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High Redshift Galaxies

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Title: High Redshift Galaxies


1
High Redshift Galaxies
  • Scott Chapman (Cambridge, IoA)
  • Aug22, 2007

2
Overview and Motivation
  • 0. Introductory remarks about galaxy
    formation evolution
  • Direct observations of galaxy progenitors
    forming at high redshift (z 1.5)
  • Protoclusters at high redshift (z 1.5)

3
Context Hierarchical Galaxy Formation (How/when
are the galaxy components assembled?)
  • Big Bang Cosmic Microwave Background
  • Galaxy Formation and Evolution Fossil
    Records today!

Submm/Radio is a superb probe of obscured forming
galaxies well defined SEDs unimpeded by dust
obscuration bolometric selection Andromeda
(M31) is ideal laboratory to study L galaxy
components.
4
Galaxy Evolution - Gravity
5
GALAXY FORMATION and EVOLUTION with baryons
Dark matter
Bright galaxies
N-body semi-analytic -gas cooling -star
formation -SNe feedback -galaxy mergers within
halos
  • Success reproducing
  • observed parameters
  • at z0.
  • High-z objects of various classes continue to be
    problematic -- SMGs, DRGs,
  • (e.g., Sommerville et al. 2000 Baugh et al.
    2005)

Low SFR
High SFR
(Kauffmann et al. 1998)
6
Progenitors of Massive Galaxies
  • Until the mid-1990s the only zgt2 objects known
    were QSOs, radio galaxies, and QS0 absorbers
    (DLA/LLS)
  • How can we go about isolating more normal
    galaxies during the epoch of star/galaxy
    formation?
  • The study of high-redshift (lets say zgt1.5)
    galaxies has exploded in the last 10 years, with
    multiple techniques for isolating high redshift
    galaxies, making use of multi-wavelength data
    spanning from the radio to the X-ray
  • As opposed to traditional magnitude-limited
    surveys, down to specific flux limit, new results
    utilize several complementary selection
    techniques for finding high-z galaxies, selecting
    overlapping yet complementary populations --gt
    must determine how they overlap/complement each
    other to describe entire galaxy population at a
    given epoch.

7
Foreground (zlt2) Galaxies
NB IAB25 ?? 1 photon/year/cm2/A
From LeFevre, Vettolani et al 2003
? Brute force spectroscopy is inefficient for
zgt2!
8
The Laboratory for studying high-z galaxies
UKIRT CSO JCMT Subaru
Keck-I/II IRTF CFHT Gemini
Spitzer
9
Ground-based vs. space-based?
  • NB in addition to transmissivity, the emissivity
    of the Earths atmosphere is a big problem sky
    at 2mm is 10,000 brighter than at 0.5mm

Some sub-mm windows from good sites
10
(Spitzer Space Telescope)
10-m mirror
0.85-m mirror
2-m astronomer
2.4-m mirror
(Hubble Space Telescope)
(Keck Telescope)
11
Local Galaxies - e.g. Luminous Elliptical Galaxies
  • the most massive galaxies in the local
    Universe
  • Pressure-supported, metal-rich stellar systems.
    Simple galactic-scale stellar systems
  • Extremely homogeneous and old (implies zgt2
    formation)
  • Live in the highest density regions (clusters)
  • Largest stellar mass of any galaxies ( up to 10
    M)
  • Host the most massive Black Holes in local
    Universe, gt109Mo
  • HOW ARE THEY MADE ???
  • -observations of the high-z Universe

12
Formation Mechanisms
  • Wide range of proposed mechanisms for forming big
    galaxies
  • (pseudo-)monolithic collapse (TmergeltTSF)
  • major merger of two existing galaxies
    (TmergeTSF)
  • an extended series of minor mergers (TmergegtTSF)
  • Can we observationally distinguish between these
    scenarios?

