Transcript 幻灯片 1 - The Kavli Institute for Astronomy and
Modeling the dependence of galaxy clustering on stellar mass and SEDs Lan Wang Collaborators: Guinevere Kauffmann (MPA) Cheng Li (MPA/SHAO, USTC) Gabriella De Lucia (MPA)
Outline
• Introduction : theory of galaxy formation • New parameterized models: Modeling galaxy clustering in a high resolution simulation of structure formation Modeling the dependence of clustering on spectra energy distributions of galaxies
Galaxy formation
• Galaxy formation includes two steps: e.g.
White & Rees 1978
Dark matter haloes form through gravitational collapse Galaxies form in dark matter halos by cooling of baryonic material — physical processes : gas cooling, star formation, SN feedback, AGN feedback, mergers etc.
Properties of dark matter haloes
Cold dark matter cosmology: structures grow hierarchically • Dark matter halos : Abundance
Press & Schechter 1974
Merger tree Density profile (NFW)
Navarro, Frenk & White 1996,1997
Link galaxy properties to DM halos • Hydrodynamic Simulation e.g.
White, Hernquist & Springel 2001
• Semi-analytic models
Kauffmann et al. 1999
• Halo Occupation Distribution models (HOD) | )
Berlind & Weinberg 2002
)
Yang, Mo & van den Bosch 2003
SAM HOD
Our Methodology
• • Falls in between semi-analytic method & HOD approach: Positions, velocities and formation history from simulation Parameterized functions to determine galaxy properties Based on
Millennium Simulation
M infall - halo mass at infall time t infall ‘Orphan’ galaxies – satellites without subhalos vs. HOD: halo mass of today Two steps • M infall →M stars • t form , t infall →SFH →D n 4000
The Millennium Simulation
Springel et al. 2005
Cosmological parameters:
m h
0.25,
b
0.73,
n
1, 8 0.045, 0.9
0.75
Particles:
N
3 8 1
h M
1 Boxsize: 500
h Mpc
M stars vs. M infall in semi-analytic catalogue
Croton et al. 2006
Statistics reproduced
vs.
semi-analytic results Stellar mass Function Correlation
Central, satellite & ‘orphan’ L & M infall Luminosity Function
‘orphan’ galaxies
• Critical for correlation at small scales
Application to SDSS
• Fit stellar mass function & clustering for different stellar mass bins Separate relations for central/satellite give better fit
Fitted relations
• Satellites are less massive than centrals •
Mandelbaum et al. 2006
SDSS observation
central young & satellite old?
SAM including AGN feedback e.g.
Croton et al. 2006; Bower et al. 2006
Modelling SFH
• Exponentially evolved SFR with time scales
c
(
M
) and
s
(
M
) central satellite t form t infall t present
Bruzual & Charlot 2003 model
• Concentrate on D n 4000 because of its weak dependence on dust
Clustering dependence on SEDs • M infall M stars metallicity
Gallazzi et al. 2005
• t form , t infall
c s
metallicity SFH
BC03
D n 4000 + M stars positions
Non-parametric fit
c
c
parameterized by a sum of Gaussians: • For satellite galaxies, assume simple Gaussian dispersion for
s
(
M
)
Best-fit:
Constant SFR:
c
1/
c
0 0
Main results
• Massive centrals have ceased forming stars • At low stellar masses, central galaxies display a wide range of different SFH, with a significant fraction experiencing recent star bursts.
• Time scale for satellite galaxies is almost independent of stellar mass
Consistency checks
• Specific SFR: our model
vs.
SDSS results • g-r distributions
SFH: compared with SAM
(
De Lucia & Blaizot 2006
) • e-folding time scale for satellites our model: ~2-2.5 Gyr SAM: ~1Gyr
Evolution to higher redshifts
• D n 4000 – local density relation redshifts: 0 0.3
0.8
1.5
2 3 • VVDS & DEEP2
Cucciati et al. 2006 Cooper et al. 2006
Conclusions
A new statistical model of galaxy clustering • Double power-law form for M stars ~ M infall relation • Applied to SDSS: For a given M infall , satellites are less luminous and less massive than centrals Clustering dependence on SEDs reproduced Massive central galaxies have ceased forming stars; At low stellar masses, a significant fraction of central galaxies have recent starbursts Satellite galaxies of all masses have declining SFR, with
s
~ 2.5
Gyr
Thank You
!
Full non-parametric test
• Time scale for satellite galaxies is almost independent of stellar mass