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Observations and Analysis of the GK Persei Nova Shell and its "Jet-like" Feature PDF

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Title: willbesetbythepublisher Editors:willbesetbythepublisher EASPublicationsSeries,Vol.?,2016 6 1 0 2 THE GK PERSEI NOVA SHELL AND ITS ‘JET-LIKE’ FEATURE n a E.Harvey1,M.P.Redman1,P.Boumis2 andS.Akras3 J 5 ] Abstract. GKPersei(1901,the‘FireworkNebula’)isanoldbutbrightnova R remnantthatoffersachancetoprobethephysicsandkinematicsofnovashells. S Thekinematicsinnewandarchivallongslitopticalechellespectrawereanal- . ysed using the shape software. New imaging from the Aristarchos telescope h p continues to track the proper motion, extinction and structural evolution of - theknots, whichhavebeenobservedintermittentlyoverseveral decades. We o presentforthefirsttime,kinematicalconstraintsonalargefaint‘jet’feature, r t that waspreviously detected beyond theshell boundary. Theseobservational s constraintsallowforthegenerationofmodelsforindividualknots,interactions a withinknotcomplexes, andthe‘jet’feature. Puttogether,andtakingintoac- [ count dwarf-novaacceleratedwindsemanatingfromthecentralsource, these 1 dataandmodelsgiveadeeperinsightintotheGKPernovaremnantasawhole. v 3 2 9 1 Introduction 0 0 GK Per (1901) is a nearby, historic and spectacular source with a proximity of 470pc . 1 Harrisonetal.,2013. The system is one of only two classical novae observed within a 0 planetarynebulatodate,offeringachancetostudytheevolutionofbothclassesofobject. 6 Aclassicalnovaeventistheresultofthermonuclearrunawayonthesurfaceofawhite 1 dwarfaccretingfrom,typically,amainsequenceoralateGorKtypestarWarner,1995. : v The accreted shell is ejected, at velocities that range from 5x102 to a few x103 km s−1 i X Bodeetal.,2008. Dwarfnovae,whicharealsoexhibitedbyGKPer,arecausedbyanin- stabilityintheaccretiondisksurroundingthewhitedwarfstarOsaki1996. Theseevents r a accelerate winds to the order of 1-6x103 km s−1, see Kafkaetal.,2004 and references therein. It is unknown if their ejection is spherically uniform or intrinsically bipolar Lloydetal.,1997, Porteretal.,1998. The common envelope phase is thought to play a majorrole in the shapingof novaremnantsand planetarynebulae alike. Slower nova 1CentreforAstronomy,SchoolofPhysics,NationalUniversityofIrelandGalway,Galway,Ireland 2NationalObservatoryAthens,IAASARS,I.Metara&V.Pavlou,Penteli,GR-15236Athens,Greece 3Observato´riodoValongo,UniversidadeFederaldoRiodeJaneiro,LadeiraPedroAntonio4320080-090 RiodeJaneiro,Brazil (cid:13)c EDPSciences2016 DOI:(willbeinsertedlater) 2 Title: willbesetbythepublisher eventsarebelievedtohavestrongerdeviationsfromsphericalsymmetrye.g. V1280Sco Chesneauetal.,2012 when comparedto their moreenergeticcounterparts. The system exhibitsapronouncedstreamofemissiontotheNEofthenovashellthatisreminiscent ofajetbutwhoseoriginhasnotbeensettled. Newandarchivalobservationsareusedto explorethestructureandkinematicsoftheGKPernovashell. 