Astronomy&Astrophysicsmanuscriptno.Hi071 February5,2008 (DOI:willbeinsertedbyhandlater) Optical emission from GRB050709: a short/hard GRB in a ⋆ star-forming galaxy 6 0 S.Covino1,D.Malesani2,G.L.Israel3,P.D’Avanzo1,4,L.A.Antonelli3,G.Chincarini1,5,D.Fugazza1,M.L. 0 Conciatore3,M.DellaValle6,F.Fiore3,D.Guetta3,K.Hurley7,D.Lazzati8,L.Stella3,G.Tagliaferri1,M.Vietri9,S. 2 Campana1,D.N.Burrows10,V.D’Elia3,P.Filliatre11,12,N.Gehrels13,P.Goldoni11,12,A.Melandri3,14,S. n Mereghetti15,I.F.Mirabel16,A.Moretti1,J.A.Nousek10,P.T.O’Brien17,L.J.Pellizza12,R.Perna8,S.Piranomonte3, a J P.Romano1,andF.M.Zerbi1 0 1 1 INAF,OsservatorioAstronomicodiBrera,viaE.Bianchi46,I-23807Merate(Lc),Italy 2 InternationalSchoolforAdvancedStudies(SISSA-ISAS),viaBeirut2-4,I-34014Trieste,Italy 2 3 INAF,OsservatorioAstronomicodiRoma,viadiFrascati33,I-00040MonteporzioCatone(Roma),Italy v 4 DipartimentodiFisicaeMatematica,Universita`dell’Insubria,viaValleggio11,I-22100Como,Italy 4 4 5 Universita`deglistudidiMilano-Bicocca,DipartimentodiFisica,piazzadelleScienze3,I-20126Milano,Italy 1 6 INAF,OsservatorioAstrofisicodiArcetri,largoE.Fermi5,I-50125Firenze,Italy 9 7 UniversityofCalifornia,Berkeley,SpaceSciencesLaboratory,Berkeley,CA94720-7450,USA 0 8 JILA,UniversityofColorado,440UCB,BoulderCO80309-0440,USA 5 9 ScuolaNormaleSuperiore,piazzadeiCavalieri7,I-56126Pisa,Italy 0 10 DepartmentofAstronomy&Astrophysics,PennsylvaniaStateUniversity,StateCollege,PA16801,USA h/ 11 LaboratoireAstroparticuleetCosmologie,UMR7164,11PlaceMarcelinBerthelot,F-75231ParisCedex05,France p 12 Serviced’Astrophysique,DSM/DAPNA,CEASaclay,F-91911Gif-sur-YvetteCedex,France - 13 NASA,GoddardSpaceFlightCenter,Greenbelt,MD20771,USA o 14 Universita`degliStudidiCagliari,DipartimentodiFisica,I-09042Monserrato(Ca),Italy r t 15 INAF/IASFMilano“G.Occhialini”,viaE.Bassini15,I-20133Milano,Italy s 16 EuropeanSouthernObservatory-Vitacura,Casilla19001,Santiago19,Chile a : 17 X-Ray&ObservationalAstronomyGroup,Dept.ofPhysics&Astronomy,UniversityofLeicester,LeicesterLE17RH,UK v i X r Abstract. a Wepresentopticalobservationsoftheshort/hardgamma-rayburstGRB050709,thefirstsucheventwithanidentifiedoptical counterpart.TheobjectiscoincidentwithaweakX-raysourceandislocatedinsideagalaxyatredshiftz=0.1606±0.0002. Multiband photometry allowed us to study the broad-band spectral energy distribution. Late-time monitoring places strong limits on any supernova simultaneous with the GRB. The host galaxy is not of early type. Spectra show that the dominant stellarpopulationisrelativelyyoung(∼1Gyr),andthatongoingstarformationispresentatalevelof2–3L/L∗ M⊙/yr.Thisis atleast2ordersofmagnitudelargerthanthatobservedintheellipticalhostsoftheshortGRB050509BandGRB050724.This showsthatatleastsomeshortGRBsoriginateinayoungpopulation.Short/hardGRBmodelsbasedonthemergerofabinary degenerate system are compatible withthe host galaxy characteristics, although there isstill thepossibility of a connection betweenyoungstarsandatleastafractionofsuchevents. Keywords.Radiationmechanisms:non-thermal–Gammarays:bursts–Gammarays:individualGRB050709 1. Introduction ones(duration<2s).Overthepastyears,greatadvanceshave beenmadeinunderstandingtheformerclass,thankstotheob- Gamma-raybursts(GRBs)areshortpulsesofgammaraysoc- servationoftheiropticalandradiocounterparts.However,until