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Resolving the fine structure of the Galactic interstellar medium with
ATCA HI 21cm measurements L. Viktor Tóth (Eötvös University, & Konkoly Obs. Budapest)
Collaborators:L.G.Balázs,Zs.Bagoly,M.Cunningham,H.Dénes,Y.Doi,J.Hakkila,I.Horvath,T.Kovács,P.Jones,
T.Onishi,S.Pintér,I.Rácz,S.Zahorecz
The1.7GpcGRBRingatz=0.8(Balázs+2015MNRAS)
Motivation and consequences
• Motivation:foregroundofextragalacticsources• Specialmotivation:GRB• Variousallskysurveysandtheiruse• HIwithATCA• Dénes,Jones,Tóth,Zahoreczetal.2018tobesubmitted
Speaking of Science
The new biggest thing in the universe, and why it’s a headache for scientists By Robert Gebelhoff August 20, 2015
The1.7GpcGRBRingatz=0.8(Balázs+2015MNRAS)
• redshiftrange:0.78<z<0.86• 21GRBs(overdensityinzdistribution)• ringof9:meanangulardiameterof36deg• correspondingto1720Mpcinthecomovingframe• coordinatedstarformingactivityamongtheresponsibleGRBhosts?
The 1.7 Gpc GRB Ring at z=0.8 (Balázs+ 2015 MNRAS)
AGWeventannouncedonMonday16thOct.2017Multi-messengerObservationsofaBinaryNeutronStarMerger
(LIGOS.C.,VirgoC.,FermiGBM+2017ApJ)GravitationalWavesandGamma-RaysfromaBinaryNeutron
StarMerger:GW170817andGRB170817A(LIGOS.C.,VirgoC.,FermiGBM+2017ApJ)
AnOrdinaryShortGamma-RayBurstwithExtraordinaryImplications:Fermi-GBMDetectionofGRB170817A
(Goldstein,A.;Veres,P.+2017ApJ)…
andalotofotherpapers
GRBs in the headlines again What happened on 17 Aug. 2017?
What happened on 17 Aug. 2017? • Agravitationalwaveevent(laterdesignatedGW170817)wasobservedat12:41:04UTCthroughbytheAdvancedLIGOandAdvancedVirgodetectors.
• TheFermiGamma-rayBurstMonitorindependentlydetectedagamma-rayburst(GRB170817A)withatimedelayof~1.7swithrespecttoGW170817.Fromthegravitational-wavesignal,thesourcewasinitiallylocalizedtoaskyregionof31deg2ataluminositydistanceof40±8Mpcandwithcomponentmassesconsistentwithneutronstars.
• Thecomponentmasseswerelatermeasuredtobeintherange0.86to2.26M¤.• Anobservingcampaignwaslaunchedacrosstheelectromagneticspectrumleadingtothediscoveryofabrightopticaltransient(SSS17a,nowwiththeIAUidentificationofAT2017gfo)inNGC4993(at~40Mpc)lessthan11hoursafterthemergerbytheOne-Meter,TwoHemisphere(1M2H)teamusingthe1mSwopeTelescope.
• Theopticaltransientwasindependentlydetectedbymultipleteamswithinanhour.Subsequentobservationstargetedtheobjectanditsenvironment.
• Earlyultravioletobservationsrevealedabluetransientthatfadedwithin48hours.• Opticalandinfraredobservationsshowedaredwardevolutionover∼10days.• Followingearlynon-detections,X-rayandradioemissionwerediscoveredatthetransient’sposition~9and~16days,respectively,afterthemerger.BoththeX-rayandradioemissionlikelyarisefromaphysicalprocessthatisdistinctfromtheonethatgeneratestheUV/optical/near-infraredemission.
• Noultra-high-energygamma-raysandnoneutrinocandidatesconsistentwiththesourcewerefoundinfollow-upsearches.
àGW170817wasproducedbythemergeroftwoneutronstarsinNGC4993followedbyashortgamma-rayburst(GRB170817A)andakilonova/macronovapoweredbytheradioactivedecayofr-processnucleisynthesizedintheejecta.
