Detailed Astrophysical Properties of Lyman Break Galaxies

Download Report

Transcript Detailed Astrophysical Properties of Lyman Break Galaxies

Observations of High Redshift
Galaxies with CCAT
Alice Shapley (Princeton University)
October 10th, 2005
Overview
• CCAT will provide new windows on star formation
for sub-ULIRG star-forming galaxies at high
redshift, including information about dust, gas
content, HII region physical conditions, and starformation feedback
• New results at shorter (optical through mid-IR)
wavelengths, CCAT observations will greatly
enhance their meaning
2
New results
• Spitzer 24 mm observations provide estimates of
Lbol for L~1011-1012 L galaxies (LIRGS) at z~2-3,
but this is indirect
• M-Z relation, gas fractions in star-forming galaxies
at z~2, using optical and near-IR imaging and
spectroscopy
• Physical conditions appear to be different in high
redshift HII regions (z~1-2), based on rest-frame
optical emission lines
3
Relevant Observations with CCAT
• submm continuum --> LFIR, Lbol, Tdust
• CO lines --> Mgas (molecular, assuming conversion
factor), gas fractions, Schmidt law
• [CII] 158 mm, [OI] 63 mm, [OIII] 88, 52 mm -->
(HII region and ISM physical conditions, densities,
cooling)
• Different probes of star formation
4
z>2 color-selection
• Adjust z~3 UGR crit. for z~2 (Adelberger et al. 2004)
• Spectroscopic follow-up with optimized UV-sensitive
5
setup (Keck I/LRIS-B) (Steidel et al. 2004)
z>2 color-selection
• Adjust z~3 UGR crit. for z~2 (Adelberger et al. 2004)
• Spectroscopic follow-up with optimized UV-sensitive
6
setup (Keck I/LRIS-B) (Steidel et al. 2004)
Redshift Distributions
LBG: z~3 (940)
SLBG=1.7/arcmin2
nLBG=1.4x10-3Mpc-3
BX: z=2-2.5 (816)
SBX=5.2/arcmin2
nBX=2.0x10-3 Mpc-3
Unsmoothed
BM: z=1.5-2.0 (118)
SBM=3.8/arcmin2
nBM=1.7x10-3Mpc-3
750 gals at z=1.4-2.5
BX/BM/LBG with R<=25.5
(Steidel et al. 2004;
7
Adelberger et al. 2004)
Redshift Distributions
Other surveys & space densities:
LBG: z~3 (940)
• K20 (z=1.4-2.5): ~10-4/Mpc3 SLBG=1.7/arcmin2
• GDDS (z=1.6-2.0):~10-4/Mpc3nLBG=1.4x10-3Mpc-3
• SMG (z~2.5): ~10-5 /Mpc3
• FIRES(z=2-3.5): uncertain BX: z=2-2.5 (816)
SBX=5.2/arcmin2
nBX=2.0x10-3 Mpc-3
Unsmoothed
BM: z=1.5-2.0 (118)
SBM=3.8/arcmin2
nBM=1.7x10-3Mpc-3
750 gals at z=1.4-2.5
BX/BM/LBG with R<=25.5
(Steidel et al. 2004;
8
Adelberger et al. 2004)
Other redshift desert surveys
Other surveys with galaxies at z~1.4-2.5
• K20/BzK (Cimatti et al.) (K<20 selection) (~40)
• Gemini Deep Deep (Abraham et al.) (K<20.6, photo-z) (34)
• FIRES (Franx, van Dokkum et al.) (J-K selection) (~10)
• Radio-selected SMG (Chapman et al.) (73) (+18 OFRG)
Now that there are several groups using different selection
techniques to find galaxies at z~2, we need to understand how
the samples relate to each other.