curringatrandompositionsinthesky.TwoclassesofGRBsare recently,noopticalemissionfromshortGRBshadbeenidenti- currentlyknown,characterisedbydifferentdurationsandspec- fied(Hurleyetal.,2002),leavingfundamentalquestionsabout tral properties (Kouveliotouetal., 1993). Long GRBs (typi- theirnature,progenitorsanddistancesunanswered. callylasting10–100s)areontheaveragesofterthantheshort Recently,thanksto the Swift andHETE-2satellites, accu- Sendoffprintrequeststo:S.Covino,e-mail:[email protected] rateandrapidlocalisationsofshortGRBshavebecomeavail- ⋆ Based onobservations carriedout atESOtelescopesunder pro- able, enabling deep, sensitive searches at long wavelengths. grammesId075.D-0787and075.D-0468. Swift discovered a weak X-ray counterpart to GRB050509B 2 Covinoetal.:GRB050709inastarforminggalaxy Fig.1.R-bandimageofthefieldofGRB050709,on2005Jul12.41(A)and20.42(B).PanelCshowstheresultofthesubtraction, evidencingafadingsourcecoincidentwiththeChandracounterpart(circle).Theboxescoveraregion30′′×20′′wide. (Gehrelsetal.,2005),located∼ 11′′ awayfromabrightellip- Table 1. Observation log and photometry of the transient tical galaxy at z = 0.2248 (Bloometal., 2005; Hjorthetal., source.Errorsareatthe1σconfidencelevel,whileupperlimits 2005a; Castro-Tiradoetal., 2005). An early-type galaxy areat3σ.DatawerenotcorrectedforGalacticextinction. (Gorosabeletal., 2005) is also associated with GRB050724 Date Instrument Exp. Filter Magnitude (Barthelmyetal., 2005)atz = 0.257(Prochaskaetal.,2005), (UT) (min) forwhichalso an opticalafterglowwassingledoutinsidethe 2005/07/1209:44 FORS2 6 V 24.38±0.10 host(Bergeretal., 2005a;D’Avanzoetal., 2005). Finally,the 2005/07/1407:21 FORS1 6 V >25.00 lineofsightofGRB050813(Retteretal.,2005)liestowardsa 2005/07/2010:16 FORS1 6 V (reference) galaxyclusteratz=0.722.Afewellipticalgalaxieswereiden- 2005/07/3002:37 FORS2 9 V >25.20 tifiedinsidetheXRTerrorcircle,againsupportingtheassoci- 2005/07/1209:57 FORS2 5 R 23.83±0.07 ation with early-type galaxies (Gladdersetal., 2005; Berger, 2005/07/2010:07 FORS1 6 R (reference) 2005b;Prochaskaetal.,2005). 2005/07/3002:54 FORS2 50 R >25.00 GRB050709 was discovered by HETE-2 on 2005 Jul 2005/07/1209:32 FORS2 10 I >23.25 9.94209UT(Villasenoretal.,2005).Itspromptemissioncon- 2005/07/1407:32 FORS1 5 I >24.10 sisted of a single pulse lasting 70 ms in the 3–400keV band, 2005/07/1806:38 FORS1 20 I (reference) followed by a weaker, soft bump ∼ 100 s long. This second 2005/07/3004:10 FORS2 9 I >23.50 episode may be due to the afterglow onset (Villasenoretal., 2005),ortoflaringactivity(Barthelmyetal.,2005;Kingetal., tify variable objects even when blended with nearby sources. 2005; Pernaetal., 2005). In any case, the prompt emission The pointlike object was found to be variable (at the ∼ 10σ propertiesareconsistentwiththoseofashort/hardGRB. level),beingundetectablefromJul14onwards.Thisconfirms Follow-up observations with the Chandra X-ray observa- the independent finding of Hjorthetal. (2005b). Magnitudes tory revealed a faint, uncatalogued X-ray source inside the of the variable source were computed assuming a negligible HETE-2 error circle (Foxetal., 2005a). At the coordinates flux in the reference epoch (see Table 1). Photometry of the α = 23h01m26s.9,δ = −38◦58′39′.