Mem.S.A.It.Vol.,1 (cid:13)c SAIt 2008 Memoriedella New High-Resolution Sunyaev-Zel’dovich Observations with GBT+MUSTANG T. Mroczkowski1,2,M. J. Devlin1,S. R. Dicker1,P. M. Korngut1,B. S. Mason3,E. 1 1 D. Reese1,C. Sarazin4,J. Sievers5,M. Sun4,andA. Young1 0 2 1 UniversityofPennsylvania,209S.33rdSt.,Philadelphia,PA19104. n e-mail:[email protected] a J 2 NASAEinsteinPostdoctoralFellow. 3 NationalRadioAstronomyObservatory,520EdgemontRd.,CharlottesvilleVA22903. 5 4 DepartmentofAstronomy,UniversityofVirginia,P.O.Box400325,Charlottesville,VA 2 22901. 5 The Canadian Institute of Theoretical Astrophysics, 60 St. George Street, Toronto, ] O OntarioM5S3H8. C Presented15November2010/Submitted23January2011 . h p Abstract.Wepresentrecenthighangularresolution(9′′)Sunyaev-Zel’dovicheffect(SZE) - observationswithMUSTANG,a90-GHzbolometricreceiverontheGreenBankTelescope. o MUSTANGhasnow imaged several massiveclustersof galaxiesinsomeof thehighest- r t resolution SZE imaging to date, revealing complex pressure substructure within the hot s intra-cluster gas in merging clusters. We focus on three merging, intermediate redshift a clusters here: MACS J0744.8+3927, MACS J0717.5+3745, RX J1347.5-1145. In one of [ these merging clusters, MACS J0744.8+3927, the MUSTANG observation has revealed 1 shocked gas that was previously undetected in X-ray observations. Our preliminary re- v sultsforMACSJ0717.5+3745demonstratethecomplementaritytheseobservationsprovide 5 whencombinedwithX-rayobservationsofthethermalemissionandradioobservationsof 0 the non-thermal emission. And finally, by revisiting RX J1347.5-1145, we note an inter- 9 estingcorrelationbetweenitsradioemissionandtheSZEdata.Whileobservationsofthe 4 thermalSZEprobethelineofsightintegralofthermalelectronpressurethroughacluster, . theseredshiftindependentobservationsholdgreatpotentialforaidingtheinterpretationof 1 non-thermalastrophysicsinhigh-zclusters. 0 1 1 : 1. Introduction 1991;Carlstrometal.1996).SZEsurveyslike v thosewiththeAtacamaCosmologyTelescope i X The Sunyaev-Zel’dovich effect (SZE), due to (Kosowsky 2003), the South Pole Telescope r inverse Compton scattering of photons from (Ruhletal. 2004), and Planck (Rossetetal. a the Cosmic Microwave Background (CMB) 2010) are now discoveringnew clusters. With off electrons in the intra-cluster medium notable exceptions(e.g. Komatsuetal. 2001), (ICM)(Zel’dovich&Sunyaev1969),haslong these and other SZE instruments have reso- been sought as a probe of cluster as- lutions ∼1–7′, and therefore do not typically trophysics and cosmology (e.g. Birkinshaw probeclustersonscales.1Mpc. 2 T.Mroczkowski:NewMUSTANGHigh-resolutionSunyaev-Zel’dovichObservations Recently, the MUltiplexed SQUID/TES ArrayatNinetyGHz(MUSTANG),areceiver on the 100-m Green Bank Telescope (GBT), has observed the SZE from clusters at 9′′ resolution (Masonetal. 2010; Korngutetal. 2010).Atthisresolution,thethermalSZEpro- videsaprobeofsubclusterscales,complemen- tary to X-ray studies. In these proceedings, wediscusstheseMUSTANGobservationsand share the preliminary results from a new ob- servationtakeninthe2010Ctrimester.Wedis- cuss the instrument in § 2, present recent re- sults in § 3, and discuss future directions for MUSTANGin§4. Fig.1.MACSJ0744.8+3927: ChandraX-rayim- 2. GBT+MUSTANG agewithMUSTANGSZE4and5-σcontoursover- MUSTANG is a cryogenic, re-imaging focal laid.X-rayanalysisguidedbythisSZEfeatureun- plane camera with an 8 × 8 array of transi- veilsasignificant dropinX-raysurfacebrightness and a rise in temperature, indicating shock-heated tion edge sensor (TES) bolometers cooled to gaswithMachnumberM=1.2±0.2. ≈ 0.3K.TheMUSTANGreceiverwasbuiltat UPennandat90GHzisthehighestfrequency instrumentontheGBT.Usingcapacitivemesh filters todefinethe bandpass,MUSTANG has 0.15–1′scales,butdonotrecovertheextended ≈ 19 GHz bandwidthforcontinuumimaging. SZE flux used to determine scaling relations The array has a 0.63fλ pixel spacing which (e.g.Bonamenteetal.2008).Theobservations yields a well-sampled 42′′ instantaneousfield wepresenthereillustrateMUSTANG’sutility ofviewwith∼9′′resolution.Formoredetails, inrevealingshock-heatedanddisturbedICM. see Dickeretal. (2009) and the MUSTANG website.1 3.1.MACSJ0744.8+3927(z= 0.69) MACS J0744.8+3927 was discovered in the 3. Results ROSAT All-Sky Survey (RASS) and is part Due to common mode subtraction of the at- of the MAssive Cluster Survey (MACS mosphere, spatial scales larger than ∼1.5– Ebelingetal. 