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Mem.S.A.It.Vol.00,0 (cid:13)c SAIt 2008 Memoriedella A deep radio and X-ray view of cluster formation at the crossroads of filaments J. Bagchi1,R.J.vanWeeren2,S.Raychaudhury3,H.J.A.Ro¨ttgering2,H.T.Intema2, 1 1 F.Miniati4,T.A.Enßlin5,M.Markevitch6,andT.Erben7 0 2 1 Inter-UniversityCentreforAstronomyandAstrophysics(IUCAA),Pune411007,India n 2 LeidenObservatory,LeidenUniversity,POBox9513,2300RALeiden,TheNetherlands a 3 SchoolofPhysicsandAstronomy,UniversityofBirmingham,Edgbaston,Birmingham J B152TT,UK 4 4 Physics Department, Wolfgang-Pauli-Strasse 27, ETH-Zu¨rich, CH-8093 Zu¨rich, 2 Switzerland 5 Max-Planck-Institut fu¨r Astrophysik, Karl-Schwarzschild-Str.1, PO Box 1317, 85741 ] O Garching,Germany 6 Harvard-SmithsonianCenterforAstrophysics,60GardenStreet,Cambridge,MA02138, C USA . 7 Argelander-Institutfu¨rAstronomie,Universita¨tBonn,AufdemHu¨gel71,D-53121Bonn, h Germany p - e-mail:[email protected] o r t s Abstract. DeepX-raydatafromChandraandXMM-Newton,andGMRTradiodataare a [ presentedforZwCl2341.1+0000,anextremelyunusual andcomplex mergingclusterof galaxies at the intersection of optical filaments. We propose that energetics of multiple 1 mergersandaccretionflowshasresultedinwide-spreadshocks,accelerationofcosmicray v particles and amplification of weak magnetic fields. This results in Mpc-scale peripheral 9 radiorelicsandhalolikenon-thermalemissionobservednearthemergingcenter. 2 6 Keywords.Galaxies:clusters:general–Galaxies:clusters:individual:ZwCl2341.1+0000 4 – X-rays: galaxies: clusters – Radio continuum: galaxies – Shock waves – Cosmology: 1. Large-scalestructureofUniverse 0 1 1 1. Introduction tersarestillgrowingbymatteraccretionatthe : v junction of large scale filaments of galaxies, i Galaxy clusters grow by mergers of smaller mediatedbythegravityofdark-mattercompo- X subclusters and galaxy groups as predicted nent.KeypropertiesfortestingmodelsofLSS r byhierarchicalmodelsoflarge-scalestructure formationinclude the total energybudgetand a (LSS) formation.For the most massive merg- the detailed temperature distribution within a ersa significantamountofenergyis released; cluster,whicharebothstronglyaffectedbythe upto1063−1064 erg,accordingto thesemod- cluster’smergerhistory.Moreover,thephysics els. All massive clusters have undergonesev- of shock waves in the tenuous intra-cluster eralmergersintheirhistoryandpresentlyclus- Bagchietal.:ZwCl2341.1+0000:deepradioandX-rayview 1 medium (ICM) and the effect of cosmic-rays distributed roughly along a north-south axis, (CR; relativistic particles) on galaxy clusters spanning &4 Mpc. A network of several fila- are all fundamental for our understanding of mentsofgalaxiesareseen branchingofffrom LSSformation. the mainstructuretowardstheeastandnorth- Diffuse radio sources with steep spectra eastforminga‘cosmic-web’(Fig.1&Fig.2). (α . −0.5), not directly associated with indi- vidual galaxies, are observed in a number of 2. RadioandX-rayObservationsof clusters ( cf. review by Ferrariet al. (2008)). ZwCl2341.1+0000 Largescale(l&500kpc)diffuseradiosources in clusters are commonly divided into ‘radio ForprobingtheBremsstrahlungemissionfrom halos’ and ‘radio relics’. Radio halos have the diffuse,hot ICM of this remarkablelarge- smoothmorphologies,areextendedwithsizes scale structure, deep X-ray observations with &1 Mpc, unpolarized, and are found at the Chandra and XMM-Newton were obtained. centers of clusters, co-spatial with the X-ray The X-ray emission is detected for about 2.5 emitting hot ICM gas. Giant radio relics are Mpc in the N - S direction and an extension foundontheclusterperiphery,withsizesupto towards the east is also visible, similar to the several Mpc, sometimes showing arc or ring- patternofgalaxydistribution.InFig.2wealso like structures, and are highly polarized (p∼ show the GMRT 610 MHz radio contourssu- 10-50% at 1.4 GHz). They are probably sig- perposedontheChandraACIS-IX-rayimage. natures of electrons accelerated at large-scale In addition to N - S X-ray emission roughly shocks. The vastmajority of clusters