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Can Supermassive Black Holes Sufficiently Heat Cool Cores of Galaxy Clusters

Can Supermassive Black Holes Sufficiently Heat Cool Cores of Galaxy Clusters
Can Supermassive Black Holes Sufficiently Heat Cool Cores of Galaxy Clusters

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Can Supermassive Black Holes Su?ciently Heat Cool Cores of Galaxy Clusters?Yutaka Fujita 1,2,and Thomas H.Reiprich 3yfujita@th.nao.ac.jp ABSTRACT Activities of a supermassive black hole or active galactic nucleus in the cen-tral galaxy of a cluster of galaxies have been promising candidates for heating sources of cool cluster cores.We estimate the masses of black holes using known correlations between the mass of a black hole and the velocity dispersion or the luminosity of the host galaxy.We ?nd that the masses are ~108?9M ⊙and the central X-ray luminosities of the host clusters (“the strength of the cooling ?ow”)are well below the Eddington luminosities.However,we do not ?nd a correlation between the mass and the central X-ray luminosity of the host cluster.If the heating is stable,this seems to contradict a simple expectation if supermassive black holes are the main heating source of a cluster core.Moreover,if we assume a canonical energy conversion rate (10%),black holes alone are unable to su?-ciently heat the clusters with strong centrally peaked X-ray emission (“massive cooling ?ows”)over the lifetime of cluster cores.These results may indicate that massive cooling ?ows are a transient phenomenon,which may be because the black holes are activated periodically.Alternatively,in the massive cooling ?ow clusters,the energy conversion rate may be larger than 10%,that is,the black holes may be Kerr black holes.

Subject headings:galaxies:active—cooling ?ows—galaxies:jets—galaxies:nu-clei

1.Introduction

Clusters of galaxies are the largest gravitationally bound virialized objects in the uni-verse.They are?lled with hot X-ray gas with temperatures of~2–10keV.The gas is thought to be heated by the energy released when clusters gravitationally collapsed.While the gas cooling through the X-ray radiation is ine?cient in most regions of a cluster,it is very e?cient in the central region because of the high gas density.From X-ray observations, it can be estimated that the thermal energy of the gas within cluster cores is lost radiatively within~108?9yr.The gas cooling should decrease the temperature and pressure of the gas at the cluster cores,and the weight of the overlying gas should produce gas?ows toward the cluster centers.The?ows are called“cooling?ows”and the idea has prevailed for about30 years(Fabian1994).

Recent X-ray observations showed that the gas in the central regions of clusters is not cooling as much as previously believed.This is indicated by the lack of metal line emission that is characteristic of cooling X-ray gas(e.g.Ikebe et al.1997;Makishima et al.2001; Peterson et al.2001;Tamura et al.2001;Kaastra et al.2001;Matsushita et al.2002).This means that the above simple cooling?ow picture is not correct and that there must be some heating sources balancing the energy loss through X-ray emission in the central regions of clusters.

There are several heating models such as heat conduction(e.g.Takahara&Takahara 1981;Tucker&Rosner1983;Friaca1986;Gaetz1989;B¨o hringer&Fabian1989;Sparks1992; Saito&Shigeyama1999;Narayan&Medvedev2001),acoustic waves propagating from the outside of a cluster core(Fujita,Suzuki,&Wada2004),or magnetohydrodynamic(MHD) e?ects(Makishima et al.2001).At present,the most promising candidate for the heating source is the supermassive black hole at the center of the giant elliptical cluster-center galaxy (e.g.Tucker&Rosner1983;Rephaeli1987;B¨o hringer&Mor?ll1988;Binney&Tabor1995; Soker et al.2001;Ciotti&Ostriker2001;B¨o hringer et al.2002;Churazov et al.2002;Soker, Blanton,&Sarazin2002;Reynolds,Heinz,&Begelman2002;Kaiser&Binney2003).In fact,the Chandra X-ray observatory has shown that the strong activities of the supermassive black holes disturb hot X-ray gas in the central regions of clusters(e.g.Fabian et al.2000; McNamara et al.2000;Blanton et al.2001;McNamara et al.2001;Mazzotta et al.2002; Fujita et al.2002;Johnstone et al.2002;Kempner,Sarazin,&Ricker2002;Takizawa et al. 2003).In many clusters,bubbles of high energy particles have been found;it is expected that jets produced by the supermassive black holes in?ate those bubbles.Moreover,numerical simulations have suggested that the bubbles move outward in a cluster by buoyancy,thus mixing the surrounding hot X-ray gas(e.g.Churazov et al.2001;Quilis,Bower,&Balogh 2001;Saxton,Sutherland,&Bicknell2001;Br¨u ggen&Kaiser2002;Basson&Alexander