13
Dust obscured, merging galaxies e.g.,The
Antennae
ISOCAM
ISO 15um
  • Distinct opt/UV and far-IR luminosity
  • 90 emitted at far-IR
  • Dust obscures UV
  • absorbs and re-radiates at longer
    wavelengths
  • (100-200 microns)

HST WFPC2
CSO/SHARC-2 350um
14
The Extragalactic Background
?
  • FIRB opt/UV EBL -gt half of the energy
    production (from SF or AGN) over history of the
    Universe arises in highly obscured regions
  • Much of the star formation in the Universe might
    be obscured resolve FIRB into constituent
    components

15
Components of FIRB (to be studied
directly and indirectly)
350
850
Dole et al. 2005
Submm is almost all high-z galaxies (80
zlt4) MidIR and FarIR is 80 zlt1.7 Radio is
extremely useful, BUT submm best (only?) way to
probe the high-z components of FIRB
16
Studying the obscured activity
SED of an ageing stellar population of solar
metalicity with dust
17
f(24mm) vs Lbol
Papovich and Bell 2003
At far-IR wavelengths, Spitzer can only observe
well at 24 mm what are the bolometric
corrections? theyre large! And especially bad
for the most luminous, dust-obscured
populations. (leave aside for now)
18
Progenitors of Massive Galaxies
  • Review of techniques
  • (focus on submm/radio selection, UV, nearIR)
  • Some key questions and results

19
zgt1.5 Submm Selection (100 zs)
(courtesy I. Smail)
(Smail 2005)
  • Submm galaxies dusty, most of luminosity comes
    out in submm waveband
  • First detected by SCUBA/JCMT in 1997 at 850 ?m
    (Smail1997)
  • Counts 1000/sq. degree at 5 mJy (limit of
    bright SCUBA survey) a few 100 submm galaxies
    IDd
  • In principle, SCUBA sensitive to dusty galaxies
    to zgt6 (negative K-correction) but we now know
    that almost no SCUBA galaxies are that distant!

20
Submm/Radio bolometric selection of galaxies?
Identify SMGs (although Spitzer proving very
useful -- Pope06) -Known tight correlation with
FIR -Good spatial resolution (MERLIN 0.3, VLA
1.4)
FarIR/radio correlation roughly holds at z2.5
(Kovacs et al. 2006)
Far-IR correlates with synchrotron radio (SNe
shock accelerates electrons)
1.4GHz
(Ivison et al. 2002)
21
SCUBA galaxies (SMGs)
High resolution RADIO and HST reveal large,
merging galaxies.
Smail1999,2004 Chapman2003,2004)
greyscale
contours
JCMT/SCUBA
HST
22
SCUBA galaxies (SMGs)
Redshift surveys have given us tremendous insight
into a hyper-luminous population of cool dust
SB-dominated galaxies.
ltzgt2.3
Massive/merging
Chapman03,05, Swinbank04 Pope05
Neri03, Greve05 Genzel02, Tacconi05
IRAM
Keck 10m
23
zgt1.5 Submm Selection
(courtesy I. Smail)
(Chapman et al. 2005)
  • Breakthrough using radio (1.4 GHz) positions
    for optical spectroscopy (ameliorates ambiguity
    from 15 SCUBA beam), 50 of sources have zs
  • Redshifts of 100 SMGs enable study of physical
    properties
  • Typical LIR8x1012L? and dust temperature Td38K
    (confirmed by 350 ?m observations)
  • Less than 10 of submm galaxies are at zgtgt3

24
zgt1.5 Submm Selection
(courtesy I. Smail)
(Chapman et al. 2005)
  • IR luminosities correspond to sfr gt1000 M?/yr
    (Salpeter) if bulk of FIR is powered by star
    formation. If SF lasts for 108 yr, significant
    stellar mass formed
  • Much rarer than other samples, but higher
    inferred SFR, likely contribute significantly to
    SFR density at high z

25
zgt1.5 Submm Selection
(Chapman et al. 2003)
  • Rest-frame UV spectra obtained with Keck/LRIS-B
    (like UV-selected samples)
  • Spectra show features of star-formation and AGN
    (Ly?, NV, CIV, SIV), rest-frame optical spectra
    sometimes NII/H?????or broad H?
  • Raises question of AGN contribution to
    bolometric luminosity, Deep (Chandra 2 Msec
    image) X-ray emission indicates presence of Fe
    K??line, and absorbed non-thermal continuum slope
  • BUT AGN appears not to be energetically
    important -gt submm emission dominated by star
    formation

26
zgt1.5 Submm Selection
Note galaxies w/ smaller star formation rates
not detected yet in CO
(Tacconi et al. 2006)
  • Masses stellar masses estimated from
    SED-fitting (how does AGN affect stellar mass
    estimates?) dynamical masses estimated from H?,
    CO-linewidths cold molecular gas masses
    estimated from CO line luminosities
  • Dynamical masses w/in 10kpc, 2x1011 M?(Swinbank
    et al. 2004, 2006), molecular gas masses 5x1010
    M? (Tacconi et al. 2006)

