Spitzer Observations of Submm/Mm/Radio-Selected Galaxies Eiichi Egami (Univ. of Arizona) MIPS team:...
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Transcript of Spitzer Observations of Submm/Mm/Radio-Selected Galaxies Eiichi Egami (Univ. of Arizona) MIPS team:...
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Spitzer Observations of
Submm/Mm/Radio-Selected Galaxies Eiichi Egami (Univ. of Arizona)
MIPS team: E. Le Floc'h, C. Papovich, P. Perez-
Gonzalez, G. Rieke, M. Rieke, H. Dole, A. Alonso-
Herrero, M. Blaylock, J. Cadien, J. Jones
IRAC team: J.-S. Huang, P. Barmby, G. Fazio
Lockman Hole
SHADES team: J. Dunlop, R. Ivison, + others
Bolocam team: J. Glenn + others
(Lijiang)
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Outline
1. Spitzer deep survey of the Lockman Hole East
● Submm/Mm/Radio selection: why should we care?
● 70/160 um observations
2. Spitzer observations of the brightest cluster
galaxies (BCGs) in strongly cooling cluster cores
● IGM accretion onto a seed mass concentration
-> another way to make galaxies IR-luminous (as
opposed to galaxy-galaxy interaction). May
play an important role at high-z (e.g., z > 3-4).
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1. Deep Survey of the Lockman Hole (E)
● Lowest HI column density● Abundance of ancillary data● Especially deep X-ray/radio● Wide submm coverage (SHADES)● Deep optical (R,I,z) coverage
We doubled the MIPS integrationsduring the spring of 2005.
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850 um: 8 mJy
24 um: 80 uJy20 cm: 20 uJy
Radio (20cm) data must be very deep to be useful.
Submm/Radio Selection vs. 24 um Selection
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Why do we care about submm/mm/radio?
● Submm/Mm
– Potential to detect extremely high-z galaxies (z>3).
– Power to constrain IR SED together with Spitzer.
● Radio
– Accuracy for estimating IR luminosity with the tight
radio-IR luminosity correlation (e.g., 24um requires
knowledge of PAH strength).
– Combination of high spatial resolution (compact AGN
vs. extended SB) and large field coverage.
Answer: Provides effective selection for high-z infrared-luminous galaxies (e.g., LBG analogy). Also,
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> 10^11 Lsun
LIRGs ULIRGs
Starbursts
Le Floc'h et al. (2005) Perez-Gonzalez et al. (2005)
LIRGs/ULIRGs become important at z > 1.
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However, submm and radio have very different selection functions. provide complementary views of high-z IR-luminous galaxies
MIPS 24um (80 uJy)
VLA deep ( 50 uJy)
VLA deepest (20 uJy)
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Lockman Hole East 24um (14' x 14')
red – 850um SCUBA, 16 src (Scott et al. 2002)
blue – 1.2mm MAMBO, 23 src (Greve et al. 2004)
green – 20cm VLA, 154 src (Ivison et al. in prep)
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MIPS 24 um MIPS 70 um
Radio selection efficiently picks up FIR luminous sources.
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MIPS 70 um MIPS 160 um
A submm/mm source strongly detected at 70 & 160 um
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Far-IR SED of a mm-selected galaxy at z=1.4
3.3um PAH
Arp 220 still works.
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SCUBA HAlf-Degree Extragalactic
Survey (SHADES)● PI: Jim Dunlop (Edinburgh)
● Lockman Hole (and Subaru-XMM Deep Field)
● 0.25 square degree x 2 fields (takes 3 years)
● 8 mJy (4 sigma) @ 850um using SCUBA
● Deep VLA/MERLIN 20cm map (Ivison et al.)
● Wide-field near-IR images (UKIDDS@UKIRT)
● Deep optical images (IfA Deep Survey@Subaru)
● BLAST @ 250, 350, and 500 um
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SHADES - Lockman Hole● 45% complete (402 square arcmin)● 69 sources (> 3.5 sigma)
8 mJy sample (published)●16 sources (>3.5 sigma)●¼ of 69 SHADES sample
ERO
8 mJy
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Redshift distribution of 32 cold-type VLA sources(LIR > 1011 L⊙ except for z<0.5)
SCUBA sources
Star Formation History – Updates available soon!
Perez-Gonzalez et al. (2005)Need to go deeper and determine LF at high-z. (e.g., EVLA, stacking)
24um sample
Radio/Submm
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2. Spitzer Observations of BCGs in
Strongly Cooling Cluster Cores● Strongly cooling cores prevalent among X-ray-
luminous clusters -> Cooling Flows
– ROSAT/ASCA: as much as 2000-3000 M⊙ yr-1
– Chandra/XMM: cooling taking place but the cooling
rates down by a factor of 10, possibly
due to turn-on of radio AGNs.
● IGM (ICM) accretion to a seed galaxy
– Another way to make galaxies infrared-luminous
– May play a important role at high-z (z>3-4)
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SEDs of 11 brightest cluster galaxies (BCGs) at z=0.2-0.3
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The IR sources are compact: D < 8 kpc
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IR-luminous BCGs are located in clusters with the shortest cooling times
Small scatter with the trend -> IGM (ICM) accretion (not galaxy-galaxyinteraction) is likely responsible for the increased IR luminosities.
Non-BCGrange
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Three-component SED model
1. Giant elliptical (gE)2. ULIRG (Arp 220)3. Radio AGN (power-law)
A1835: 8 • 1011 L⊙
Z3146: 4 • 1011 L⊙
LIRGs !
A2390: 3 • 1010 L⊙
Most BCGs harbor a radio AGN (70%)
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IRS spectrum of Z3146: Strong PAH - IR luminosity of starburst originStrong H
2 - a few times more luminous than N6240!
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The two LIRG BCGs are overluminous in CO (1-0) for their IR luminosities.
Similar to the radio galaxiespresented by A. Evans.
Result of IGM (ICM) accretion onto the BCGs?
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Summary
● Submm/mm/radio-selected galaxies
– Provide effective selection for high-z infrared-luminous
galaxies
– Allow accurate determination of SEDs & LIR
together with
Spitzer.
● Infrared-luminous brightest cluster galaxies (BCGs)
– Increased LIR
likely due to star formation triggered by IGM
(ICM) accretion.
– Similar process may play an important role at high-z
(z>3-4).