2001, 2007), a sample of some 2× the 42′′ instantaneous field of view are of the most massive clusters at z > 0.3. As severelyattenuatedfromMUSTANGobserva- reportedin Korngutetal. (2010), MUSTANG tions. The resulting high-pass filtered obser- observations of this cluster revealed a feature vations of the thermal SZE provide a mea- inthelineofsightpressure,offsetfromX-ray sureoflineofsightintegratedpressure.2They surfacebrightnesspeak(seeFig.1).Infact,the arewell-situatedtocomplementotherSZEin- inside edge of the SZE feature aligns with an strumentsbymeasuringclustersubstructureon X-raysurfacebrightnessdiscontinuity. Using the MUSTANG observations as a 1 http://www.gb.nrao.edu/mustang/ guide,Korngutetal.(2010)analysedtheavail- 2 Other manifestations of the SZE include: the able90ksecofChandradata.Weinterpretthe kinematic SZE, proportional to the line of sight X-raysurfacebrightnesspeakastheintactcore propermotionoftheICM,thepolarizedSZE,pro- of the main cluster, and the MUSTANG se- portional to the transverse motion of the ICM, andthenon-thermal SZE,proportionaltorelativis- lected featureas shock-heatedgas.Thegasto tic electrons in the ICM. See e.g. Carlstrometal. the westofboththe MUSTANG selectedfea- (2002). ture and the second X-ray surface brightness T.Mroczkowski:NewMUSTANGHigh-resolutionSunyaev-Zel’dovichObservations 3 Fig.2. MACS J0717.5+3745 preliminary data: Fig.3. RX J1347.5-1145: MUSTANG S/N map Maetal.(2009)temperaturemapwithMUSTANG withVLA1.4GHzcontoursfromGittietal.(2007) S/N (black)andGMRT600MHz(white)contours overlaid. The SZEdecrement at >3-σcorresponds from vanWeerenetal. (2009) overlaid. The peak totheradioemissionatfoundat>9-σ.Bothareen- SZEdetectioniscospatialwiththehottest(∼24keV, hancedtothesoutheast, outsidethecoolcore.The inwhite) regionidentifiedinthetemperaturemap, centralpointsourceintheMUSTANGmapwasde- andisborderedbytheradiorelictothenorth. tectedat∼40-σ,andisfullysaturatedinthismap. 3.3.RXJ1347.5-1145(z= 0.45) discontinuity is likely the pre-shock medium. We derivea bestfitMachnumberM = 1.2± RXJ1347.5-1145,anothermemberofMACS, 0.2 (Korngutetal. 2010), implying this is a is the most X-ray luminous cluster known. fairly weak shock, marginally consistent with While its X-ray emission is dominated by beingtransonic. its relaxed cool core, there is substantial ev- idence pointing to a high impact parameter merger. High resolution SZE measurements 3.2.MACSJ0717.5+3745(z= 0.55) with Nobeyama (Komatsuetal. 2001) indi- MACS J0717.5+3745, also found in MACS, cated(at∼3-σ)thepresenceofa pressureen- exhibits many signposts of on-going merger hancement to the southeast. The Nobeyama activity.Opticalobservationsshowthiscluster result was soon confirmed by X-ray observa- to have the largest known Einstein radius and tions(Allenetal.2002).MUSTANGlaterim- a complicated mass distribution (Zitrinetal. proved upon the significance of the SZE re- 2010). Radio observations with the VLA and sult to many sigma in its first cluster obser- GMRT have revealed what is likely a relic vation (Masonetal. 2010). Interestingly, ra- (Bonafedeetal.2009;vanWeerenetal.2009) dioemissionfromRXJ1347.5-1145,predomi- due to electrons re-accelerated to relativistic nantlyduetothemini-haloassociatedwiththe energiesbyashock.X-rayobservationsreveal relaxed cool core, shows a similar southeast a complexICM morphologyandregionswith enhancement (Gittietal. 