27
zgt1.5 Submm Selection
  • Submm galaxies appear to be massive systems with
    prodigious star-formation rates, may also be
    strongly clustered (but uncertain because of
    small number of redshifts)
  • Could be progenitors of QSOs, and massive
    galaxies at lower redshift
  • Interesting note several years ago, a lot was
    made of the fact that there was so little overlap
    between submm galaxies and z3 UV-selected
    galaxies. But now we know that most submm
    galaxies are at zlt3, and have similar redshift
    distribution to z2 UV-selected galaxies. gt50
    of submm galaxies have colours of UV-selected
    galaxies (but bigger SFRs)

28
Photometric Pre-selection UV
  • 50 objects/square arcmin down to R25. How do
    you pick out the high-redshift galaxies?
  • Lyman discontinuity at rest-frame 912 A gives
    z3 galaxies very distinctive observed UGR colours

(Steidel et al. 1992, 1993, 1995, 1996, 2003)
29
zgt1.5 Rest-UV Color Selection
  • z3 UGR Lyman Break criteria, adjusted for z2
    (Adelberger et al. 2004)
  • Spectroscopic follow-up with optimized
    UV-sensitive setup (Keck I/LRIS-B)
  • 1000 galaxies at z3, gt750 galaxies with
    spectroscopic redshifts at z1.4-2.5, in what was
    previously called the Redshift Desert

30
Measuring Redshifts z3
  • Meaure Lya em/abs, IS abs at zgt2.5
  • At z 1.4-2.5, these features are in the near
    UV bonus strong rest-frame optical emission
    lines have shifted into the near-IR
  • formerly called THE REDSHIFT DESERT

31
Redshift Desert
  • Low redshift
  • Emission-line z
  • OII, OIII, Hb, Ha
  • At z gt 1.4, OII moves past 9000 AA,
    while Lya below 4000 AA at zlt2.3 no strong
    features in the optical

SDSS galaxy at z0.09
32
Redshift Desert
  • Low redshift
  • Abs-line z
  • 4000 AA break, Ca HK, Mg
  • At z gt 1.4, 4000AA break moves past 9000 AA

SDSS galaxy at z0.38
33
Keck/LRIS-B Efficiency
  • LRIS-B 400/3400 grism --gt 40 efficiency from
    3800-5000 AA
  • Low night-sky background in near-UV (3 mag
    fainter than at 9000 AA)
  • (Steidel et al. 2004)

Unsmoothed
34
Measuring Redshifts z2
  • Low- and high-ionization outflow lines, Ly?
  • He II emission, CIII emission
  • Fewer galaxies have Lya emission (57 have no
    Lya) than in z3 sample (cf. SMG!)
  • (Steidel et al. 2004)

35
Outflow Kinematics z3 vs. z2
  • Kinematic evidence for large-scale outflows is a
    generic feature of UV and submm-selected galaxies
    at zgt2
  • Signature of feedback, perhaps fundamental to
    understanding galaxy formation
  • (Steidel et al. 2004)

z3
z2
Unsmoothed
36
zgt1.5 Rest-UV Color Selection
  • z3 UGR criteria (Lyman Break), adjusted for
    z2 (Adelberger et al. 2004)
  • Spectroscopic follow-up with optimized
    UV-sensitive setup (Keck I/LRIS-B)
  • 1000 galaxies at z3, gt750 galaxies with
    spectroscopic redshifts at z1.4-2.5, in what was
    previously called the Redshift Desert

37
Evolution of Clustering to z1, 0
(Adelberger et al. 2004)
(Blain et al. 2004)
  • Follow evolution of DM halo clustering in
    simulation
  • Matches early-type absorption line DEEP2
    galaxies at z1 (Coil et al. 2003) SDSS Es at
    z0.2
  • Typical UV-selected galaxy at z2-3 will evolve
    into an elliptical by z0

38
Summaryzgt1.5 Rest-UV Colour Selection
  • (typical sfr50-100M?/yr)
  • (typical stellar mass few x 1010M?, large range)
  • What does UV-selection mean in terms of physical
    properties?
  • Star-formation thats only moderately (factor of
    few-100) extinguished by dust, but a large range
    of stellar masses (smaller range of baryonic
    masses), clustering implies that these will
    correspond to early-type galaxies at z0.