2 Kinematicsoftheshell,knotsand‘jet’ Using the Aristarchos telescope in Greece, new imaging was collected of GK Per in September 2014. The observations consisted of three narrow band filters (Hα, [N ii] and[Oiii]),with1800sexposuresineachfilter. ArchivaldataofLiimetsetal.,2012was used and of Lawrenceetal.,1995, Sharaetal.,2012. The imaging was reduced using iraf. Tobuildafullerviewoftheremnantandexaminethe‘jet-like’feature,Manchester EchelleSpectrometer(MES)data were obtainedatthe San PedroMa´rtirobservatoryin Mexico. Position-Velocity(P-V) arrayswere generated. The knotandshell P-V arrays were simulated using the morpho-kinematicmodelling code shape Steffenetal.,20061. AfulldiscussioncanbefoundinHarveyetal. (2016inprep). Shellkinematics: shapemodelingdemonstratesthattheshellmostprobablyconsists ofanoblateelongatedring-likeequatorialstructure(PA∼120◦ andinc∼54◦)withpolar over-densities (Fig. 1). The ‘boxy’ nature of the nebula has long been observed e.g. Seaquistetal.,1989. The position angle derived of the old nova shell fits that of the ‘fossil’ bipolar planetary nebula and the inclination to that of the binary. We find that the‘polarcaps’haveasystematicallylowerexpansionvelocitythantherestoftheshell. In the IRSA archives the longer wavelength WISE Wrightetal.,2010 bands show an abundanceofmaterialalongthesepolarregions,potentiallyhavingasignificanteffecton theirvelocitystructureevolution. Knot Characteristics: In a clump-wind interaction their relative velocities must be considered,asitisbelievedtobethemainmechanismintheshapingoftheclumps. Un- dermoreuniformconditions,sub-sonicclumpshavelongtailsandtheirsupersoniccoun- terparts display short-stubby tails Pittardetal. 2005. There are a variety of tail shapes presentinGKPersuggestingdiverselocalflowconditions. Thesinusoidalnatureofthe tailsoftheknotsalongtheouteredgeoftheshellareevidentinthe1997Hubbleimages inSharaetal.,2012. Thesewavy tailscouldbeattributedtoshapingbythedwarfnova winds,whichcanthusbefoundtohaveavelocityof∼4400kms−1.Bianchinietal.,1986 gaveavelocityestimateofGKPer’sdwarfnovawindsofafew1000kms−1. Kinematics of the jet-like feature: Previously there have been several theories to theoriginofthisfeature,Bodeetal.,2003,Anupamaetal.,2005,Sharaetal.,2012,first mentionedinAnupamaetal.,1993. Light-echocontoursoverIRASimageryhintedthat it predated the nova shell Bodeetal.,2003. As our new kinematic data suggests a low velocity (<17 km s−1 with a Gaussian FHWM rangingfrom 30-40 km s−1) we suggest that the feature may be an illuminated part of the waist of the fossil planetary nebula. Thiswouldalsoexplainthecurvatureandspreadingoutofthefeature. Thereisaslight 1Afulldescriptionofshapecanbefoundathttp://bufadora.astrosen.unam.mx/shape/ Harveyetal.:GKPerKinematics... 3 Fig. 1: Panel(a) showsthe red-blueDopplerdistributionasderivedfromP-Varraysas well as channelmaps overlaid on an image from the Mayall telescope, north is up and eastistotheleft. Panel(b)showstheobservedradialvelocitiesof148knotsdependant ontheir‘y’position,i.e. fromthenorthtosouthofthenebula,wherethegreyscaleisthe equivalentforthemodelcreatedinshape. Panel(c)isthesameasthemiddlepanelexcept thepositionalargumentsarefromtheeasttowest. Fig.2:Examplesofknotsprogressingovertime(2007-2014)andtheircorrespondingP-V arrayandmorpho-kinematicshapemodel.AdditionalepochP-Vinformationisincluded, the knots here are along an axis of symmetry of the nova shell. The ALFOSC P-Vs correspond to the 2007 NOT image and the MES P-Vs correspond to the Aristarchos observationsepoch. augmentationinbrightnessofthislineintheHαand[Oiii]5007Ålinescorrespondingto thelocationofinteractionwithpre-existingmaterialseeninradioandX-rayobservations Anupamaetal.,2005,Balman,2005,Takeietal.,2015. 