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Which dust attenuation curve(s)forstarforming galaxies?
VéroniqueBuat1DavidCorre1,MédéricBoquien2,Kasia Malek3,1
&theHELP/Herschelteam1LAM,Aix-MarseilleUniversité,France
2 CITEVA,Universidad ofAntofagasta,Chile3NCNR,Warzawa,Poland
DustingtheUniverse,Tucson,2019
Dusting theUniverse,Tucson,2019
Theshape oftheattenuation law is found tovary atlow andhighz,fromdataandsimulations….only fewexamples
From numerical simulationsNarayanan+18Cousin+19Z=0,SDSS,Salim+18
ULIRGs atz=2LoFaro+171.5
Thederived quantities SFR&Mstar aremodified
DustingtheUniverse,Tucson,2019
Theios +19SMC(UVsteep)andCalzetti (UVflat)curves
(nodust emission)
Maleketal.2018,HELPprojectCharlot&Fall recipe (NIRflat)andCalzetti (NIRsteep)attenuation lawsLoFaroetal.2017Very flatattenuation curves forULIRGs atz=2
9.0 9.5 10.0 10.5 11.0 11.5 12.0log(Mstar) [M�]
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
Nor
mal
ized
coun
ts
CF00
Calzetti2000
LoFaro2017
Charlot&Fall 00recipe
Outline of the talk
• Formalisms fortheattenuation laws &flexiblerecipes• Thestudy ofaHerschel+3D-HSTsample intheCOSMOSfield• Extinction/attenuation:galaxieshosting Gamma-raysbursts (GRBHs)
**Comparison with RadiationTransfermodeling**
DustingtheUniverse,Tucson,2019
𝐴"#$ = 𝐴$ 𝜆 0.55+
,-.
𝐴"/01 = 𝐴&/01 𝜆 0.55+
,234
Charlot&Fall 2000(CF00)à freeISMslope
Calzetti+2000(C00)à freeslope
Themost usual formalisms fortheattenuation laws &flexiblerecipes
(daCunha+08,,Wild+11,Chevallard+13,LoFaro+17,Malek+18)
(Buat+11,12,Kriek&Conroy 13,Salmon+15,Zeimann+15,Seon &Draine2016,Corre+18,Wang+18)
nosingleattenuation lawage dependent attenuation forstars
t~107 yrs (BC),
CF00:nBC=nISM=-0.7,µ=0.3
Asingleattenuation law forallthestellar continuumMWextinction+screen fornebular lines
C00:δ =0,EBV-factor=0.44
EBV-factor=E(B-V)star/E(B-V)lines
DustingtheUniverse,Tucson,2019
𝑘 𝜆 = 𝐴(𝜆)
𝐸(𝐵 − 𝑉) ×
𝜆𝜆&
>
𝜇 = 𝐴&/01 𝐴&/01 + 𝐴$+
• OriginalCF00recipe fortheISM:𝜆-0.7 ,Rv ~5.8
• Calzetti lawRV=4.05
0:2 0:3 0:4 0:5 1 2
wavelength[¹m]
0:05
0:1
0:2
0:5
1
2
5A
(¸)=
A(V
)
C00¡ ± = 0Calz¡mod¡ ± = ¡0:6Calz¡mod¡ ± = 0:2CF00¡ slope = ¡0:7CF¡ ISMfree¡ slope = ¡1:1CF¡ ISMfree¡ slope = ¡0:5
TheCalzetti law is steeper than theCharlot&Fall recipe at𝜆> 𝜆V
Dusting theUniverse,Tucson,2019
LoFaro+17,Buat+18
100 101 102 103
� [µm]
0.0
0.2
0.4
0.6
0.8
1.0
tran
smis
sion
GALEX NUV
CFHT MegaCam u
Subaru suprime B
Subaru suprime V
Subaru suprime r
Subaru suprime i
Subaru suprime z
Subaru suprime y
UKIRT WFCam J
CFHT wircam H
VISTA vircam Ks
Spitzer IRAC 3.6
Spitzer IRAC 4.5
Spitzer IRAC 5.8
Spitzer IRAC 8.0
Spitzer MIPS 24
Herchel PACS 100
Herchel PACS 160
Herchel SPIRE 250
Herchel SPIRE 350
Herchel SPIRE 500
21photometric bands+Hαfluxes
DustingtheUniverse,Tucson,2019
THECOSMOS3DHSTandHerschelsample
+Hα+[NII]fluxes
1e¡ 20 1e¡ 19 1e¡ 18FH®(3D¡ HST)[Wm¡2]
1e¡ 20
2e¡ 20
5e¡ 20
1e¡ 19
2e¡ 19
5e¡ 19
1e¡ 18
2e¡ 18
FH®(¯
ts)[
Wm¡
2]
Buat+18,A&A,619,A135
33SEDs,fits with CIGALEPhotometry
+Emissionlines (Cloudy)Boquien+19
NUV submm
0.6
0 0:2 0:4 0:6 0:8 1:0¹
0
0:2
0:4
0:6
0:8
1:0
E(B¡
V) s
tar=
E(B¡
V) l
ine
¡1:0 ¡0:8 ¡0:6nISM
¡0:6¡0:5¡0:4¡0:3¡0:2¡0:1
0
0:1
0:2
±
Parametersoftheflexibleattenuation recipes:• µ andEBV-factor correlate• nISM and 𝛿 correlate ,inaverage steeper valuesthan theoriginalones.