39
zgt1.5 Near-IR selection
  • Extension of K20 survey group (i.e., get zs for
    everything with Klt20), use B-z, z-K color
    criteria to select both star-forming galaxies and
    passive galaxies at zgt1.4
  • Incomplete for fainter objects with small Balmer
    Breaks, weighted more towards fairly massive
    objects
  • Significant overlap of BzK/SF with UV-selected
    samples

(Daddi et al. 2004)
40
zgt1.5 FIRES/J-K selection (20 zs)
(Franx et al. 2003)
(Reddy et al. 2005)
  • J-Kgt2.3 criteria meant to select massive evolved
    galaxies with significant Balmer/4000 Å breaks at
    zgt2 turns out selection also yields massive
    dusty starbursts
  • 25 appear to contain AGN (much higher than
    fraction of UV-selected population)
  • Only limited number of spectroscopic redshifts

41
zgt1.5 Summary
  • In addition to UV-selected, BzK, J-K, submm,
    there are other techniques, such as the
    K-band/photo-z technique of the Gemini Deep Deep
    Survey (GDDS), and new Spitzer capabilities IRAC
    (mass-selected), MIPS/24 micron (sfr-selected,
    analogous to SCUBA)
  • Now that there are several groups using
    different selection techniques to find galaxies
    at z2, we need to understand how the samples
    relate to each other (each sample has certain
    benefits but is incomplete e.g., UV-selected
    sample has largest set of redshifts and spectra)
  • Reddy et al. (2005) considered the overlap among
    different samples, and contribution of each to
    the sfr density at z2-2.5

42
At the highest redshifts?
Hard stuff to study! (e.g., contamination)
Controversy at z 6? Did the star formation rate
change from z 6 to z 3? If so, did it
increase or decrease? Each possibility
(increase, decrease, stay the same) had been
claimed by various groups studying z 6 galaxies.
For z 6, Lyais between I z bands, so we are
looking for I-drops R. J. Bouwens, G.D.
Illingworth, J. P. Blakeslee, M. Franx set out
to do the most careful analysis possible and
thereby come to some firm conclusions about such
galaxies.
43
The Star Formation History of the Universe
  • Millimeter/Radio galaxies form most of the stars
    we see today in big bursts
  • 2-5 billion years after the big bang.
  • LESSONS
  • we still dont even know about all the galaxies
    in the Universe!
  • Local galaxies (M31) show unexpected components!
  • Simulations of how galaxies form are not always
    very predictive!

UV-selected
Radio/submm
(Chapman et al. 2005)
44
Key Questions
  • What is the evolution in global sfr and stellar
    mass density vs. z?
  • What is the evolution in number density of
    galaxies as a function of (stellar) mass and
    star-formation rate?
  • What are the star-formation histories of
    galaxies (burst/episodic, continuous), and how do
    they accumulate their stellar mass?
  • What are the origins of different morphological
    types?
  • What is the chemical enrichment in galaxies vs.
    z, and by how much do they enrich their
    surroundings (vs. mass)?
  • What is the effect of supernovae/AGN feedback on
    gas in galaxies and the surrounding IGM?
  • How do we make a continuous timeline of galaxies
    from high redshift to z0 (map one sample to
    another)?

45
Key Techniques/Goals
  • New multi-wavelength technologies are helping us
    address these questions, beyond ground-based
    optical imaging and spectroscopy
  • Wide-field near-IR imaging (stellar masses) and
    near-IR spectroscopy (dynamical masses, sfr,
    chemical abundances)
  • Chandra X-ray observations (sfr and AGN)
  • Spitzer/IRAC (stellar masses) and MIPS (dust
    luminosity, sfr)
  • HST ACS/NICMOS (morphologies)
  • Full understanding of energetics and stellar and
    metal content is a multi-wavelength endeavor
  • Detailed comparison with numerical simulations
    and semi-analytic models

46
Concluding Philosophical Comment
  • Rich set of observations of galaxies in the
    early universe, for statistical samples of
    galaxies selected with different techniques
    (though its still a challenge to get spectra)
  • Theres much more that I could have presented
  • Field of zgt1.5 galaxy evolution is completely
    different since just 10 years ago, when
    UV-selection technique was first implemented
  • Whats happening in the next 10 years?
    (feedback, connecting to samples at other
    redshift, building mass/sfr-limited samples, disk
    galaxies)
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