3 Discussion&Questions One of the main findings from Liimetsetal.,2012was there is no significantdecelera- tionoftheknotsintheSWquadrantofthenovashell,thoughithadbeenlongbelieved 4 Title: willbesetbythepublisher that the shell had been experiencing a stronger interaction with circumbinary material in this quadrant Duerbecketal.,1987. The barrel with polar over-densities structure presented here, as well as the basic bullet crushing time calculation support their find- ing. Takeietal.,2015 indicates the system is moving through less dense material than during the time of the observations of Balman,2005. The derived morphology is de- cidedly oblate, in contrast to the shapes of other nova shells e.g. Ribeiroetal.,2009, Munarietal.,2010. Lloydetal.,1997used a 2.5D codeto investigateremnantshaping for a variety of speed classes and produced rings, blobs and caps as expected but also created oblate remnants. Later Porteretal.,1998 included the effects of a rotating ac- creted envelope,surprisinglythe first panelin their Fig. 2 baresquite a resemblanceto themorphologyderivedhere. SOKER:HaveyoulookedatthejetsinNGC40thatareperpendiculartotheshell? HARVEY:Interestingbutno. Iwillinvestigate. HAMAGUCHI:DoesyourmodelfittheX-raymorphology? HARVEY:Itsuggeststhattheflattenedshellisanintrinsicfeatureandissupportedby thenon-perpendicularpropermotionofthesystemfrom1917-1993,derivedbyBode. DEMARCO:Ontheneonoverabundance,couldGKPerbeabornagainABGstar? HARVEY:In photoionisationsimulations, we conductedusing Cloudy, a significant initialoverabundanceofneonwasrequired.However,thestellarspectrumisnotdeficient inhydrogennorenrichedinhelium,suggestinganovaoriginismorelikely. E.HarveywishestoacknowledgethesupportoftheIrishResearchCouncilforprovidingfundingforthisproject undertheirpostgraduateresearchscheme. TheauthorsgreatlybenefittedfromdiscussionswithDr. Wolfgang Steffen,Prof.JohnMeaburn,Dr.MyfanwyLlyod,Dr.TomilsavJurkicandDr.ValerioRibeiro,amongstothers. References Anupama,G.C.andPrabhu,T.P.1993,MNRAS,335,363 Anupama,G.C.&Kantharia,N.G.2005a,A&A Balman,S¸.2005b,ApJ,933-952,627 Bianchini,A.,Sabbadin,F.,Favero,G.C.,andDalmeri,I.A&A,367-373,160 Bode,M.,O’Brien,T.J.,andSimpson,M.2003,ApJ,L63,600 Bode,M.&Evans,A.2008,ClassicalNovae,2ndedn.,CambridgeAstrophysics Chesneau,O.,Lagadec,E.,Otulakowska-Hypka,M.,etal.2012a,A&A,A63 Duerbeck,H.W.andSeitter,W.C.1987,Ap&SS,467-473,131 Harrison,T.E.,Bornak,J.,McArthur,B.E.,&Benedict,G.F.2013,ApJ,767 Kafka,SandHoneycutt,R.K.2004a,AJ,2420-2429,128 Lawrence,S.S.,MacAlpine,G.M.,Uomoto,A.,etal.1995,AJ,2635,109 Liimets,T.,Corradi,R.L.M.,Santander-Garca,M.,etal.2012b,ApJ,761,34 Lloyd,H.M.,andO’Brien,T.J.,andBode,M.F.1997,MNRAS,137-147,284 Osaki,Y.1996,PASP,39,108 Munari,U.,Ribeiro,V.A.R.M.,Bode,M.F.etal.2010b,MNRAS,525-534,410 Pittard,J.M.,Dyson,J.E.,&etal.2005,MNRAS,361,1077 Poludnenko,A.Y.,Frank,A.,andMitran,S.2004b,ASPconf,APNIII,434,313 Harveyetal.:GKPerKinematics... 5 Porter,J.M.,andO’Brien,T.J.,andBode,M.F.1998,MNRAS,943-948,296 Ribeiro,V.A.R.M.andBode,M.F.,Darnley,M.J.etal.2009,ApJ,1955-1963,703 Seaquist,E.,Bode,M.,Frail,D.,etal.1989,ApJ,344,805 Shara,M.M.,Zurek,D.,Marco,O.D.,etal.2012c,AJ,143 Steffen,W.,LopezJ.A.,2006,RMxAA,99-105,42 Takei,D.,Drake,J.J.,YamaguchiH.,etal.2015,ApJ,92,801 Warner,B.1995,CambridgeUniversityPress,”CataclysmicvariableStars” Wright,E.L.,Eisenhardt,P.R.M.,Mainzer,A.K.etal.2010a,AJ,1868-1881,140

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