with ex- followingthefilamentofgalaxiesvisibleinthe tendeddiffuseradiosourcesaremassive,X-ray optical image, embedded within the extended luminous and are merging systems. Although diffuseemission,wecanidentifyseveralother stillunderdebate,shocksandturbulence,both prominentX-rayemittingsystems,whichmost causedbymergers,arethoughttoberesponsi- likely representhotgasassociated with merg- blefor(re)acceleratingelectronstohighlyrel- inggroupsandclusters(Fig.1). ativistic energies,andsynchrotronradiationis The overallcluster temperaturein a r=4′ producedinthepresenceofmagneticfieldsin region (roughly1 Mpc or close to r ), mea- 500 the ICM. Thereforedeep radio and X-ray ob- sured from the Chandra ACIS-I observation, servationsofmergingclustersmayprovideex- is 4.4±0.6keV. ThecorrespondingX-raylu- tremely important information on the dynam- minosity within the same region in the 0.1– icsofLSSformation. 2.4 keV range is L =2.4×1044 erg s−1, and X ZwCl2341.1+0000,discoveredbyBagchi the bolometric X-ray luminosity being L = bol et al. (2002), is an extremely interesting and 4.6 × 1044 erg s−1(h = 0.71, Ω = 0.27, M complexsystem of galaxies, composedoutof Ω = 0.73). From the XMM-Newton com- Λ several different subclusters arranged along a binedPNandMOSobservations,fromthecen- north-south filamentary axis extending upto tral r = 4′ region, we obtain an average tem- at least ∼4 Mpc. It is probably a very large peratureof 4.7±0.5 keV. Thusboth Chandra and massive cluster coming together at the andXMM-Newtonmeasuredtemperaturesare junction of supercluster filaments. A 2.5 Mpc consistentwitheachother. scale diffuse radio emission was detected in Deep GMRT radio maps were published the main filamentary structure (Bagchi et al. by us recently (van Weeren et al. 2009) at 2002;Giovanninietal. 2010)whichmakesit 610,240and150MHz.Thesemaps(specially uniqueandahighlyvaluablesourceforcosmo- 610 MHz map shown here in Fig. 2) success- logicalstudies.Thesystemislocatedatared- fully resolved the compact sources from the shift of z = 0.27, based on SDSS DR7 spec- extended diffuse emission of extremely low troscopic redshifts of several galaxies in the surface brightness (only 100 - 200 µJy/beam vicinity.Agalaxyisodensitymapderivedfrom at 610 MHz), which was found to be located SDSS imaging data shows an elongated clus- mainlyintwoMpc-scaleradiostructurestothe ter of galaxies, including several subclusters northandsouthofthecluster,cappingthetwo 2 Bagchietal.:ZwCl2341.1+0000:deepradioandX-rayview Fig.1.Leftpanel:TheopticalR-bandimageofmergingsystemZwCl2341.1+0000obtainedfromWFIat theESO2.2mtelescope.TheoverlaidcontoursshowthethermalX-rayemissionintheenergyrange0.5– 3keVobservedwithXMM-Newton.Rightpanel:Grey-scaleversionofthesameX-rayemissionobserved with XMM-Newton. Both images cover about 4 Mpc on a side at redshift z=0.27 (Raychaudhury et al. (2011)). endsofX-rayemittinghotgasandthecentral that is occurringpreferentiallyalongthe NW- optical filament. We interpretthis structure as SEaxis–i.e.,alongthemajorfilamentclearly beingaperipheraldoubleradiorelic,wherethe seen in the distribution of galaxies. An ad- particlesareacceleratedbythediffusiveshock ditional arm of the X-ray emission extends acceleration (DSA or Fermi-I) mechanism in from the middle of the cluster towards NE, outwardpropagatingshockwavesgeneratedin roughly coinciding with another filamentary major cluster merger activity observed at the galaxystructure.ZwCl2341.1+0000maythus center (cf. Bykov et al. (2008)). The merger representbyfarthemostcomplexmergercon- axis is clearly along the galaxy filament, with figurationfoundamonggalaxyclusters.Dueto radiorelicsplacedtangentialtothisaxis,asex- its highly unrelaxed dynamical state revealed pected in a merger-shockgeometry.However, by our X-ray data, this system may provide to the limits of surface-brightness sensitivity a rare glimpse into the early steps of assem- achieved(∼30µJynoisefora5′′beamat610 bly of a galaxy cluster at the junction of fil- MHz,∼12hon-sourcetime),nocentralradio- aments. In addition, rare detection of diffuse halowas