9
Dust: Bolometric Luminosities
and Extinction
Mid-IR Lum. from Spitzer/MIPS
• Spitzer/MIPS 24 mm
band probes PAH
emission at z=1.5-2.6,
probe of L5-8mm
• Average ratio of L5-8
to LIR is 28.3 for local
star-forming galaxies;
use this to convert
MIPS to bolometric IR
luminosities
(Reddy et al. 2005)
• Optical and near-IRselect gals at z~2 have
<LIR>~3-5x1011 L
11
Mid-IR Lum. Vs. LX(bol)
• Using z~2 galaxies in
the GOODS-N field, it
is possible to do X-ray
“stacking” analysis, as
a function of L5-8 (1020 gals per bin)
• LX probes bolometric
SFR (not AGN)
• Strong linear
correlation between
L5-8 and LX
(Reddy et al. 2005)
• Evidence that L5-8 is
a good SFR indicator
12
Mid-IR Lum. Vs. LFIR(bol)
• Compare LFIR
derived from L5-8 with
LFIR measured from
SCUBA and other
sources
• For SCUBA/SMG
sources, FIR inferred
from MIR is low by a
factor of ~2-10 (Tdust,
AGN)
(Reddy et al. 2005)
• We need direct
comparisons for
fainter galaxies
(CCAT)!!
13
Lbol vs. Dust Extinction
• Relationship between Lbol
and extinction evolves from
z~0 to z~3
• Galaxies at fixed
extinction are ~100X more
luminous (or galaxies at
fixed luminosity are less
dusty)
• Geometry, evolution of
dust distribution
• Direct Lbol at high-z is
critical for this analysis
• CCAT will provide this
(Tdust, Lbol)
(Reddy et al. 2005)
14
Metallicities & Gas Fractions
Evolution of Galaxy Metallicities
• Gas phase oxygen abundance in star-forming galaxies
• Fundamental metric of galaxy formation process, reflects
gas reprocessed by stars, metals returned to the ISM by SNe
explosions (HII regions in sf-galaxies, stars in early-type).
• Departures from closed-box expectations can reveal
evidence for outflow/inflow
• Galaxies display universal correlations between Luminosity
(L), Stellar mass (M), and metallicity (Z)
• 10,000s of galaxies in the local universe with O/H
• Now the challenge is to obtain these measurements at high
redshift (evolution will give clues)
• Measuring gas fractions is very important to quantify how
much material has been processed into stars -- currently very
16
indirect!!!
Abundance Indicators: Bright (R23)
• High-Z branch:
R23 decreases as Z
increases
• Low-Z branch:
R23 decreases as Z
decreases
• Uncertainty in
which branch R23
corresponds to
(Kobulnicky et al. 1999)
• Systematic
differences from
17
direct method
Local L-Z Relationship
• Lots of local emission
line measurements
(10000’s, 2dF, Sloan)
• At z=0.5-1, 3 groups
(>=200 gals, CFRS,
DGSS, CADIS, TKRS)
• At z>2 there were
< 10 measurements
(mainly LBGs)
(Tremonti et al. 2004)
• DLAs provide
metallicity information
from abs lines, but
hard to relate
18
Local M-Z Relationship
• M-Z possibly more
fundamental than L-Z
relationship
• closed box model
relates gas fraction
and metallicity,
according to the yield
• SDSS sample
revealed lower
effective yield in lower
mass galaxies
(Tremonti et al. 2004)
• importance of
feedback
19
Near-IR spectroscopy of z~2 gals
• z~2 ideal for measuring several neb lines in JHK
• evidence of M-Z relation at z~2, gas fractions are
necessary part of interpretation (CCAT)
20
[NII]/Ha ratios: z~2 metallicities
• relationship
between [NII]/Ha
and O/H
• N is mixture of
primary and
secondary origin
N2=log([NII] 6584/Ha)
12+log(O/H)=8.9+0.57xN2
s~0.18, factor of 2.5 in O/H
• age, ionization,
N/O effects, integ.
spectra, DIG, AGN
(Pettini & Pagel
2004) 21
z~2 M-Z Relationship
• New sample of 87
star-forming galaxies
at z~2 with both M*
and [NII[/Ha (gas
phase O/H)
measurements
• Divide into 6 bins in
M* , which increases
as you move down
• clear increase in
[NII]/Ha with
increasing M*
(Erb et al. 2005)
• M-Z at z~2!!