′5(0′.′4error),itwas J2000 J2000 transient was performed by inserting artificial stars of known coincidentwithapointlikeobjectembeddedinabrightgalaxy brightnessandcalibratedbyobservingLandoltstandardfields. (Jensenetal.,2005)atz = 0.16(Priceetal.,2005a).Thevari- On Jul 30 we took medium-resolutionspectra of the host abilityofthissourceledPriceetal.(2005b)toproposeitasthe galaxy.ObservationswerecarriedoutwiththeFORS2instru- opticalcounterpartofGRB050709. mentattheVLT-UT1,withthe300Vgrism,coveringthewave- lengthrange6000–9200Å(6ÅFWHM).Fromthedetectionof 2. Observationsanddataanalysis severalemissionlines,amongthemHα,Hβ,and[OII],wede- rivedaredshiftz=0.1606±0.0002.Thisisconsistentwiththe We observed the field of GRB050709 with the ESO Very resultsofFoxetal.(2005b).Therefore,therest-frame B-band LargeTelescope(VLT),usingtheFORS1andFORS2instru- luminosityof the hostis1 LB ∼ 3.5×1042 ergs−1 (∼ 0.10L∗, ments. In our first images, taken on 2005 Jul 12, the point- assuming M∗ = −20.13asdeterminedfromtheSDSSsurvey; like object reported by Jensenetal. (2005) was clearly visi- B Blantonetal.,2003)andthecandidateafterglowliesatapro- blein theV andRbands(Fig.1).Itscoordinatesareα = J2000 jecteddistanceof≈3.3kpcfromthegalaxycore. 23h01m26s.96,δ = −38◦58′39′.′3(0′.′25error),fullyconsis- J2000 tentwiththeChandraposition.Theobjectliesinsideabright galaxy(≈ 1′.′2 away from its nucleus),whose magnitudesare 3. Discussion V = 21.35±0.07,R = 21.08±0.07,andI = 20.63±0.08.To Assuming a power-law flux decay (F(t) ∝ t−α), our observa- searchforbrightnessvariations,wemonitoredthefieldatsev- tionsconstrainαtobegreaterthan1.0intheV band(3σupper eral epochs. Data analysis was performedby adopting a sub- tractiontechnique(Alard&Lupton,1998),wellsuitedtoiden- 1 AssumingacosmologywithΩ =0.3,Ω =0.7,andh =0.71. m Λ 0 Covinoetal.:GRB050709inastarforminggalaxy 3 Fig.2.Broad-bandspectralenergydistributionoftheafterglow Fig.3. DetailsoftheGRB050709hostgalaxyspectrumclose ofGRB050709onJul12.4UT.Thebow-tieshapedregionrep- totheHαandHβlines,showingthatthenarrowemissionemis- resent the simultaneous X-ray spectrum taken from Chandra sionsaresuperimposedonwiderabsorptionfeatures. (Foxetal., 2005b). The dot-dashed and dotted lines indicate theextrapolationoftheopticalandX-rayspectra,respectively. identifies a dominant stellar population ∼ 1 Gyr old (mostly A-dwarfstars),togetherwithayounger,hottercomponent.As limit).Thislimitisconsistentwiththeopticaldecayfoundby indicatedfrom the prominentnebular emission lines, star for- Foxetal.(2005b)usingHSTdatabetween5and10dafterthe mation is still present. From the Hα and [OII] emission lines GRB (see also Hjorthetal., 2005b). A similar limit was also (havingluminosities2.62×1040and2.45×1040ergs−1,respec- puttotheX-rayafterglowdecay.Flaringactivitywasreported tively),weinferastarformationrateof0.21and0.34M⊙ yr−1 in the X-raylightcurve(Foxetal., 2005b). Giventhe limited (Kennicutt, 1998), which corresponds to ∼ 2–3.5 M⊙ yr−1 availabledata,itisdifficulttosaywhetherasimilarbehaviour oncenormalisedto L∗.Thisissignificantlylessthanthattyp- waspresentalsointheopticalband.OurmeasurementsonJul