2003).As a result of the mixing,hot X-ray gas in the outer region of the cluster is brought into,and subsequently heats the cluster center.Moreover,Chandra found that acoustic waves formed through jet activities are propagating in the hot X-ray gas of the Perseus cluster(Fabian et al.2003).Through the viscosity of the gas,the waves may heat the surrounding gas.

The mass of a supermassive black hole generally needs to be large(~109?10M⊙)to balance the cooling of X-ray gas regardless of the actual heating mechanism(e.g.bubbles, waves,and so on),if the strong X-ray emission from the cluster is not a transient phe-nomenon(Fabian,Voigt,&Morris2002).Moreover,relatively high heating e?ciency may be required.For example,assuming Bondi accretion,XMM-Newton observations showed that the supermassive black hole at the center of the Virgo cluster has to convert5%of the rest mass of the accreted gas into thermal energy of the surrounding gas to prevent cooling at least at present(Churazov et al.2002,see also Di Matteo et al.2003).This is close to a canonical value that is often used in this kind of studies(~10%).In this paper,we derive the masses of supermassive black holes and compare the maximum energy they can produce with the total energy released as X-rays from the central regions of the clusters.In this paper,we assume h=0.7(H0=100h km s?1Mpc?1),?0=0.3,andΛ=0.7unless otherwise noted.

2.Samples and Analysis

2.1.Black Hole Masses

We study53clusters that have been observed with the ROSAT satellite(Peres et al. 1998),and belong to the X-ray?ux limited sample of55clusters(Edge,Stewart,&Fabian 1992).Unfortunately,clusters of galaxies are generally distant,and the mass of the super-massive black hole at the center of a cluster cD galaxy has been directly measured only for a few clusters.However,it has been known that the mass of the black hole is related to the properties of the host https://www.doczj.com/doc/a111028415.html,ing HST and other observations,the relations have been determined more exactly than early studies(e.g.Magorrian et al.1998).In this paper,we use the relations between the black hole and the host galaxy to obtain the black hole mass. The mass of the supermassive black hole at the center of a cluster cD galaxy can be obtained from empirical M BH–σand M BH–M R relations,where M BH is the mass of a supermassive black hole,σis the velocity dispersion of stars in the host galaxy,and M R is the R-band absolute magnitude of the host galaxy.For the M BH–σrelation,we adopt

log(M BH/M⊙)=(8.12±0.07)+(3.75±0.3)log(σ/200km s?1)(1)

(Gebhardt et al.2000),and for the M BH–M R relation,we adopt

log(M BH/M⊙)=?(0.50±0.02)M R?(3.33±0.48)(2) (McLure&Dunlop2002).The coe?cients are slightly di?erent from those in the original papers because of di?erences in the assumed cosmological parameters.There are more recent studies of the M BH–σrelation that give steeper slopes;Tremaine et al.(2002)obtained4.02 and Ferrarese(2002)found4.58.Tremaine et al.(2002)discussed the di?erence between Tremaine et al.(2002)and Ferrarese(2002)and indicated that the large value obtained by Ferrarese(2002)is due to inappropriate treatment of central velocity dispersion.We con?rmed that the di?erence between Gebhardt et al.(2000)and Tremaine et al.(2002)is so small that it does not a?ect the results in this paper(see Figure26in Pinkney et al. 2003).More recently,Pinkney et al.(2003)studied the M BH–σrelation only for early-type galaxies and the slope they obtained is almost the same as that obtained by Gebhardt et al. (2000),although the number of galaxies in the sample is only10.From these reasons,we use the result of Gebhardt et al.(2000).The optical data for the galaxies at cluster centers,such as the velocity dispersions and absolute magnitudes,are obtained from the HYPERLEDA database1.If there are several measurements for a given cluster,we adopted the latest one. Among the53clusters,the velocity dispersions of the central galaxies are measured for29 clusters.Since there are only14galaxies for which the R-band magnitudes are obtained,we use B-band magnitudes for other galaxies;B-band magnitudes have been measured for40 galaxies including the above14galaxies.For the galaxies for which only B-band magnitudes are obtained,the B-band magnitudes are transformed to the R-band magnitudes using B–R color,where the color is assumed to be the average of the14galaxies,B–R=1.67±0.01. The black hole masses are shown in Table1;the black hole mass derived from the M BH–σrelation is referred to as M BH,σand that derived from the M BH–M R relation is referred to as

M BH,M

R .There are43clusters for which M BH,σor M BH,M

R

can be determined.The errors

in the black hole masses are calculated using the worst case ranges given in equations(1) and(2).

