The Star Formation History of the Universe · 2010. 5. 7. · Chary: NOAO/NSO 50th Anniversary 1/40...
Transcript of The Star Formation History of the Universe · 2010. 5. 7. · Chary: NOAO/NSO 50th Anniversary 1/40...
Chary: NOAO/NSO 50th Anniversary 1/40
The Star Formation History of the Universe
Star-formation History:<1960 : 7 (*) papers1960-2010 : 3300 papers
General Relativity: <1960: 4001960-2010: 19000
Ranga
Ram CharySpitzer/Planck/IPAC
California Institute of Technology
x400
x40
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How do galaxies evolve from the 1 kpc
irregularblobs to the structure we see today ?
Candidate z~10 galaxies (Bouwens
et al. 2010)
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Extragalactic Background Light ConstraintsUV estimates of SFRIR estimates of SFRSpitzer Measured Stellar Mass DensitiesGamma-ray Bursts
•We’d like to know what the ongoing star-formation rate in galaxies is;
dust unobscured and obscured•We’d like to measure the integral of the past history of star-
formation;cross consistency depends on the stellar IMF
•We’d like to know how metallicity
evolves in galaxiescross consistency with stellar mass estimates
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Extragalactic Background Light =Total Line of Sight Brightness –
Stars –
Zodiacal Light –
Interstellar Medium
Integrated Galaxy Light =Sum over light from all individually detected galaxies
IGL =< EBL
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CGRB
Blazars
300μm 3μm 300nm 0.4keV 40keV 4MeV 400MeV
Hasinger
‘00
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2.2 micron contributions
74%
14%
12% 0%
Zodiacal LightStarsCIRBISM
140 micron contributions
37%
27% 36%
Zodiacal LightCIRBISM
Unfortunately Sky Background at Infrared Wavelengths is Dominated By Zodiacal Light
CIRB (nW
m-2
sr-1)λ νIν
2.2: 22.4±6.03.5: 11.0±3.3140: 25±7240: 14±3
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2.6’
5.8μm25 hrs
24μm10.9 hrs
3.6μm25 hrs
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EBL Constraints
RC&Pope2010
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Results from the EBL
•
EBL is hard to measure and is known to poor precision
•
Equal components of optical+NIR
and FIR EBL → Dust reprocessing is important
•
IGL is lower than EBL at 1.2, 2.2, 3.6 and 60 microns → Diffuse source of radiation like cometary
dust or reionization
epoch galaxies ?
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Lyman break technique to identify star-forming galaxies
Vanzella
et al. 2007
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Hard to do spectroscopy of dusty sources
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But there is dust in different phases
Jason Marshall andIRS GTO Team
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Caputi
et al. 2007,Perez-Gonzalez et al. 2004Le Floch
et al., CE01, Franceschini
et al. 02Magnelli
et al. 2009
But phot-z
errors at z>1.4 are notoriousbecause σ(Δz/1+z)~0.03⇒σ(LIR)~3
Strong Evolution of LIRG and ULIRG population between z~0 and 1
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RC&Pope2010
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Cosmic Evolution of Extinction
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If UV slope were correct, EBL limits would be violated
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Option 1: Dust extinction in many z~4 galaxies is more consistent with SMC extinction law
H. Shim et al 2010
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Stars only
Nebular only
Stars+Nebular
Black line is for 1 Myr
old populationRed line is for 10 Myr
old populationCourtesy of Starburst99Leitherer
et al. 1999
Option 2: Nebular emission makes UV slopes redder
Top heavy IMF increases nebular emission
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Can we reliably understand the nature of galaxies dominating the SF ?
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?
Needs more data for confirmationDefinitely resolved by Herschel.LIRGs
are lower mass, ULIRGs
are higher mass
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Even for objects with spec-z, some violate upper limits or FIR photometry
Evidence for AGN ?
E. Murphy et al. 2009
Intriguingly, this happens at LIR>3E12 Lwhich is the most extreme source in the local Universe
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JD2: A z~2 LIRG. NOT a 6E11 M z~6.5 galaxy.
Are We Missing the z~2-3 LIRGs
?
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Sensitivity of Different Wavelengths to Dust Obscured Star- Formation
Mid-Infrared wavelengths are the most sensitive and least affected by confusion.However, requires large bolometric corrections.
