Title: Predictions for surveys with HERSCHEL from a CDM model of galaxy evolution
1Predictions for surveys with HERSCHEL from a CDM
model of galaxy evolution
- Cedric Lacey
- Durham University
2Collaborators on theoretical models
- Galaxy formation models
- Carlton Baugh Durham
- Shaun Cole Durham
- Carlos Frenk Durham
- Andrew Benson Oxford
- Dust Modelling
- Alessandro Bressan Padova
- Gian Luigi Granato Padova
- Laura Silva Trieste
3Galaxy formation in the CDM model key physical
processes
- Assembly of dark matter halos
- Shock-heating and radiative cooling of gas within
halos - Star formation and feedback
- Production of heavy elements
- Galaxy mergers
4Galaxy formation made simple
- gas cools to make disks
- halos merge
- galaxies merge by dynamical friction
- major mergers make galactic spheroids from disks
- mergers trigger starbursts
- spheroids can grow new disks
5Modelling the stars dust
- dust in diffuse medium and molecular clouds
- stars form in clouds and leak out
- stellar emission from population synthesis
- radiative transfer of starlight through dust
distribution - heating of dust grains -gt dust temperature
distribution
GRASIL code Silva etal 1998, Granato etal 2000
6More details of dust modelling
- Physical model for dust grains, chosen to
reproduce local ISM extinction law - Mixture of graphite silicate grains, with
distribution of grain sizes - Includes PAHs (polycyclic aromatic hydrocarbons)
- Assume dust/gas proportional to gas metallicity
- Optical depth for dust depends on both dust mass
and galaxy radius - these both predicted by galaxy formation model
7Model for radio emission
- Free-free radiation from HII regions ionized by
young stars
- Synchrotron radiation from relativistic
electrons accelerated in supernova remnants
assume const frac of SN energy radiated
(Bressan, Silva Granato 2002)
8Example Model SED (1)
- unextincted starlight
- ( radio)
9Example Model SED (2)
- starlight with dust extinction
10Example Model SED (3)
- starlight with dust extinction
- emission from diffuse dust
11Example Model SED (4)
- starlight with dust extinction
- emission from diffuse dust molecular clouds
12Example Model SED (5)
- starlight with dust extinction
- emission from diffuse dust molecular clouds
- total
13SEDs from dust model comparison with
observations
- model predicts galaxy spectrum from far-UV to
sub-mm - accurately reproduces observed SEDs for nearby
normal and starburst galaxies
14Important features of galaxy formation model
- Star formation timescale in quiescent disks
- disks more gas-rich at high z
- mergers more gas-rich at high-z
- Bursts triggered by minor and major mergers
- Top-heavy IMF in bursts
Cole etal 2000 Granato etal 2000 Baugh etal 2004
15Cosmic star formation history
total
quiescent
quiescent
bursts
bursts
16Present-day galaxy luminosity functions in
optical near-IR
B-band
K-band
total
total
no dust
quiescent
no dust
quiescent
bursts
bursts
17Present day luminosity functions in far-UV
far-IR
Far-UV (2000 A) Far-IR (60
mm)
total
total
no dust
bursts
bursts
quiescent
quiescent
18Sub-mm source counts
850 mm
- model predicts
- at observed fluxes, counts dominated by galaxies
with ongoing burst of star formation triggered by
galaxy merger - at very faint fluxes, dominated by quiescent disks
total
total
bursts
bursts
quiescent
quiescent
19Redshift distribution of sub-mm sources
- model predicts median z2 for S(850)1-10 mJy
- consistent with observational constraints (e.g.
Chapman etal 2003, z(median)2.4 at S5mJy)
total
bursts
quiescent
20Galaxy luminosity function in rest-frame UV at z3
Lyman-break galaxies
- Lyman-break galaxies dominated by ongoing bursts
- dust extinction has huge effect on predicted
luminosity function - most of UV radiation emitted by stars is
absorbed by dust
no dust
bursts
total
quiescent
21Predictions for HERSCHEL
22Sensitivities in different bands
Diffraction limit 40 beams per source,
galaxies only
23PACS 60-90 mu
24PACS 90-130 mu
25PACS 130-210 mu
26SPIRE 250 mu
27SPIRE 350 mu
28SPIRE 500 mu
29Comparison with SPITZER 24 70 mu
30Comparison with ASTRO-F
N60 50-75 mu
N170 150-200 mu
WIDE S 50-110 mu
WIDE L 110-200 mu
31Evolution of bolometric (8-1000 mu) LF
Z0
Z2
Z4
32Cumulative fraction of bolometric (8-1000 mu)
luminosity gtL
Z0
Z2
Z4
33Bolometric (8-1000 mu) luminosity vs S(75mu)
Z0.5
Z1
Z2
Z3
34Bolometric (8-1000 mu) luminosity vs S(250mu)
Z0.5
Z1
Z2
Z3
35Bolometric (8-1000 mu) luminosity vs S(500mu)
Z0.5
Z1
Z2
Z3
36Bolometric (8-1000 mu) luminosity vs S(24mu)
Z0.5
Z1
Z2
Z3
37Bolometric (8-1000 mu) luminosity vs S(850mu)
Z0.5
Z1
Z2
Z3
38SFR vs S(250mu)
Z0.5
Z1
Z2
Z3
39Stellar mass vs S(250mu)
Z0.5
Z1
Z2
Z3
40Flux in other bands vs S(250 mu) _at_ z0.5
75mu
500mu 24mu
850mu
1.4GHz I
band
41Flux in other bands vs S(250 mu) _at_ z1
75mu
500mu 24mu
850mu
1.4GHz I
band
42Flux in other bands vs S(250 mu) _at_ z2
75mu
500mu 24mu
850mu
1.4GHz I
band