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FIRST LIGHT IN THE UNIVERSE

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Presentation on theme: "FIRST LIGHT IN THE UNIVERSE"— Presentation transcript:

1 FIRST LIGHT IN THE UNIVERSE
Saas-Fee, April 2006 Richard Ellis, Caltech Role of Observations in Cosmology & Galaxy Formation Galaxies & the Hubble Sequence Cosmic Star Formation Histories Stellar Mass Assembly Witnessing the End of Cosmic Reionization Into the Dark Ages: Lyman Dropouts Gravitational Lensing & Lyman Alpha Emitters Cosmic Infrared Background Future Observational Prospects

2 z > 6 Surveys Represent the Current Frontier
Motivation: census of earliest galaxies (z=6, =0.95 Gyr) contribution of SF to cosmic reionization constraints on early mass assembly planning effective use of future facilities (ELTs, JWST) Developing complementary optical/IR techniques: - continuum dropouts: reducing contamination - HST ACS grism, SEDs with low background - Ly LF: sensitivity to physical state of IGM - strong lensing: extends capabilities at faint end of LF - Spitzer detections: masses & early SF histories

3 Some Key Issues How effective are the various high z selection methods? L*(z=6)  i~26 where spectroscopy is hard spectroscopic samples biased to include strong L - great reliance on photometric redshifts Is there a decline in the UV luminosity density 3<z<6? results are in some disagreement differing trends in continuum drops & L emitters Is the observed UV at z>6 sufficient for reionization? - contribution from (unobserved) faint end of LF? - unusual popns: intense EW(L), steep UV continua? Significant stellar masses for post-burst z~6 galaxies - how reliable are the stellar masses? - inconsistent with declining SF observed 6<z<10? does this imply an early intense period of activity?

4 Continuum sources probed via dropout technique
z-dropout Stanway et al (2003) Traditional dropout technique poorly-suited for z>6 galaxies: - significant contamination (cool stars, z~2 passive galaxies) - spectroscopic verification impractical below ~few L* i-drop volumes: UDF ( ), GOODS-N/S (5.105), Subaru (106) Mpc3 flux limits: UDF z<28.5, GOODS z<25.6, Subaru z<25.4

5 Reducing Contamination from z~2 Passive Galaxies
Addition of a precise optical-infrared color (z - J) can, in addition to the (i - z) dropout cut, assist in rejecting z~2 passive galaxy contaminants. (Stanway et al 2004) (i – z) 5.7 < z < 6.5 z~2 passive galaxies This contamination is ~10% at z~25.6 but is negligible at UDF limit (z~28.5) (z – J)

6 Contamination by cool Galactic dwarfs - more worrisome
UDF z<25.6 (Stanway et al 2004) L dwarfs E/S0 HST half-light radius Rh more effective than broad-band colors Contamination at bright end (z<25.6) is significant (30-40%)

7 Keck spectroscopy of i-drops: 10.5 hrs zAB < 25.6
z=5.83 L L-dwarfs contaminate at bright end

8 Counts for i-band drops (GOODS+UDF)
 6 from z~3 Spec limit GOODS/UDF data to zAB=28.5 consistent with z=3 LBG LF but  6 Bunker, Stanway, Ellis & McMahon MNRAS 355, 374 (2004)

9 ACS dropouts: Luminosity Dependent Evolution?
z=3 Bouwens et al (2006, astro-ph/ ) propose L-dependent evolution - decline in abundance over 3<z<6 mostly for luminous sources If correct, this affects z-dependent integrated SF density measures corrected to some fiducial luminosity

10 How much steeper could LF slope be at early times?
i-drop counts N(28.5) = 54 N(30.0) = 108 Yan & Windhorst (2004) extend UDF i-drop search to z(AB)=30.0 (c.f. Bunker et al z(AB)=28.5) and claim  -1.9 after correcting for incompleteness implying a significant increase in integrated density at z~6

11 Decline in UV over 3<z<6 has been controversial
Giavalisco et al 2004 Bunker et al 2004 Poisson errors fail to account for dispersion in claimed number of z~ i-drops, because of varying ways of accounting for contamination plus cosmic variance (10% in GOODS; 40% in UDF) Bouwens et al 2005 Ap J 624, L5

12 Results from Subaru HST offers superior photometry & resolution (important for stellar contamination) but SuPrimeCam has much bigger field (each pointing = 2  GOODS-N+S) Additional photometric bands developed to sort stellar contamination Shioya et al (2005): used intermediate band 709nm, 826nm to estimate stellar contamination in z~5 and z~6 samples respectively Shimasaku et al (2005) split z-band into two intermediate filters zB, zR - to measure UV continuum slope These studies confirm decline indicated via HST studies

13 z~6 dropouts from Subaru - the upshot
SDF dataset > 2  GOODS N+S; cosmic variance ~ 25% Confirm 5 abundance drop from z~3 to 6 (c.f. Bunker et al, HST) Luminosity dependent trends - more evolution in massive galaxies? Remember: this is observed number not dust-corrected SFR

14 Further confirmation of i-drop technique
star z~2 passive Malhotra et al (2005) use 40 orbit ACS UDF grism exposures & consider utility of (i - z) color cut vs. contamination Traditionally use (i - z) > 1.3 (e.g. UDF) Of 29 z<27.5 candidates with (i - z) > 0.9, 23 are at z~6

15 Determining Abundance Necessary for Reionization
e.g. Madau, Haardt & Rees (1999): Input details depend on considerable imponderables: TIGM  10,000 – 20,000 K ? Teff & Z of stellar population (IMF) ? C = <HI2 > / <HI>2 simulations suggest C  30 ? fesc (=1 implies no HI absorption) ? Leading to factors of 10 uncertainty!

