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OWLS: OverWhelmingly Large Simulations

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Two sets: L = 25 Mpc/h to z=2. L = 100 Mpc/h to z=0 ... Many groups use (nearly) the same subgrid recipes. Insufficient awareness of models ingredients ... – PowerPoint PPT presentation

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Title: OWLS: OverWhelmingly Large Simulations


1
OWLS OverWhelmingly Large Simulations
The formation of galaxies and the evolution of
the intergalactic medium
2
Outline
  • Introduction to OWLS
  • Radiative cooling
  • Feedback from star formation
  • Star formation histories
  • Intragroup medium
  • Gas accretion

3
OWLS people
4
OWLS features
  • LOFAR IBM Bluegene/L
  • Cosmological (WMAP3), hydro (SPH)
  • Modified Gadget III
  • 2xN3 particles, N 512 for most
  • Two sets
  • L 25 Mpc/h to z2
  • L 100 Mpc/h to z0
  • Runs repeated many times with varying
    physics/numerics

5
Video of the evolution of a massive galaxy down
to z2
3 Mpc/h
6
Zoom
CDV, OWLS project
7
OWLS New gastrophysics modules
  • Star formation JS Dalla Vecchia (2008)
  • Galactic winds Dalla Vecchia JS (2008)
  • Radiative cooling Wiersma, JS, Smith (2008)
  • Chemodynamics Wiersma et al.
  • AGN feedback Booth et al.

8
Radiative cooling (above 104 K)
  • What is typically done
  • H and He including optically thin
    photo-ionization
  • Metal cooling ignored or assuming CIE and solar
    relative abundances

9
Video of density dependence
Wiersma, JS Smith (2008)
10
Radiative cooling above 104 K
  • Photo-ionization suppresses metal cooling ?
    cooling rates decrease by up to an order of
    magnitude
  • Relative abundance variations are important ?
    cooling rates change by factors of a few
  • Tables of cooling rates, element-by-element,
    including photo-ionization available

Wiersma, Schaye Smith, arXiv0807.3748
11
Galactic winds
  • Thermal feedback is quickly radiated away due to
    lack of resolution
  • Solutions
  • Kinetic feedback
  • Temporarily suppress cooling
  • Most cosmological simulations employ the SPH code
    Gadget, which uses kinetic feedback
  • Our kinetic feedback differs from that of Gadget
  • Not hydrodynamically decoupled
  • Winds are local to the SF event

12
1e12 M?, face-on, gas density
Dalla Vecchia JS (2008)
13
1e12 M?, edge-on, gas density
Dalla Vecchia JS (2008)
14
1e12 M?, edge-on, gas pressure
Dalla Vecchia JS (2008)
15
Galactic winds
  • Hydro drag determines outcome,
  • gravity only indirectly important
  • Low mass galaxies
  • wind drags lots of gas out to the IGM
  • High mass galaxies drag quenches wind ? fountain
  • Most popular existing prescription overestimates
    the energy in the outflow by orders of magnitude
  • The details of wind implementations have grave
    consequences

Dalla Vecchia Schaye, 2008, MNRAS, 387, 1431
16
Lots of plots of SFR histories
  • Most of these were flashed by

17
Simulating galaxy statistics
  • Cooling and feedback are crucial, SF law and
    structure of the ISM are not
  • (Too) much freedom in implementation of galactic
    winds

18
Groups at z0 Scaled entropy
McCarthy et al.
19
Groups at z0 Scaled entropy
McCarthy et al.
20
Groups at z0
  • Massive galaxies reside in groups ? detailed
    information about gaseous environment from X-ray
    observations at z0
  • Highly sensitive to (metal) cooling and feedback
  • Simulations can match detailed entropy,
    temperature, density and abundance profiles
    surprisingly well
  • But it is a challenge to reproduce both the
    optical and X-ray properties of groups

21
How do galaxies get their gas?
  • Classical picture Gas-shock heated to the virial
    temperature, then cools onto disk
  • Recent modifications
  • Much of the gas falls in cold through filaments,
    particularly in low-mass galaxies
  • Efficient AGN feedback requires a hot halo
  • Galaxy bi-modality may be caused by transition
    from cold to hot accretion

22
Hot and cold accretion
23
Hot and cold accretion
  • Did not get to these slides

24
Gas accretion - Conclusions
  • Cold accretion fraction sensitive to definition
  • Halo accretion
  • Independent of subgrid physics
  • Hot fraction increases with mass and with
    decreasing redshift
  • Smooth transition from cold to hot
  • Disk accretion
  • Sensitive to subgrid physics
  • Cold accretion dominates at all masses unless it
    is stopped by feedback

25
Conclusions 1/2
  • Some predictions from hydro simulations suffer
    from subgrid uncertainties (e.g. SSFRs, LFs),
    others are robust (e.g. accretion onto halos)
  • Even when predictions are uncertain, hydro
    simulations can pinpoint the important physical
    processes, e.g.
  • Star formation laws are helpful but not
    constraining
  • Cooling can and must be done better
  • Freedom in feedback implementations is currently
    the bottleneck ? need higher resolution and a
    better treatment of metal mixing
  • Realistic simulations of the formation of
  • Individual high-z dwarfs are within reach
  • Massive galaxies are still far beyond the horizon
  • Comparisons with galaxy surveys are too
    challenging and not always the most productive
    strategy

26
Conclusions 2/2
  • Progress is most likely to come from studies of
    gas properties
  • intergalactic, intra-group and intra-cluster
    media Available hard X-ray profiles
  • Needed soft X-ray and UV at high (spectral)
    resolution
  • HI and CO structure of individual galaxies
  • QSO/GRB absorption spectra
  • DANGERS (rant)
  • Many groups use (nearly) the same subgrid recipes
  • Insufficient awareness of models ingredients
  • Much more discussion about numerical accuracy
    (e.g. resolution and SPH vs grid) than subgrid
    uncertainties
  • Pressure to reproduce observations
  • Subgrid variations are at least as important as
    convergence tests!
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