ically observedin longGRB hostgalaxies(Christensenetal., 12arenearlysimultaneouswiththefirstChandraobservation, 2004),butmuchlargerthanthatinthehostsofGRB050509B2 sowecanconstructthebroad-bandspectralenergydistribution (Bloometal., 2005) and GRB050724 (Bergeretal., 2005a), (Fig.2).TheX-rayspectralindexissimilartothatoflongGRB byfactorsof>50and>150,respectively. afterglows(DePasqualeetal.,2003;Nouseketal.,2005).The Themostpopularmodelforshort/hardGRBsisthemerger extrapolation of the X-ray spectrum matches the optical flux of a binary compact object system (e.g. Eichleretal., 1989). (thatis,theoptical-to-X-rayslopeβ =1.1isconsistentwith OX Such events can occur in a late-type, star-forming galaxy theX-rayslopeβ = 1.24±0.35).Thespectrumcorrespond- X (Belczyn´ski&Kalogera, 2001), and give rise to short GRBs ing to the optical colours is quite red (β = 2.3± 0.7), but opt (Perna&Belczyn´ski,2002).Sincethemergingtimescalesmay givenitslargeuncertaintyitisconsistentwithβ atthe1.7σ OX beoftheorderof10Myr,smalloffsetsbetweentheexplosion level.Smalldustextinction(A ≈ 0.2mag;Foxetal.,2005b) V site andthe galaxycoreare possible.Therefore,GRB050709 wouldmaketheintrinsiccolorbluerandfullyconsistentwith might have been produced in a tightly bound system, with the X-ray slope, so that the optical and X-ray emission may a short merging time, similar to GRB050724 (Bergeretal., constituteasinglecomponent.However,thesparsenessofthe 2005a). However, we also note that according to the stan- datapreventsusfromdrawinganyrobustconclusion. dard Faber-Jackson relation, the escape velocity from the Thepropertiesofthehostgalaxyareintriguing.Itscolours GRB050709 host is quite large (about 300 km s−1), so that are consistent with those of an irregular galaxy at z ≈ 0.2 onlyafractionofbinarysystemsmaybeabletoescapeitspo- (Fukugitaetal.,1995),andaremuchbluerthanthoseofellip- tential well. In this case, a larger delay (∼ 1 Gyr) would be ticals(likethoseassociatedwithothershortGRBs).Moreover, consistentbothwiththeobservedoffsetandwiththeageofthe hintsofmorphologicalstructureareseeninourbest-seeingim- older stellar population. A large instantaneous star formation ages.AcloseinspectionofthespectrumshowsthatboththeHα rate would not be expected in this case, even if this does not and Hβ lines have a narrow emission component (FWHM < poseanyproblemforthemergermodel. 6Å)partiallyfillingawider(∼ 12ÅFWHM)absorptionfea- ture(Fig.3).Thisclassicalsignature(Dressler&Gunn,1983) 2 However,manybluegalaxieswerelocatedintheXRTerrorcircle. 4 Covinoetal.:GRB050709inastarforminggalaxy Belczyn´ski,K.,&Kalogera,V.2001,ApJ,550,183 Berger,E.,Price,P.A.,Cenko,S.B.,etal.2005a,Nature,438, 988 Berger,E.2005b,GCN3801 Blanton, M.R., Hogg, D.W., Bahcall, N.A., et al. 2003, ApJ, 592,819 Bloom, J.S., Prochaska, J.X., Pooley, D., et al. 2005, ApJ, in press(astro-ph/0505480) Castro-Tirado,A.J.,deUgarte-Postigo,A.,Gorosabel,J.,etal. 2005,A&A,439,L15 Christensen, L., Hjorth, J., & Gorosabel, J. 2004, A&A, 425, 913 D’Avanzo, P., Covino, S., Antonelli, L.A., et al. 2005, GCN 3690 DePasquale,M.,Piro,L.,Perna,R.,etal.2003,ApJ,592,1018 Dressler,A.,&Gunn,J.E.1983,ApJ,270,7 Eichler, D., Livio, M., Piran, T., & Schramm, D.N. 