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Simulating the Bullet Cluster Is there Evidence for a LongRange NonGravitational Force

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Simulating the Bullet Cluster. Is there Evidence for a Long-Range Non-Gravitational Force? ... GRF Rachel Rosen astro-ph/0610298, Phys Rev Lett in press ... – PowerPoint PPT presentation

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Title: Simulating the Bullet Cluster Is there Evidence for a LongRange NonGravitational Force


1
Simulating the Bullet Cluster Is there Evidence
for a Long-Range Non-Gravitational Force?
  • Glennys R. Farrar
  • Center for Cosmology and Particle Physics
  • New York University
  • Based on
  • GRF Rachel Rosen astro-ph/0610298, Phys
    Rev Lett in press
  • Volker Springel GRF astro-ph/0703232

2
Long Range 5th Force
  • Natural in many theories, e.g., superstrings or
    matter in a shadow universe.
  • 5th force is NOT MOND.
  • 5th force cant couple to ordinary matter
    (Eotwash limits)
  • 5th force may not simply decrease with distance,
    e.g., may be screened in dense concentrations of
    matter (chameleon models)
  • Strategy measure the mass of a DM concentration
    and the acceleration it produces -- Is the
    acceleration consistent with gravity alone?
  • If 5th force exists, DM coupling to ordinary
    matter must be very weak (radiative corrections
    Eotwash)

3
Possible Benefitsof an attractive 5th force
  • Enhances structure formation for a given density
    contrast. This helps because
  • Large Scale Structure simulations fit power
    spectrum with ?8 0.9, but ?8 0.75 from WMAP3
    (further exploration needed)
  • 10 times more super-clusters observed in SDSS
    than in LCDM simulations (Einasto et al,
    astro-ph/06)
  • Voids in LCDM simulations not empty enough (?) --
    5th force helps (GRF P.J.E.Peebles Ap. J.
    6401(2004). D. Croton GRF in prep)
  • Too much late accretion in LCDM simulations
    (Nusser, Gubser, Peebles astro-ph/0412586)
  • Baryons are less tightly bound, explaining
  • Fewer DM substructures in galaxies than predicted
    by LCDM simulations

4
IE0657-56 bullet cluster, Z 0.3
  • X-ray observations
  • (Markevitch astro-ph/0511345)
  • Mach 3.0 0.4 Velocity
  • V rel_DM 4740- 550 630 km/s
  • Tclus 14 keV

5
Statistical Approach(Hayashi and White MNRAS
370, L38 (2006))
  • HW
  • Parameterize distribution of vsubcl/v200 in
    Millenium Run.
  • HW used early estimate
  • vsubcl / v200 1.9
  • probability ? 1/500 to find subcluster as fast as
    bullet.
  • Latest values of vsubcl and v200
  • vsubcl / v200 2.7
  • probability ? 10-6 to find subcluster as fast as
    bullet

6
Expected Velocity from Gravitational Acceleration
(GRF Rachel Rosen, astro-ph/0610298, PRL in
press)
  • Simplest assumptions gives Fiducial model
    vrel 2950 km/sec
  • Consider alternate density profiles, initial
    conditions, mass accretion histories
    Conspiracy model (uncertainties conspire to
    maximize velocity)
  • vrel 3435 km/sec
  • Other uncertainties reduce the predicted velocity
  • If measurements and their interpretations are
    correct, we seem to need an attractive 5th force
    on ranges Mpc with strength GN

7
Simulation of Bullet DM gas V. Springel
GRF astro-ph/0703232
8
Default Toy Model V. Springel GRF
astro-ph/0703232
  • Spherical NFW Profiles, truncated at virial
    radius, (parameters from Clowe, private
    communication)
  • Main Cluster M200 1.5 1015 M? c 2.0
    rvir 2300 kpc
  • Subcluster M200 1.5 1014 M? c 7.2
    rvir 1070 kpc
  • v 0 at 8 when touch, vsubcl 1870 km/s (C.M.)
  • GADGET2 N-Body/SPH (Springel et al 05)
  • 3-D (essential to get gas dynamics right)
  • 4.4 106 particles (mgas 1.3 108 M?, mDM 6.2
    108 M?)
  • Rerun best-fit case with 8x more particles -- no
    visible change.

9
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10
X-ray Surface Brightness
11
Luminosity-weighted projected Temperature
12
Best Matching Snapshot with Basic Modelt 1340
Myr (180 Myr after core passage)
Data from Markevitch, our contours (private
communication)
13
t 1340 Myr (180 Myr after core passage) Mach
2.8
14
Positions of Landmarks as a function of time
Velocities of Landmarks as a function of time
15
Using different initial concentrations
16
Best-fit model compared to data
17
Off-Center Collision (12.5 kpc offset)
Plane of sky
45o to plane of sky
Perpendicular to plane of sky
18
Add fifth force (no other changes here)
? 1
? 0.3
Clear potential to constrain 5th force (V.
Springel GRF -- stay tuned)
19
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20
Conclusions
  • Bullet Cluster
  • Relative DM velocities 2600 260 km/s .
  • Agrees well with fiducial prediction of GRFRAR
    (2950 km/s)
  • NO NEED for FIFTH FORCE
  • Custom Simulations of Merging Clusters
  • Must include DM and gas dynamics! (Naïve
    Markevitch et al estimate vrel Mach ? cs
    overestimates vrel, DM by 70)
  • Fully realistic simulations essential (2D
    simulation of Milosavljevic et al astro-ph/070319
    16 instead.)
  • Custom simulations will be a very powerful tool.
  • Many observables to fit. Precision observations
    crucial!
  • .

21
Keep Observing and Testing!
  • kpc scales Milky Way dwarfs (oblate-prolate
    paradox!)
  • Mpc scales cluster dynamics -- peculiar
    velocity weak lensing
  • Cosmological scales -- LSS simulations
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