2007). In Fig. 3, we temperatures as high as ∼ 24 keV (Maetal. showthattheSZEdecrementisco-spatialwith 2009), indicatinga sharp pressure discontinu- theradioemission. ity to the southof the radio relic.The prelim- inaryMUSTANGdatahelpcompletethispic- 4. Conclusions&FutureWork ture:the peakin the MUSTANG maps agrees wellwiththepositionofthehotgasseeninthe MUSTANG has been pioneering in the X-ray(seeFig.2). study of cluster astrophysics and substruc- 4 T.Mroczkowski:NewMUSTANGHigh-resolutionSunyaev-Zel’dovichObservations ture through the SZE. The clusters targeted Dicker, S. R., Mason, B. S., Korngut, P. M., in MUSTANG observations to date, however, etal.2009,ApJ,705,226 havebeenchoseninanadhocfashion.Toad- Ebeling, H., Barrett, E., Donovan, D., et al. dress this, we are moving to image a cluster 2007,ApJ,661,L33 sample down to a uniform depth, confirming Ebeling,H.,Edge,A.C.,&Henry,J.P.2001, or rejecting the presence of cluster substruc- ApJ,553,668 turethatwouldaffectSZE scalingrelationsat Gitti, M., Ferrari, C., Domainko, W., Feretti, thelevelofafewpercent. L.,&Schindler,S.2007,A&A,470,L25 We are also working to improveour anal- Komatsu, E., Matsuo, H., Kitayama, T., et al. ysis tools. Notably, we will soon be able to 2001,PASJ,53,57 remove point source contaminationfrom, and Korngut, P. M., Dicker, S. R., Reese, E. D., fit cluster models to, the time ordered data. etal.2010,ArXive-prints This will provide a method by which to fit Kosowsky,A.2003,NewAstronomyReview, MUSTANG data jointly with X-ray data and 47,939 thatfromotherSZEinstruments. Ma, C., Ebeling,H., & Barrett, E. 2009,ApJ, 693,L56 Most tantalizing of all, we have pro- Mason, B. S., Dicker, S. R., Korngut, P. M., posed a successor instrument to MUSTANG, etal.2010,ApJ,716,739 MUSTANG2, which is designed to have a larger instantaneous field of view (4.5′) and Rosset, C., Tristram, M., Ponthieu, N., et al. & 30× higher sensitivity than MUSTANG. 2010,A&A,520,A13+ Ruhl, J., Ade, P. A. R., Carlstrom, J. E., et al. Observations that currently take hours with 2004,5498,11 MUSTANG could be performed in a matter of minutes, imaging the SZE at ∼ 9′′ reso- van Weeren, R. J., Ro¨ttgering, H. J. A., lution and recovering SZE flux out to ∼ 9′ Bru¨ggen,M.,&Cohen,A.2009,A&A,505, 991 scales. This upgrade is crucial as the GBT Zel’dovich, Y. B. & Sunyaev, R. A. 1969, isheavilysubscribed,andMUSTANG’shigh- Ap&SS,4,301 frequency observations demand the best ob- Zitrin, A., Broadhurst, T., Barkana, R., servingconditionsGreenBank,WestVirginia, Rephaeli,Y., & Benitez, N. 2010,ArXive- has to offer. This upgrade will also ensure prints GBT+MUSTANG2willremaincompetitiveas ALMA comes online, as MUSTANG2 will provide an order magnitude better mapping Acknowledgements. We thank M. Gitti, C. Ma, speedforcontinuumemissionat90GHzthan and R. J. van Weeren for sharing data used for the50-elementALMA. comparisonwiththeMUSTANGobservationspre- sented.Weappreciatethelatenightassistancefrom the GBT operators, namely Greg Monk, Donna Stricklin, Barry Sharp and Dave Rose. Support References for TM was provided by NASA through the Allen,S.W.,Schmidt,R.W.,&Fabian,A.C. Einstein Fellowship Program, grant PF0-110077. 2002,MNRAS,335,256 Much of the work presented here was supported by NSF grant AST-0607654. Phil Korngut was Birkinshaw,M.1991,inPhysicalCosmology, also funded by the NRAO graduate student sup- 177 port program. The National Radio Astronomy Bonafede,A.,Feretti,L.,Giovannini,G.,etal. Observatory is a facility of the National Science 2009,A&A,503,707 Foundation operated under cooperative agreement Bonamente,M.,Joy,M.,LaRoque,S.J.,etal. by Associated Universities, Inc. The observations 2008,ApJ,675,106 presentedherewereobtainedwithtelescopetimeal- Carlstrom,J.E.,Holder,G.P.,&Reese,E.D. located under NRAO proposal IDs AGBT08A056, 2002,ARA&A,40,643 AGBT09A052,AGBT09C059andAGBT10A056. Carlstrom, J. E., Joy, M., & Grego, L. 1996, ApJ,456,L75