GRB 170817A and
GW170817
• Gamma-rayburstsasdetectedbytheFermi(2bands)andINTEGRAL(1band)satellites
• GravitationalwaveeventdetectedbyLIGO-HanfordandLIGO-Livingstondetectors
• Resultedbyabinaryneutronstarmerger
Abbot+2017ApJ
Localization of the gravitational-wave (from the LIGO-Virgo 3-detector global network), gamma-ray (by the Fermi and INTEGRAL satellites) and optical (the Swope discovery image) signals
http://public.virgo-gw.eu/ligo-and-virgo-make-first-detection-of-gravitational-waves-produced-by-colliding-neutron-stars/
AlenticulargalaxyLocationoftheGWsourcemarkedHSTimagehttps://apod.nasa.gov/apod/ap171023.htmlImageCredit:NASA&ESA
NGC 4993 the host galaxy
GW170817 afterglow
Multibandobservationshttps://kilonova.space/kne/GW170817/
Gamma-ray bursts (GRB) – as they appear
• briefeventsoccurringatanaveragerateofafewperday• Typicallyforabriefperiodofsecondstominutes• Onanotherwisealmostdarkgamma-raysky• Whiletheyareon,theyoutshineeveryothersourceofgamma-raysinthesky,includingtheSun.
• TheyarethemostconcentratedandbrightestelectromagneticexplosionsintheUniverse.
• GRBswerefirstdiscoveredin1967bytheVelasatellites,althoughtheywerenotpubliclyannounceduntil1973[224].Thesespacecraft,carryingomnidirectionalgamma-raydetectors,wereflownbytheU.S.DepartmentofDefensetomonitorfornuclearexplosionswhichmightviolatetheNuclearTestBanTreaty.
GRB170817AintheFermiduration-hardnessplane
(Goldstein,Veres+2017ApJ)
T90=2.048sHR32=0.56
Short,hardtype
Long,softtype
• classifiedaccordingtothelengthoftheirγ–rayemission:T90
• Mainclassesare: long&short
• Gammaspectralhardnessisdefined(spectralindex)
• Shortburstare„hard”• Longburstsare„soft”Itisanoutdatedclassification
Classification of GRBs
duration-hardnessplane
Long or “classical” GRBs (Mészáros 2006)
• associatedwithexplosionsofmassivestars(Stanek+2003)• expectedtotraceongoingstar-formationuptoz=9.4• Promptγ-rayemission(0.1-2MeV)–internalshock
• Thermalemissionfromthephotosphere• Non-thermalemission,producedinthejet• byreverseshockpropagatingbackintotheejecta• Note:Lesslikelyfrommagneticreconnectionordissipationprocesses,iftheejectaishighlymagnetized
• Afterglow–externalshock• fireballadvancingintoanapproximatelysmoothexternalenvironment(windblownstellarorISM)
• GRBjetimpactsthesurroundingmediumàafterglow(e.g.Mészáros+Rees1992;Sari+1998)
Long GRB fireball model (Mészáros 2006)
LGRBs – information on distant stars, and IGM
• Explosionofanindividualstarvisiblefromz>7• Observedradiationcarriesinformationabout
• GRBprogenitor• ISMaroundGRBinitshostgalaxy• mediaalongpath
Firststars firstquasars nowAgeoftheUniverse 500Myr 3Gyr 6Gyr 13.7Gyr
Intrinsic ISM parameters (density, metallicity, …) at the GRB jet (< 200 pc)?