22
z~2 M-Z Relationship
• Evol. Comparison
with SDSS, where Z is
based on [NII]/Ha (for
both samples)
• Clear offset in
relations --> at fixed
stellar mass, z~2
galaxies significantly
less metal rich than
local gals
(Erb et al. 2005)
• Not evolutionary (z~2
probably red&dead by
z~0)
23
z~2 M-Z Relationship
• Important: measure
change of Z with m
(gas fraction)
• Must estimate Mgas,
which we do from SHa,
to Ssfr, to Sgas
(assuming Schmidt
law)
• Very indirect!
• Low stellar mass
objects have much
higher m
(Erb et al. 2005)
24
z~2 M-Z Relationship
(Erb et al. 2005)
• Different models for feedback, using different yields and different
outflow rates
• Data are best fit by model with super-solar yield and outflow rate
greater than SFR (for all masses)
• Rate of change of m with metallicity gives evidence for feedback ; m is
25
very important (measure with CCAT, CO lines)
HII Region Physical Conditions
z~2 Physical Conditions
• Well-defined sequence
in [OIII]/Hb vs. [NII]/Ha
in local galaxies (SDSS)
(star-formation vs. AGN)
• z~2 star-forming
galaxies are offset from
this locus (as is DRG)
• ne, ionization parameter,
ionizing spectrum (IMF,
star-formation history)
(Erb et al. 2005)
• Implications for derived
O/H
27
z~1 Physical Conditions
• Well-defined sequence
in [OIII]/Hb vs. [NII]/Ha
in local galaxies (SDSS)
(star-formation vs. AGN)
• z~1.4 star-forming
galaxies are offset from
this locus (as is DRG)
• ne, ionization parameter,
ionizing spectrum (IMF,
star-formation history)
(Shapley et al. 2005)
• Implications for derived
O/H
28
z~2 Physical Conditions
• Among K<20
galaxies (brightest
10%), [SII] line ratio
indicates high
electron density
• Inferred electron
density is ~1000/cm3,
• This is higher than
in local HII regions
used to calibrate N2
vs. O/H relationship
(Pettini et al. 2005)29
Beyond [NII]/Ha: All the lines
O
H O
HN
• Deriving Oxygen
Abundance from
[NII]/Ha relied on
several assumptions
• Physical conditions
appear different.
Observations of full
set of lines important
for constraining sfr in
high redshift objects
• GNIRS/Gemini
(van Dokkum et al. 2005)
30
Beyond [NII]/Ha: All the lines
O
H O
HN
• FIR [OIII] lines,
accessible with CCAT
at l>200 mm for z>1.5
• independent probe
of HII region physical
conditions
• [CII] 158 mm line,
probes physical
conditions in different
phase (compare with
CII* 1335)
(van Dokkum et al. 2005)
31
Summary
• New results about dust, star formation, chemical
enrichment, and feedback, using optical, near-IR, and
mid-IR imaging and spectroscopy
• CCAT observations can provide independent
measurements of dust, gas, and star-formation rates for
these objects, as well as probing physical conditions
• Both continuum and line emission measurements will
be crucial for physical understanding
32
Q1700+64: Distribution of M*
6/72 have
M*>1011M &
contain 50% of
the mass
(Steidel et al. 2005)
• Mstar,med=2.0x1010 Msun
• Distributions with and
without IRAC data very
similar (uncertainties
smaller with IRAC data)
• Stellar mass density of z~2
BX/MD galaxies is
~108MsunMpc-3 16% of z=0
stellar mass density (Cole et
al. 2001)
• caveats: IMF, bursts