detectedinourGMRT observations. radioemission fromsuch a system will throw Possiblereasonisthatsomeoftheshortbase- much light on the dynamicsof cluster forma- linesinthe GMRTobservationswereaffected tion.Theoptical,radioandX-rayobservations by RFI and had to be flagged, which allowed presented in this paper firmly establishes the imaging of spatial scales of < 4′ only (at 610 linkofthismergertotheaxisofasupercluster MHz).Averydeep327MHzGMRTobserva- filament along which the merger takes place. tionisinpreparationtoresolvethisissue. This work represents a substantial advance in the field, because it probes several important componentsofthecosmicenvironment:inter- 3. Discussion galacticgas,magneticfields,andcosmic-rays. Largescaleradioemissionindicatesthatmag- The X-ray images clearly reveal a highly un- neticfieldsofappreciablestrengtharepresent relaxedclusterexperiencingacomplexmerger Bagchietal.:ZwCl2341.1+0000:deepradioandX-rayview 3 notonlyinthe ICM butalso inthediffusein- tergalacticmedium,i.e.,inthegasthatwillbe shocked as it accretes onto collapsing struc- tures-theprecursorsofvirializedgalaxyclus- ters.Thesearchformagneticfieldsintheinter- galacticmediumisoffundamentalimportance for cosmology(Bonafedeet al. 2010;Dolag 2006). In a recent deep 1.4 GHz VLA observa- tion,Giovanninietal. (2010)presentevidence of2Mpc-scalepolarizedradioemission,mid- way between the peripheral radio relics. The radioemission clearlyfollowsthedistribution of optical galaxies and X-ray emission which might suggest that it is similar to radio ha- los found in dynamically unrelaxed clusters (Ferrarietal. 2008).Thepolarizationvectors (p∼10 - 20%) are very regular, indicating an Fig.2. A radio, optical and X-ray overlay map. The solid contours represent the radio emission at organized magnetic field pattern. This feature 610MHzfromtheGMRTdata[vanWeerenetal. might result from the accretion flow shocks (2009)].Broadbeamof15′′FWHMisusedtoshow in filaments compressing the weak magnetic betterthediffuseradioemission.Theradiocontours fields of the infalling IGM, which is consis- aredrawnat[1,2,4,8,16,32,...]×0.224mJy/beam. tent with a model proposed by Bagchi et al. Dashed contours show the galaxy isodensity con- (2002). An observation of large scale diffuse toursfromSDSS,corresponding roughlytoalimit radioemissionandmagneticfieldsinfilamen- of M = −18.1 (i.e., M∗ +2.4). The dashed con- V tarygalacticenvironmentalsoprovidesafore- toursare drawnat [2, 3, 4, 5,...]galaxiesarcmin−2 tasteoffuturedetections,asamajorgoalofup- with a redshift cut. Grey-scle image is smoothed, cominglowfrequencyradiotelescopeslikethe point source subtracted X-ray emission map from LOFARandLWA istoprobethenon-thermal Chandrainthe0.5-3.0keVenergyband. processesinhundredsofmergingclustersand inthefilamentarycosmic-webofthenearand whichresultedintheradiodata.TheGMRTisana- distantUniverse. tional facility operated by the National Centre for RadioAstrophysicsoftheTIFR,India. 4. Conclusions WehavepresenteddeepX-rayandradioobser- References vations which show that ZwCl 2341.1+0000 Bagchi,J.etal.2002,NewAstron.,7,249 constitutesacomplex,large-scaleensembleof Bonafede, A. et al. 2010, Proc. ISKAF2010 clusters, which are merging at the intersec- ScienceMeeting,TheNetherlands tion of filaments identifiable in optical and Bykov, A. M., Dolag, K. & Durret, F. 2008, X-ray images. Energeticsof multiple mergers SSRv.,134,119 andaccretionflowshasresultedinwide-spread Dolag,K. 2006,AstronomischeNachrichten, shocks, acceleration of cosmic ray particles 327,575 and amplification of weak magnetic fields. Ferrari,C.etal. 2008,SSRv.,134,93 Thisisevidentinapairofgiant,peripheralra- Giovannini, G., Bonafede, A., Ferreti, L., diorelicsandafaint,diffuseradiohaloextend- Govoni,F.,&Murgia,M. 2010,A&A,511, ingmorethan∼1Mpcbetweenthetworelics, L5 followingthelarge-scalefilamentarystructure. Raychaudhury,S.etal. 2011,Inpreparation Acknowledgements. We thank the operations team vanWeeren,R.J.etal. 2009,A&A,506,1083 of the NCRA–TIFR GMRT observatory for help

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