• WhataretheparameterstherearoundtheGRB?• Afterglow:continuumradiationinallwavelengths• AfterglowX-rayspectrum–brightand“simple”
• Approximatedaspower-lawcontinuummodulatedbyabsorption(Behar+2011;Schady+2011;Zafar+2011;Campana+2012…)
• Ironemissionline
• Absorption:intrinsic,CGM,IGM,MW (eg.Schady2015JHEA)
• RestframeopticalandUVabs.lines(eg.Fynbo+2009gas;Elíasdóttir+2009dust;Perley+2011,
Schady+2011)• Metallicityandextictionpeculiarities
GRB 070802 Lα spectral line (Elíasdóttir+ 2009)
Estimating the Galactic foreground – input data
SwiftGRBsatlowBwithknownzoverlaidonN(H)map(LAB)
• Spectroscopy• HIsurveys
• LAB36’(LeidenArgentineBonnSurvey,Bajaja+1985;Kalberla+2005)
• EBHIS10.8’(Effelsberg-BonnHISurveyofMilkyWaygasWinkel+2015)
• HI4PI16.2’(EBHIS+GASS,HI4PIcollaboration2016)
• IRASproducts5’-6’• SFD(IRASrecalibrated,Schlegel+1998)• SFDrecalibrated(SDSS,Schlafly+2011)
New:• pan-STARRS1E(B-V)7’-14’(d<4.5kpcstellar
photometry,Schlafly+2014,Green+2015)• AKARIFIS2’(Doi+2015)• PlanckPR2AV5’Planck,IRAS,WISE
intermediateresultsXXIX(PlanckCollab.2016)
Estimating the intrinsic N(H) – LAB foreground
SwiftGRBsatlowBwithknownredshiftoverlaidonN(H)map(LAB)
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−50 0 50
1e−1
01e−0
21e
+06
1e+1
41e
+22
b [°]
NH
host
(LAB
) [cm
−2]
• IntrinsicN(H)fromXspecX-rayafterglowspectralfit• GalacticforegroundestimationisbasedonLAB(36’)• ànoISMatGRBforasubsample?
àNO!
ToolowintrinsicN(H)forvariousdirections
IRASbasedN(H)Schlegeletal.1998
HI21cmlineintensityWinkeletal.2016
HI21cmlineintensityDickey&Lockmann1990
PlanckbasedN(H)Tóth+2017
AKARIbasedsmoothedN(H)Tóth+2017
AKARIbasedN(H)Tóth+2017
GRB131227A,z=5.3;foregroundN(H)20%lower
About 400 SWIFT detected GRB sources with known spectroscopic redshifts. Selected 84:
-availablegoodqualityAKARIFISimages-bestX-rayafterglowlightcurves-bestX-rayafterglowspectra
Lowandintermediategalacticlatitudesareover-represented
B
L
z
Estimating the Galactic foreground – data processing
PlanckAVPR2- basedonWISE12μm;IRAS60μm
&100μm;Planck857GHz;545GHz;353GHzPR2
- Dustmodel(Drain+Li2007)renormalizedtoSDSSQSO
AKARIFISbasedN(H)- AKARIFarInfraredSurveyor(FIS,
Kawada+2007)- Allskyimages65,90,140,
160μm(Doi+2015)- Zodisubtraction(Ootsubo+2016)- T_dustàradianceàN(H)- Smoothedto5’&correlatedwith
PlanckAV- 30’x30’fieldsselected(GRBs)- RenormalizedtoPlanck
CorrelationofPlanck&AKARIbasedN(H)
Planckmaps:http://pla.esac.esa.int/pla/#maps
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0.0 0.2 0.4 0.6
0.0
0.2
0.4
0.6
NHgal Akari (5’ res) [1e22 cm−2]
NH
gal
from
Pla
nck
[1e2
2 cm
−2]
GRB 051022A – an LGRB in the Giant GRB Ring
• WellknowndarkLGRB,(noopticalafterglowßAV,Int)• Hostgalaxy
SFR=271M⊙yr-1(from[OII]lineflux);stellarmass:logM*=10.42±0.05M⊙(Levesque+2014);detectedinCO4-3(ALMA,Hatsukade+2014)
• HIforegroundEBHIS:N(H)Gal=3.9E+20cm-2
Planck smoothedAKARIFIS AKARIFIS AKARI:N(H)Gal=3.3E+20cm-2(Tóth+2017)
X-ray spectrum of GRB 051022A re-fitted
• Swift-XRTGRBCatalogue(Evans+2009)
• analyzedwithXspec(Arnaud1996)
• samemodelasintheautomaticanalysisoftheUKSSDC(Evans+2009)
• withrefinedAKARIbasedforegroundN(H)Gal
• N(H)Intathostgalaxy:5%higher 10.5 2 5
10−3
0.01
0.1
norm
aliz
ed c
ount
s s−
1 keV
−1
Energy (keV)
GRB051022
N(H) from LABN(H) from AkariN(H) from EBHISN(H) from Planck
Seealso:http://www.swift.ac.uk/xrt_spectra/docs.phphttp://www.swift.ac.uk/xrt_spectra/algorithm.php Rácz+2017
ATCA HI 21cm observations
• Observations• 2015-2016-2017,alsousing“greentime”
• 4targets• LGRBswithspectroz;precisepositions• strongX-rayafterglow;highS/NX-rayspectra• galacticforeground:2x1020cm-2<N(H)LAB<8x1020cm-2
• Severalarrayconfigurations• 2-3arcminutesresolution
• Goodspectralresolution• 0.1km/s
GRB100425 L=14.8; B=-25.3
GRB070508 L=314.9; B=-32.4 –– near Cha
ATCA HI 21cm observations
• ReductionwithMiriad• Calibrated• CombinedwithParkesGASSsurveydata
• lowresolution16’• binnedchannels1km/s
• Correctedforbeam• ConvertedtoTB[K]• Continuumsources• Absorptionsearched
Dénes,Jones,Tóth,Zahorecz+inprep.