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There are some nightmare sources!
SBS 0335−0521/40 ZHouck et al. 2004
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Wilkins et al. 2008Hopkins & Beacom
2006
An Evolving IMF at z<3 ?
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Reddy & Steidel
2009
Not so fast…..
Systematics
from: 1. Proper treatment of stellar
Remnants2. Integrating down the LF3. Dust corrections at z>2
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Results on SF History
•
Dust reprocessing well understood at z<1•
Some constraints on z>1 from 24 microns
•
Dusty SFR >> Unobscured
SF @ z<2•
At z>2 UV slope is x2 overestimate of obscuration–
Probably because dust is grey
•
No significant discrepancy with stellar mass density → no evolving IMF at z<3
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Everything Consistent ? GRB 090423 at z=8.2607.008.0
+−
•
Gamma-ray burst on 23 April 2009; highest spectroscopically
confirmed astrophysical object known; 600 Myr
after the Big Bang.
•First clue it was at high redshift
was the absence of an optical afterglow. Subsequently detected in the NIR (UKIRT/Gemini), ~0.5-1 hr after the burst.
•
Luminous (but not unusual) explosion, probably associated with the death of a massive star. 1053
ergs released within ~10s (observers frame).
•GRBs
are vital probes of metals, gas, star-formation and reionization
at early epochs since galaxies are too faint for spectroscopy (See e.g. Chary et al. 2007).
Tanvir et al. 2009, NatureSalvaterra et al. 2009
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Chary, Berger & Cowie 2007
WFC3 UDF(Bouwens)
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Could be due to GRB efficiency increasing as metallicity
decreases ?
Butler, Bloom et al. 2010
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Metallicity
increases as (stellar mass density)^0.69+/-0.17Exactly the same as dust content
Gamma-Ray Bursts Also Trace Metallicity
Evolution
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Results from GRBs
•
Star-formation rate density is higher than from field galaxy surveys
•
Not due to dust obscuration
•
Can be explained by GRB production efficiency increases with decreasing metallicity
•
GRBs
are our ONLY tracer of metallicity
evolution especially at the faint end of the galaxy LF.
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Physical Triggering Mechanism ?
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Understanding Modes of Star-formation: Cold Flows or Minor/Major Mergers ?
Dekel
et al. 2009>10:1 mergers
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Are these starbursts or quiescent star-formation ?
Tightness of the SFR-Stellar Mass at 0.8<z<1.2seems to indicate it is quiescent star-formation
Morphological evidence is not clear –
some of theLIRGs
are spirals while some are irregular/S0s
Is this due to increasing dust content in massive galaxies ?
A starburst spans a relatively short time scale ~10% of the cosmic time within that redshiftrange. Expect a large scatter –
there is a good number of “evolved” red galaxies at z~1.
Unclear what fraction of the dust is heated by therelatively evolved stellar population rather thanyoung stars. Is this evidence that a significantfraction of MIR emission is dust heated by A stars? (Salim
et al., Bendo
et al.)Elbaz
et al. 2007Noeske
et al, Papovich
et al., Reddy et al., Daddi
et al.
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Some evidence for continuous accretion at z~4
H. Shim et al.
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But, some of those are morphological trainwrecks
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Summary
•
We have an excellent understanding of what dominates SF over half of cosmic time (z<1)
•
At z>1, uncertainties increase due to observational selection effects. But SFRD appears to be declining. Dusty galaxies still might dominate SFRD –
Herschel will be
insightful.•
At z<1, evolution appears to be due to mergers. At z>1, still up for discussion –
accretion from IGM might
contribute a fraction but 0.0 observational evidence.•
Massive galaxies appear to turn off their star-formation first (due to gas depletion or AGN feedback ?)
•
Metals and dust increase with increasing stellar mass density but at a slower rate, probably due to outflows in low mass halos.
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The Future
•
We have made immense progress in identifying star-forming galaxies to the earliest cosmic times
•
Measure EBL with precision; need to go beyond the inner solar system.
•
Measure FIR SEDs
of galaxies at z~2-4 using Herschel
•
Better spec-z in 1.4<z<2.5 range•
Get spectra of GRBs
efficiently –
best tracer of
z>6 star-formation and the first massive stars•
Get spectroscopic evidence for a cold flow before jumping on the bandwagon