2.2.X-Ray Luminosities

In addition to comparing current X-ray luminosities of clusters and the masses of the central black holes,we compare the total energy released in X-rays from the central region of clusters throughout the cluster lifetime with the maximum energy that the black holes can

supply.We use the ROSAT data obtained by Peres et al.(1998).While data from Chandra and XMM-Newton might be better suited for our purpose,ROSAT data are the only ones available for a su?ciently large number of clusters to conduct a statistically relevant uniform study.

The hot gas in a cluster core loses its thermal energy through X-ray emission.Without an energy supply,the gas temperature would go to zero within~108?9yr(Fabian1994). The total energy that must be supplied to prevent the cooling depends on the age of the cluster core(t age),which should be larger than that of the cluster itself.In this paper,we assume that cluster cores formed at z~1because numerical simulations indicated that X-ray emission from a cluster has not changed much since then(Eke,Navarro,&Frenk 1998),and because a signi?cant part of the X-ray emission from a cluster comes from its central region including the core.Note that the simulations done by Eke et al.(1998)include neither cooling nor heating.The hot gas in the central region of a cluster is generally in pressure equilibrium with the gravity of dark matter because of the small sound crossing time.Therefore,the simulations done by Eke et al.(1998)indicate that the gravitational structure of cluster cores formed at z~1.In actual clusters,observations suggest that both cooling and heating are e?ective but they appear to be well balanced(Peterson et al.2001; Tamura et al.2001;Kaastra et al.2001).In fact,Allen,Schmidt,&Fabian(2001)showed that temperature pro?les among clusters are similar and that the central temperatures drop only a factor of1/2even for“cooling?ow clusters”(see also Ikebe2001).Although there is no consensus on the mechanism that keeps the balance(for thermal conduction,see Ruszkowski &Begelman2002;Kim&Narayan2003),the balanced cooling and heating may mean that the gas motion in the central regions of clusters is slow and that the X-ray emission from cluster cores re?ects the gravitational structure there,which formed at z~1.Since there is no reason that z=0is a special epoch,we assume that the cooling and heating have been balanced since the formation of the cluster core,and thus we assume that the X-ray emission from the core has not changed much since z~1.In fact,Valdarnini(2002) performed numerical simulations including both cooling and heating and showed that the X-ray luminosity of a cluster has not changed or even has decreased since z~1.2(high resolution simulations in his Figure11).The heating sources of the gas in these simulations are supernovae,not supermassive black holes.However,since the radiatively cooled gas is the fuel for both sources,the results should be at least qualitatively the same.The reason for the decrease in X-ray luminosity is that radiative cooling dominates heating before enough stars are formed out of the cooled gas.After the cooling and heating are balanced,the central gas density and X-ray luminosity of the cluster decrease.Therefore,although we estimate the required energy supply from a black hole,assuming that the X-ray luminosity of a cluster core has been unchanged for z 1,the supply may be underestimated if we?x

the X-ray luminosity at the observed value at z ~0.

On the other hand,semi-analytic models of galaxy formation predict that the supermas-sive black holes at galaxy centers gain most of their mass at z 1–2(Haehnelt &Kau?mann 2002;Hatziminaoglou et al.2003;Volonteri,Haardt,&Madau 2003).Thus,we also assume that the formation epoch of the supermassive black holes is z ~1.

Since we assume that cluster cores formed at z ~1,the hot X-ray gas within radii where the cooling time of the gas is t age =7.7Gyr (the look-back time for z =1)must be heated.Peres et al.(1998)listed the X-ray luminosities of 53clusters within radii where the cooling time of hot X-ray gas is 13Gyr.In a classical cooling ?ow model,the central X-ray luminosity is correlated with the strength of the cooling ?ow (Fabian 1994).We modify the central X-ray luminosities listed by Peres et al.(1998)into those for the cooling time of

7.7Gyr to estimate the energy supplied by supermassive black holes.

