars,HVSsandtheMBHintheGC
Ini*allyunboundbinaries
Summaryontheobserva*onalsta*s*csforHVSsandGCS-stars
HVSs: Ø Mass ~3-4M"; B-type
Ø Number: ~21(24) (~100)
Ø Spatial distribution: anisotropic
Ø Distance distribution
Ø Velocity distribution
S-Stars
Ø Mass ~7-15M"; B-type
Ø Number: ~17 (<4000AU)
Ø Spatial distribution: isotropic
Ø Semi-major axis distribution
Ø Eccentricity distribution
Consistent?
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DynamicsofHVSsandS-stars:assumingHillsmechanism
Modelingredient HVSs S-Stars
Injec*ngstellarbinaries
Fromthestellardiskorfrominfinity;(slowly)scaqertothelosscone;1-150M";semimajoraxisandmassra*odistribu*onsofthebinaries;
IMF:intermediatetop-heavyorothersTidalbreakup Ejected Captured(full3-body)
Laterdynamicalevolu*on
TransportfromtheGCtotheGalac*chalo
² Non-andResonantrelaxa*ons;² GRprecessionandGravita*onalwavedecay.
Stellarevolu*on Mainsequenceorpulsar,SNkickLu(withZhangandYu:2010a;2010b;2013;2014)
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ARMAmodelbyMadiganetal.
Confron*ngobserva*onswithmodels:velocitydistribu*onofHVSs
v ReproducingmostHVSsta*s*cs:Ø theory: memory of injecting direction; Ø observation: consistent with being on two disk planes, one of which is the same as that of the CWS disk in the GC; Ø conclusion: HVS probably originated from the GC disk(s).
CWSstellardisk
Luetal.2010
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HVSsfromLAMOST
AnHVSfoundintheLAMOSTGalac*csurvey:
Ø Mass:~9M"(possiblecompanionofS-stars)Ø Velocity:vrf=477km/s(~545km/s)Ø Loca*on:~19kpc(Galactocentricdist.)Ø GCorigin:consistentAnotheroneisrecentlyfoundinLAMOST.
2/11/16 GCconference@Aspen 14Zhengetal.2014
Confron*ngobserva*onswithmodels:velocitydistribu*onofHVSs
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Mainfactors:Ø Theini*aldistribu*onofthe
semimajoraxesofinjec*ngbinaries;
Ø Theperturba*onthatcausestheinjec*onofbinaries.
Canbewellreproducedifbinarystarsperturbedontolow-Jorbitsbydiffusionprocesses/randomwalkorΔJ<<J.
Largeperturba*onsleadtotooflatvelocitydistribu*on.
Slowlydiffusedtothelosscone,binariesaredisruptedbymul*ple*mesofcloseencounter.
CWSdisk
AssumingseveralGalacScpotenSal
ElenaRossiandReemSari’stalksEmptylosscone:slowlydiffusedThroughtheboundaryofthelosscone
Zhangetal.2010
Confron*ngobserva*onswithmodels:S-stars
v ReproducingmostoftheS-starsta*s*csØ semi-majoraxisdistribu*on(importanceofrelaxaSonresonanceandGRdynamics)Ø eccentricitydistribu*on LuwithZhang&Yu(2010;2013)
Semimajoraxis eccentricity
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Stellarmassfunc*on:topheavy
Ø Thenumberra*oofHVSs/S-starscanbere-producedifthestellarini*almassfunc*onistop-heavy,withMFslope∼−1.6(arequirement).– AsteeperIMFleadstoatoolargenumberra*oofHVSstoGCS-stars;a
shallowerone->atoosmallnubmerra*o.
Ø Recentobserva*onsuggeststhattheIMFslopeoftheyoungclusterintheGCis-1.7±0.2,consistentwithourmodelresult.
AfurthersupportforthecommonoriginoftheGCS-starsandtheHVSs.
(Lu,J.etal.,2013;Jessica’stalk)2/11/16 GCconference@Aspen 17
Zhang,Lu,&Yu2013
Modelpredic*ons v Loca*onsofHVSsatthesouthernheimsphere
v EjectedcompanionsoftheS-stars:Ø ∼20-60detectableHVSs(~7-15M")intheGalac*cbulgeandhaloØ locatedinadistance<30kpcfromtheGC,radialvelocity~−500-1500km/s,andpropermo*on~5-20mas/yr(thefirstHVSfoundbyLAMOST~9M")
v CapturedcompanionsofthedetectedHVSsØ ∼20-30capturedstars(~3-7M")intheGC(≲4000AU)Ø theinnermostone:~300-1000AU
v PulsarsintheGCØ ~100within4000AU;~10within1000AU(alsoPfahl&Loeb2004,Dexter&O’Leary2014)Ø theinnermostone:~120-460AU
v HyperfastpulsarsintheGalac*chalo(resulSngfromexplosionofmassiveHVSsandS-stars)
Ø ~severaltotenhyperfastpulsars(>1500km/s)
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Modelpredic*ons:theinnermostcapturedstarwithmass~3-7M"
(Zhang, Lu, & Yu, 2013, 2014)
Testing GR Probability distribution of the semimajor axis
Probability distribution of the pericenter distance
The innermost one is expected to have a semimajor axis ∼300–1500AU and a pericenter distance ∼10–200AU (depending on different injection models) with a significant probability of being closer to the MBH than S2.
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Semimajor axis
Prob
abili
ty
Prob
abili
ty
pericenter distance
Modelpredic*ons:thecloseststartotheMBH
S0-102
S0-102
The predicted probability distribution of the semimajor axis and pericenter distance of the closest star is well consistent with the new observations.
Zhang et al. (2013, 2014)
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Semimajor axis pericenter distance
Prob
abili
ty
Prob
abili
ty
Modelpredic*ons:theclosestpulsartotheMBH
The predicted probability distribution of the semimajor axis and pericenter distance of the closest pulsar to the central MBH. (even closer to the MBH than the captured S-stars)
Zhang, Lu, & Yu (2014)
Gravitational Wave decay í
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Semimajor axis
Prob
abili
ty
Prob
abili
ty
pericenter distance
SummaryØ AlmostallthediscoveredHVSsarespa*allyconsistent
withbeinglocatedontwothindiskplanes,similartotheorienta*onsofsomeGCstructures(CWSdiskandNortharmofthemini-spiral?),whichsupportstheGCorigin.
Ø Weinves*gatethelinkbetweentheHVSsandtheGCS-starsunderthehypothesisthattheybotharetheproductsof*dalbreakupofthesamepopula*onofstellarbinariesbythecentralMBH.Mostofthesta*s*calproper*esofthedetectedHVSsandGCS-starscouldbereproducedundersomebinaryinjec*ngmodels.
Ø Wepredictthesta*s*caldistribu*onsoftheircompanions(ejectedcompanionsforGCS-starsandcapturedcompanionforHVSs)andthepulsarsresul*ngfromthoseejec*ngstarsandcapturedstars,whichmaybetestedbyfutureobserva*ons.
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