ithaca - 19 jun 2006 vc the irs gto ulirg program
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Ithaca - 19 Jun 2006VC
The IRS GTO ULIRG ProgramThe IRS GTO ULIRG Program
0
5
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15
20
25
0.04 0.16 0.28 0.4 0.52 0.64 0.76 0.88 1
redshift
Current IRS ULIRG Sample
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26
58
93
60
3924
8 9 4 2 2 1 0 0 4 1 2 2 1 0 0 1 1 00
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40
60
80
100
0.04 0.16 0.28 0.4 0.52 0.64 0.76 0.88 1
redshift
all ULIRGs
0
5
10
15
20
11.9 12.1 12.3 12.5 12.7 12.9 13.1 13.3
log LFIR
Current IRS ULIRG Sample
166
5540 30 22 10 9 4 2 0 4 0 0 1 10
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100
150
200
11.9 12.1 12.3 12.5 12.7 12.9 13.1 13.3
log LFIR
all ULIRGs
Ithaca - 19 Jun 2006VC
The IRS GTO ULIRG program - details The IRS GTO ULIRG program - details
Of the 110 sources Flux limited: 32 have S25 0.3 Jy and log LFIR 11.85 L.
We are observing all 32 in low and high-res modes. High redshift: 27 have z 0.3.
GTO1-: 12/27 are being observed in low and high-res. + GTO2 (all rest) High luminosity: 11 sources have log LFIR 12.5 L .
10/11 are being observed in low and high-res.. Mix of Far-IR colors: 68 are “cold” (S25/S60 < 0.2) and 21 are “warm”.
This is a higher fraction of warm sources than in a flux-limited survey (typically ≤ 10%).
GO Programs: Veilleux et al., Lutz et al., Imanishi et al., Verma et al. Sturtm et al.
Additional IRS spectroscopy of ~30 “Template” galaxies “usual suspects” Weedman et al. 2005, Brandl et al. 2006 (submitted), Devost et al.
2006 (in prep)
Ithaca - 19 Jun 2006VC
Rigopoulou et al. 1999
IRS Spectra of BGS Sources IRS Spectra of BGS Sources
Armus et al. 2006
ISO PHT-S spectra of BGS Sources ISO PHT-S spectra of BGS Sources
Ithaca - 19 Jun 2006VC Armus et al. 2006
Quantifying the contributionQuantifying the contributionof of accretion to a SMBHaccretion to a SMBH - -and and a Stabursta Staburstto the total mid-IR fluxto the total mid-IR flux
AGN Tracer:AGN Tracer:•[NeV] at 14.3μm / 23.2μm (Ep~97eV)
Starburst Tracers:Starburst Tracers:•[NeII] at 12.83μm(Ep~21eV)
•Presence of PAHs6.2μm EQW
Ithaca - 19 Jun 2006VC
AGN
starburst
ULIRG
Armus et al. 2006
Quantifying the contributionQuantifying the contributionof the energy from the AGNof the energy from the AGNto the total IR luminosityto the total IR luminosity
Ithaca - 19 Jun 2006VC
starburst
ULIRG
AGN
[NeV] not detected in deeply obscured ULIRGs: Is the AGN NLR fully obscured?
[NeV] not detected in deeply obscured ULIRGs: Is the AGN NLR fully obscured?
Ithaca - 19 Jun 2006VC
• Rising slope of thermal emission from the AGN torus from 2-5μm due to grains radiating in near-equilibrium
• Excess over starlight at ~4-5μm“Laurent Diagram”
Alonso-Herrero et al. 2003
f(5μm)~10Jyz~0.004D~14Mpc
f(5μm)~7mJyz~0.9
D~5.8Gpc
FSC15307+3252
AGN thermal emission in mid-IR continuum AGN thermal emission in mid-IR continuum
Ithaca - 19 Jun 2006VC
Decomposition of the Infrared Spectrum
Core of the method Assume absorption cross sections from Li & Draine (2001) and an
MRN grain-size distribution Calculate the opacities of PAH, graphitic and smoothed
astronomical silicate grains.
Each dust component has a quasi-fixed temperature i.e.. the fitting process is really an expansion into several temperature basis components.
The number of dust components is fixed for the sample so that all galaxies are fit in a uniform manner.
In addition to a ~3500 K stellar blackbody and PAH component, we find that we need ~3 additional continuum dust components with T~400, ~150, and ~30 K to accurately fit the entire sample.
An AGN manifests its presence with the requirement of an additional hot dust component T~800K (Laurent et al. 2000)
Talk to Jason Marshall !Talk to Jason Marshall !
Ithaca - 19 Jun 2006VC
Decomposition of Arp220
TCold=31KTWarm=96KTHot=873K
LHot/LTotal=0.005L1-40/LTotal=0.19LPAH/LTotal=0.004
Ithaca - 19 Jun 2006VC
Decomposition of Mrk231
TCold=38KTWarm=151KTHot=486K
LHot/LTotal=0.13L1-40/LTotal=0.52LPAH/LTotal=0.006
Ithaca - 19 Jun 2006VC
Conclusions based on the BGS ULIRGs
AGN fraction estimates based on various methods