In order to modify the central X-ray luminosity,we need to ?nd the density pro?le of the X-ray gas in a cluster.We assume that a cluster is isothermal.For “cooling ?ow clusters,”Chandra observations showed that the temperature at the center is ~1/2of the average (Allen et al.2001).However,this temperature drop does not a?ect photon counts in the ROSAT band (at most ~10%,see Mohr et al.1999).A parametric description of the cluster gas density pro?le has often been used,and it is called the β-model (e.g.Cavaliere &Fusco-Femiano 1976).Assuming spherical symmetry,the model

S X (R )=S 0 1+

R 2

r 2c ?3β/2.(4)

If excess emission (so-called cooling ?ow)is seen in the innermost region of a cluster,the surface pro?le can be ?tted with two β-model functions

S X (R )=S 01 1+R 2r 2c 2

?3β2+1/2,(5)where r c 1S 02.In this case,the density pro?le is given by

ρgas (r )2=ρ2gas ,0,1 1+r 2r 2c 2 ?3β2,(6)

whereρgas,0,1>ρgas,0,2.

The results of the?ts are shown in Table2;the results of single-β-model?ts are rep-resented by subscript2.Among106clusters investigated by Reiprich&B¨o hringer(2002), there are24clusters that overlap with the53clusters studied by Peres et al.(1998)and that the qualities of the data are high enough.For these clusters,we?t the surface bright-ness with twoβmodels without the assumption ofβ1=β2and obtain the density pro?le (equation[6]).The selection criteria of the clusters with high data quality are(1)ROSAT PSPC pointed observations had been made,and(2)S02>0and S01>S02.These clusters are indicated by‘RB2’in Table2.

Among the remaining,22clusters were studied by Mohr,Mathiesen,&Evrard(1999). For the clusters with central excess,they?t the surface brightness and obtain density pro?les assuming thatβ1=β2.Since they presented only the central gas density,ρgas,obs,0,for the clusters with a central excess,we estimateρgas,0,1andρgas,0,2by solving equations

ρ2gas,0,1+ρ2gas,0,2=ρ2gas,obs,0,(7)

ρgas,0,2= S02r c1

ρgas(r[t cool=13?h?1/2Gyr])=

13?h?1/2

Here r(t cool=13?h?1/2Gyr)corresponds to r cool,P/?h.We de?ne r cool,FR≡r(t cool=7.7Gyr) to be discriminated from r cool,P.

Peres et al.(1998)also derived X-ray luminosities of clusters within their cooling radii, L P(

L FR(

other hand,L FR(

There are two possibilities to overcome this di?culty.One is that the radiative e?ciency ηis larger than the canonical value(0.1).This happens if the black holes are rapidly rotating Kerr black holes.In this case,the maximum value ofηis0.42,based on the binding energy of particles on the innermost stable circular orbit(Shapiro&Teukolsky1983).Moreover, Kerr holes also alter the energy that can be stored and extracted from the black holes(e.g. via the Blandford-Znajek mechanism).The other possibility is that a massive cooling?ow or strong X-ray emission from a cluster core is a transient event.This may also be consistent with the fact that there is no correlation between the mass of a black hole and the X-ray luminosity of a cluster(Figure2),which may indicate that the cooling and heating at the cluster center are not exactly balanced(see Soker et al.2001).Here,we assume that the supermassive black holes we selected are an unbiased sample of the whole supermassive black hole population,and that the average of the energy conversion rates,ε,can be regarded as the time-average of the conversion rate for a black hole.However,since our cluster sample is ?ux-limited,the bright clusters tend to be preferentially selected.In order to correct for this e?ect,we take the average ofεby weighting with1/V max,where V max is the maximum volume within which clusters with a given luminosity can be observed.The volume is represented by ,where L X is the total X-ray luminosity of a cluster obtained from David et al. V max∝L3/2

X

(1993).For43clusters for which we could estimate the mass of supermassive black holes,the

×10?2.Moreover,we describe below how we correct average conversion rate is ε =6.4+4.7

?1.6

the bias attributed to the10clusters for which we could not estimate the black hole masses. The X-ray luminosity and the back hole mass of a cluster are not correlated(Figure2),and the average black hole mass for the43clusters is6.3×108M⊙.Assuming that the black hole mass for the remaining10clusters is the same as the average mass,we can estimate εfor these clusters.If we include these10clusters,the average of the conversion rate is ×10?2.Since ε is much smaller than one,the supermassive black holes can

ε =6.6+4.7

?1.6

heat the surrounding hot X-ray gas of the clusters unless the past X-ray luminosities were 20times larger than the current values.Some of the results of numerical simulations by Valdarnini(2002)show that the X-ray luminosity of a cluster is increasing toward higher

redshift(high resolution simulations in his Figure11).However,the increase is at most a factor of10.