Galactic foreground - ATCA HI 21cm with optical depth correction using continuum point sources
• Spatialresolution:2.75’x2.12’• velocityresolution:0.103kms-1
• onephaseISM
• i.e.themeasuredTBwascorrectedwiththeopticaldepthfromHIabsorptiontowardsacontinuumsourcenearthetarget
• GRB081008(seeontheright)
Dénes,Jones,Tóth,Zahorecz+inprep.
HI 21cm line, τ, corrected line
• NearChaclouds• HIspectrumcorrectedforopticaldepth
• DerivedHcolumndensityincreasedby50%
Dénes,Jones,Tóth,Zahorecz+inprep.
• a
HI4PI & ATCA HI foreground
X-ray afterglow spectrum of GRB 070508 re-fitted using ATCA HI foreground
• Swift-XRTGRBCatalogue(Evans+2009)
• analyzedwithXspec(Arnaud1996)
• samemodelasintheautomaticanalysisoftheUKSSDC(Evans+2009)
• N(H)Gal• HI4PI:7.1x1020cm-2
• RQ:10.3x1020cm-2
• ATCA:14.6(9.0)x1020cm-2
• HostgalaxyN(H)Int:few%diff.
SeealsoRácz+2017;Tóth+2018Dénes,Jones,Tóth,Zahorecz+inprep.
Resolution dependence of the Galactic foreground (MW) hydrogen column density
Tóth+2017
AKARIandLAB PlanckPR2andAKARI
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0.0 0.1 0.2 0.3 0.4 0.5 0.6
0.0
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0.4
0.6
NHgal LAB [1e22 cm−2]
NH
gal A
kari
[1e2
2 cm
−2]
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0.0 0.2 0.4 0.6
0.0
0.2
0.4
0.6
NHgal Akari [1e22 cm−2]
NH
gal
from
Pla
nck
[1e2
2 cm
−2]
Effect of foreground (MW) correction on the intrinsic (host galaxy) hydrogen column density
Tóth+2017
Galacticforeground(MW) IntrinsicN(H)(hostgalaxy)
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0.0
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0.6
NHgal LAB [1e22 cm−2]
NH
gal A
kari
[1e2
2 cm
−2]
Summary
• GRBs• Galacticforegroundrevealedby
• PlanckandHIsurveys• N(H)MWoftenslightlylowerthanLABestimates
• ClumpyISM(alsoatlowcolumndensities)
• Resolutionmatters(abit)• higherintrinsicN(H)atsomecases • NeedfurtherhighresolutionN(H)
Planck PR2 RQ AV centered to the double core (Daniel’s talk, Zahorecz+ 2018)
HI4PI N(HI) centered to the double core (Daniel’s talk, Zahorecz+ 2018)
Galactic foreground - Osaka-1.85m CO (2-1)
Onishi+2017priv.comm.
Spatialresolution:2’velocityresolution:0.1kms-1