16 Cosmic Star Formation History
The combined uncertainties in the data (plus uncertain input physics necessary for the predictions) mean we cannot yet convincingly claim (or reject) that the abundance of z>5 sources is sufficient for reionization Bouwens et al astro-ph/ )

17 The Spitzer Space Telescope Revolution
A modest 60cm cooled telescope can see the most distant known objects and provide crucial data on their assembled stellar masses! IRAC camera has 4 channels at 3.6, 4.5, 5.8 and 8 m corresponding to 0.5-1m at z~7! Egami et al (2005) - characterization of a lensed z~6.8 galaxy Eyles et al (2005) - old stars at z~6 Yan et al (2005) - masses at z~5 and z~6 Mobasher et al (2005) - a galaxy > 1011 M at z~6?

18 Spitzer detections of i-drops at z=6
Eyles et al (2005) MNRAS 364, 443 4 i-drops in GOODS-S confirmed spectroscopically at Keck Ly  emission consistent with SFR > 6 M yr-1 IRAC detections from GOODS Super-Deep Legacy Program

19 Spectral Energy Distributions of i-drops
#1 z=5.83 #3 z=5.78 VLT K VLT K Spitzer + Ly emission constrains present & past star formation Ages > 100 Myr, probable Myr (7.5<zF<13.5) Stellar masses: 2-4 1010 M (>20% L*)

20 Independent z~5-6 UDF Spitzer analysis
Yan et al Ap J 634, 109 (2005)

21 Evidence for Unusually Strong UV Continua
Several UDF objects at z~6 show unusually blue (z-J) colors which lie outside the predictions of standard Bruzual Charlot models; a point first noted by Stanway et al (2004) - unclear what this means! Yan et al Ap J 634, 109 (2005)

22 Spitzer detection of resolved J-drop in UDF
Criterion: (J – H)AB > 1.3 plus no detection in combined ACS JD2: strong K/3.6m break  potential high mass z~7 source Mobasher et al (2005) Ap J 635, 832

23 High mass resolved J-drop in UDF + two breaks Mobasher et al (2005)
STARBURST99: z=6.6; EB-V =0.0; Z=0.02, zF>9 BC03: z=6.5; EB-V =0.0; Z=0.004, zF>9 Stellar Mass: 2-7  1011 M dependent on AGN contamination

24 Uncertainty in Redshift and Stellar Mass
~ 25% chance of being z~2.5

25 `Double-Break’ Objects Seem Fairly Common

26 Abundance of Massive Galaxies at z~6: A Crisis?
Abundance of massive galaxies at z~6 with CDM in terms of their implied halo masses, assuming Scalo IMF SF efficiency 20% Find a 1013 M halo in the tiny UDF is a problem! z = 5.8 Mobasher et al z = 15 Yan et al Eyles et al Barkana & Loeb (2005)

27 Measured z~5-6 Mass Density
all SFH only accounts for mass assembled in SF galaxies at z~5, so still a lower limit Luminous SF galaxies Stark, Bunker, Eyles, Ellis & Lacy (2006)

28 Summary of Lecture #6 Great progress using v,i,z,J-band drop outs to probe abundance of SF galaxies from 3<z<10: Bouwens et al discuss the properties of 506 I-band dropouts to z~29.5! In practice, these samples are contaminated by foreground stars, z~2 galaxies etc to an extent which remains controversial. We are unlikely to resolve this definitively with spectroscopy until era of ELTs. Comoving SF rate declines from z~3 to z~6 (and probably beyond) suggesting insufficient 6<z<10 luminous galaxies to reionize Universe Contribution of lower luminosity systems less clear (lensing: Lecture 7) Spitzer’s IRAC can detect large numbers of z~5-6 galaxies and it seems many have high masses (one spectacularly so!) and signatures of mature stellar populations - implies earlier activity Reconciling mature galaxies at z~6 with little evidence for SF systems with 7<z<10 may turn out to be a very interesting result

29

30 Combining intermediate & broad-bands (Shioya et al)
Stars Starburst candidates Passive SDF example (for z~5 R-drops) shows how high z galaxies can be separated from interlopers by demanding strong intermediate band depressions (709-i), in addition to a regular (R-i) color cut Method reduces number of `traditional’ R-drops from 3519 Similar technique using 826nm filter reduces i-drops from 96

31 Intermediate + broad-bands contd.. (Shimasaku et al)
stars z~6 gals z~2 passive Breaking z-band into two components (zR, zB) can insist on blue continuum slope within z-band for z~6 galaxies. Reduces conventional i-band drops z < 25.4 from 22  12

32 Low Abundance of z~6 Sources
No extinction Necessary for reionization 6<z<9 (Stiavelli et al 2003) GOODS+UDF Bunker et al (2004) Can rescue situation appealing to: cosmic variance (unlikely given independent datasets) steep faint end LF (Yan & Windhorst 2004) low Z populations (Stiavelli et al 2004)

33 Ages and Stellar Masses
#1 z=5.83 #3 z=5.78 Explored range of BC models including dust: Ages > 100 Myr, probable range Myr (7.5<zF<13.5) Stellar masses: 2-4 1010 M (>20% L*)


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