There is one more possibility;the M BH–σand M BH–M R relations we used may not apply to the supermassive black holes in the cD galaxies in clusters.As far as we know, there are two clusters for which the masses of the supermassive black holes have been directly measured.One is the Virgo cluster and the other is Cygnus A.The mass of the supermassive back hole at the center of the Virgo cluster is(3.2±0.9)×109M⊙(Macchetto et al.1997) and that of Cygnus A is(2.5±0.7)×109M⊙(Tadhunter et al.2003).On the other hand,

the masses obtained from the M BH–σrelation are3.1+11.3

?2.5×108M⊙and3.3+12.0

?2.6

×108M⊙,

respectively(Table1).Thus,the values obtained from the M BH–σrelation are signi?cantly smaller than those directly measured.However,since there are only two samples,it is premature to conclude that the discrepancy generally exists for cD galaxies.

4.Conclusions

We estimated the masses of supermassive black holes,M BH,at the centers of43clusters of galaxies included in an X-ray?ux limited sample.We showed that M BH~108?9M⊙using an empirical relation between M BH and the velocity dispersion(or the luminosity) of the host galaxy.The central X-ray luminosities of the host clusters are well below the Eddington luminosities.We found that there is no correlation between M BH and the central X-ray luminosity of the cluster core.This seems to contradict a simple expectation if a supermassive black hole is the main heating source of the cluster core.We also showed that strong X-ray emission observed in some cluster cores may not be sustained by the heating by supermassive black holes for the ages of the cluster cores.These results may indicate that the strong X-ray emission is a transient phenomenon,which may be because the black hole activities are periodic.Moreover,the clusters with the strong X-ray emission may be very e?ectively heated by Kerr black holes.

We thank the anonymous referee for useful suggestions.We also thank T.E.Clarke, I.Tanaka,Y.Sato,M.Machida,K.Shimasaku,T.Goto,M.,Enoki,M.Nagashima,S. Iwamoto,N.Yoshida,K.Asano,and M.Kino for useful comments.Y.F.was supported in part by a Grant-in-Aid from the Ministry of Education,Culture,Sports,Science,and Technology of Japan(14740175).T.H.R.acknowledges support by the Celerity Foundation through a postdoctoral fellowship.

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Table1.Cluster and Black Hole Parameters.

ClusterσM R M BH,σM BH,M

L FR(

R

(km s?1)(108M⊙)(108M⊙)(1044erg s?1)

Table1—Continued

L FR(

R

(km s?1)(108M⊙)(108M⊙)(1044erg s?1)

a The R-band magnitude is determined from the B-band magnitude by B?R=

1.67.

Table2.Fitting Parameters.

Cluster zρgas,0,1ρgas,0,2r c1r c2β1β2ref a (10?27g cm?3)(10?27g cm?3)(kpc)(kpc)

Table2—Continued

Cluster zρgas,0,1ρgas,0,2r c1r c2β1β2ref a (10?27g cm?3)(10?27g cm?3)(kpc)(kpc)

a References–RB1:oneβ-model?ts by Reiprich&B¨o hringer(2002),RB2:clusters in the catalogue of Reiprich&B¨o hringer(2002)?tted with twoβmodels,MME:Mohr et al.(1999),and M:Matsushita et al.(2002)

10M BH, σ (M M B H , M R ( Fig. 1.—Black hole mass derived from the M BH –σrelation (M BH ,σ)versus that derived from the M BH –M R relation (M BH ,M R )for 26clusters for which both velocity dispersion and

absolute magnitude are measured.The line indicates M BH ,M R =M BH ,σ.

10L FR (

ε

10

10

L FR(

Fig. 3.—The central X-ray luminosity of a cluster,L FR(

with solid errors)or the M BH–M R relation(open circles with dotted errors).

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