• relate to z~3, evolution
(???? Weak constraints)
• Better constraints for most
massive gals (8%)
33
Direct Abundance Determination
Z=1/25 Zsun
• Use [OIII] 4363/(5007,4959) to get Te, [SII] to get ne
• Problem: 4363 weak, even in local low-Z gals; star-forming
gals are not very metal-poor--NO HOPE at high redshift
(figure from van Zee 2000)
34
L-Z relation and evolution
• Correlation over
11 mags in MB
and factor of 100
in (O/H) (SF gals)
• Ellipticals show
analogous trend
(Garnett 2002)
Evolution of L-Z provides clues…
• Fainter gals
have higher gas
fraction (younger,
lower Ssfr); or
outflows more
important 35
Stellar Populations & Masses
Near/Mid-IR Imaging
Ks (2.15 mm)
(Barmby et al. 2004, Steidel et al. 2005)
• Deep J, K imaging with
WIRC, Palomar 5-m, to
Ks~22.5, J~23.8
• 4 fields, ~420 galaxies
with zsp> 1.4
• Spitzer IRAC data in
Q1700 field, 3.6, 4.5, 5.4, 8
mm
• Use for modeling stellar
populations, masses
36
Stellar Populations & Masses
Near/Mid-IR Imaging
IRAC (4.5 mm)
(Barmby et al. 2004, Steidel et al. 2005)
• Deep J, K imaging with
WIRC, Palomar 5-m, to
Ks~22.5, J~23.8
• 4 fields, ~420 galaxies
with zsp> 1.4
• Spitzer IRAC data in
Q1700 field, 3.6, 4.5, 5.4, 8
mm
• Use for modeling stellar
populations, masses
37
Near-IR spectroscopy of z~2 gals
M*=41011 M
K=19.3, J-K=2.3
M*=5109 M
Ha spectra of 101 z~2
gals KeckII/NIRSPEC
• Kinematics: linewidths,
Mdyn, some spatiallyresolved, tilted lines,
compare with stellar
masses
• Line ratios: HII region
metallicities, physical
conditions
• Ha fluxes: SFRs, compare
with UV, models
• Offsets between nebular,
UV abs and Lya em
redshifts -> outflows 38
Measuring gas masses at z~1-3
• In addition to filling in huge gap in O/H vs. z, and testing
evolution of L-Z relation….
• In simple closed-box chemical evolution models:
Z=y ln (1/m)
• m=Mgas/(Mstar+Mgas), y=yield of heavy elements
• Using broad-band photometry, fit stellar populations and
determine Mstar
• Test for the importance of outflows (effective yield)
39
Measuring O/H at z~1
• At z~1.3-1.4, [NII]/Ha in Hband, [OIII]/Hb in J-band
• At z~1, [NII]/Ha in J-band,
[OIII]/Hb in NIRSPEC1 band
• DEEP2 gals already have [OII]
• DEEP2 z-hist from Coil
et al. 2004, ~5000 gals,
10% of survey
• Statistical O/H sample
(50-100) at z=1-1.5 40
Different Estimates of Dust
• b measures dust
from UV slope
• LFIR/L1600 measures
dust from inferred
ratio of FIR (based on
MIPS) to UV
luminosity
• Local starbursts
show correlation
between b and FIR/UV
(Reddy et al. 2005)
• MIPS implies
correlation works for
z~2 galaxies on avg.
41
Does Calzetti Work?
• Stack 171 zspec=1.4-2.5 S.F. galaxies
(excluding all direct detections, AGN)
• 10s detection in X-ray
<SFR(Xray)> = 42 Msun/yr
• 5s detection in radio 
<SFR(Radio)>=50Msun/yr (LIRG)
• Corresponds to <SFR(1500)> = 8.5 Msun/yr
• <A(1500)>= factor of 4.9, very similar to
results at z~3, and to inference from UV colors
with CSF+Calzetti
Chandra Stack
(CDFN 2Ms exposure)
(Reddy & Steidel
2004)
• K<20 z=1.4-2.5 BX/BM: <SFR(Xray)>=130
Msun/yr (Reddy et al. 2005)
Star-forming BzK gals: <SFR(Xray)>=170
42
Msun/yr (Daddi et al. 2004)