-->Nouniversal values
EBV-factor=0.44
µ=0.3
nISM =-0.7
DustingtheUniverse,Tucson,2019
=0.54± 0.19=0.60± 0.23
=-0.33± 0.18=-0.82± 0.19
𝛿 =0
EBV-factor
Buat+18
0 0:5 1:0 1:5 2:0 2:5 3:0
AV(mag)
¡3
¡2
¡1
0
pow
er¡
law¡
expon
ent[FU
V¡
V]
0 0:5 1:0 1:5 2:0 2:5 3:0
AV(mag)
¡3
¡2
¡1
0
pow
er¡
law¡
expon
ent[H¡
V]
Comparison with Radiationtransfer modeling ofspiralgalaxieswhich predicts aflattening ofattenuation laws with increasing
obscuration/inclination(e.g.Pierini+04,Tuffs+04,Law+18&Chevallard+13compilation)
FUV-VrangeV-Hrange
DustingtheUniverse,Tucson,2019
__Chevallard+13■.DBPL-free•Calzetti-like __Chevallard+13
■.DBPL-free•Calzetti-like
stee
per
CFfreerecipe
CFfreerecipe
Buat+18
D.Corre,PhDthesis.Corre,Buat,etal.Inprep
• 𝜆 < 𝜆V K(𝜆)mod =K(𝜆)C00*(𝜆 /𝜆V)𝛿• 𝜆 >𝜆V K(𝜆)mod =K(𝜆)C00*(𝜆 /𝜆V)𝛿+𝜀
CANDELS@UMASS,october2018
Modifying theflexibleCalzetti-like recipe intheNIR?
RTfrom Seon &Draine2016(various dust models andspatialdistributions)
D.Corre,PhDthesis.Corre,Buat,etal.Inprep
RTfrom Seon &Draine2016(various dust models andspatialdistributions)
• 𝜆 < 𝜆V K(𝜆)mod =K(𝜆)C00*(𝜆 /𝜆V)𝛿• 𝜆 >𝜆V K(𝜆)mod =K(𝜆)C00*(𝜆 /𝜆V)𝛿+𝜀
CANDELS@UMASS,october20180 1 2 3
AV(mag)[H¡ V]
¡3
¡2
¡1
0
pow
er¡
law¡
expon
ent
! =0
Average SD16relation
Modifying theflexibleCalzetti-like recipe intheNIR?
Aselection ofGRBhoststostudy dust extinction/attenuation
DustingtheUniverse,Tucson,2019
Corre,BuatInprep.
GRBhostgalaxieswith:• Atleast5photometric bands,1inFUVrest-frame• Hα,H𝛽 (Kruehler+15)
Dust attenuation andcomparison with Seon andDraine(2016)models
Among them:6GRBHs with anextinctioncurvemeasured along thelineofsight oftheGRBafterglow
à extinction/attenuation comparison
Corre+18,A&A,617,A141
D.Corre,2018,PhDthesis
Extinctioncurves forGRBHsmeasured with observationsoftheafterglow
Zafar+18
Theafterglow is modelled byasingleordoublepower-law:any deviationin theUV-NIRrangeis duetodust extinction
DustingtheUniverse,Tucson,2019Corre+18
DustingtheUniverse,Tucson,2019
MWlike curves observed
Attcurve flatterthan Extcurve
Attcurve similar toExtcurve
Attcurve flatterthan Extcurve Attcurve steeper than Extcurve
DustingtheUniverse,Tucson,2019Corre+18
Attcurve flatterthan Extcurve
Attcurve similar toExtcurve
Attcurve flatterthan Extcurve Attcurve steeper than Extcurve
DustingtheUniverse,Tucson,2019Corre+18
variety of configurations
flexibility of models & recipes
Dusting theUniverse,Tucson,2019
Which dust attenuation curve(s)forstarforming galaxies?
ANSWER:alot……