1989, Nature,340,126 Fox,D.B.,Frail,D.A.,Cameron,P.B.,etal.,2005a,GCN3585 Fig.4.LightcurveoftheGRB050709afterglow(points),com- Fox, D.B., Frail D.A., Price, P.A., et al. 2005b, Nature, 437, paredto those of severalSNe (R band).Zeroextinctionis as- 845 sumedattheGRBsite. Fukugita,M.,Shimasaku,K.,&Ichikawa,T.1995,PASP,107, 945 Gehrels, N., Sarazin, C.L., O’Brien, P.T., et al. 2005, Nature, The presence of pronouncedstar formationactivity in the 437,851 host galaxy of GRB050709, however, prompts us to inves- Gladders,M.,Berger,E.,Morrell,N.,&Roth,M.2005,GCN tigate whether this event could be directly related to young 3798 stars. Recently, it was proposedthat shortGRBs may be pro- Gorosabel,J.,Castro-Tirado,A.J.,Guziy,S.,etal.2005,A&A, duced by giant flares from soft gamma-ray repeaters (e.g. inpress(astro-ph/0510141) Hurleyetal., 2005). However,the luminosityof GRB050709 Hjorth,J.,Sollerman,J.,Gorosabel,J.,etal.2005a,ApJ,630, would be a factor ∼ 103 larger than that of the giant flare L117 fromSGR1806-20.Thepromptemissionpropertiesalsomake Hjorth,J.,Watson,D.,Fynbo,J.P.U.,etal.2005b,Nature,437, thishypothesisunlikely(Villasenoretal.,2005).Furthermore, 859 our photometry can put strong constraints on the presence of Hurley, K., Berger, E., Castro-Tirado, A.J., et al. 2002, ApJ, an unextinguished supernova (SN) exploded simultaneously 567,447 with the GRB (see Fig. 4). Our limits impose a SN >∼ 100 Hurley,K.,Boggs,S.E.,Smith,D.M.,etal.2005,Nature,434, times fainter than a typical type-Ia SN or a bright hypernova 1098 like SN1998bw. Also fainter events like SN1994I and even Jensen, B.L., Jo¨rgensen, U.G., Hjorth, J., et al. 2005, GCN SN1987Aareincompatiblewithourdata.Anassociationwith 3589 a SN seems therefore ruled out for GRB050709 (see also Kennicutt,R.C.Jr1998,ARA&A,36,189 Hjorthetal.,2005a,b;Foxetal.,2005b).Thepropertiesofthe King, A., O’Brien, P.T., Goad, M.R., et al. 2005, ApJ, 630, GRB050709hostare howeverconsistentwiththemodelpro- L113 posedbyMacFadyenetal.(2005),whichadvocatesacollaps- Kouveliotou,C.,Meegan,C.A.,Fishman,G.J.,etal.1993,ApJ, ingneutronstar accretingfroma closenon-compactcompan- 413,101 ion. Such model would also naturally explain the flares ob- MacFadyen, A.I., Ramirez-Ruiz, E., & Zhang, W. 2005, servedintheX-raylightcurve. astro-ph/0510192 Perna,R.,&Belczyn´ski,K.2002,ApJ,570,252 Acknowledgements. DMthanksINAFandtheItalianMIURforsup- port. This research was supported at OABr and OAR by ASI grant Perna,R.,Armitage,P.J.,&Zhang,B.2005,ApJ,636,L29 I/R/039/04. Weacknowledge theexcellent support of theESOstaff. Nousek,J.A.,Kouveliotou,C., Grupe,D.,etal.2005,ApJ,in KH is grateful for support under MIT-SC-R-293291 and FDNAG5- press(astro-ph/0508332) 9210.Wealsothanktheanonymousrefereeforher/hisvaluablecom- Price,P.A.,Roth,K.,&Fox,D.W.2005a,GCN3605 mentsandsuggestions. Price, P.A., Jensen, B.L., Jo¨rgensen,U.G., et al. 2005b,GCN 3612 Prochaska, J.X., Bloom, J.S., Chen, H.-W., et al. 2005, ApJ, References submitted(astro-ph/0510022) Alard,C.,&Lupton,R.H.1998,ApJ,503,325 Retter,A.,Barbier,L.,Barthelmy,S.,etal.2005,GCN3788 Barthelmy, S., Chincarini, G., Burrows, D.N., et al., 2005, Villasenor, J., Lamb, D.Q., Ricker, G.R., et al. 2005, Nature, Nature,438,994 437,855