Dark Matter Substructure and Dwarf Galactic Satellites

13
Dark Matter Substructure and Dwarf Galactic Satellites By Andrey Kravtsov Presented By Curtis McCully Thursday, October 8, 2009

Transcript of Dark Matter Substructure and Dwarf Galactic Satellites

Page 1: Dark Matter Substructure and Dwarf Galactic Satellites

Dark Matter Substructure and Dwarf

Galactic SatellitesBy Andrey Kravtsov

Presented By Curtis McCully

Thursday, October 8, 2009

Page 2: Dark Matter Substructure and Dwarf Galactic Satellites

Outline• Introduction

• CDM Simulations vs Observations

• Quantifying the Substructure Problem

• Dark Satellites

• Luminous Satellites

• Possible Solutions

• New Cosmological Model

• Galaxy Formation Suppression

Thursday, October 8, 2009

Page 3: Dark Matter Substructure and Dwarf Galactic Satellites

Fig. 1— Formation of a Milky Way-sized dark matter halo in a cosmological simulation of flat ΛCDM cosmology(Ωm = 1 − ΩΛ = 0.3, h = 0.7, σ8 = 0.9). The panels show an evolutionary sequence at nine redshifts (from left toright and from top to bottom) focusing on the most massive progenitor of the main halo at each epoch (redshift ofeach epoch is shown in the left upper corner). The rendering shows the dark matter particles with intensity indicatingthe local matter density on a logarithmic stretch. The build-up of the halo proceeds through a series of spectacularmergers, particularly frequent in the early stages of evolution. Many of the merging clumps survive until the presentepoch ( = 0) in the form of ”substructure”. The size of the region shown is about 3 comoving Mpc at = 15,monotonically zooming in to a scale of ≈ 1 comoving Mpc across at = 0.

is a visual manifestation of approximate self-similarity of CDM halos of different mass. Ifwe would compare similar images of distribu-tion of luminous matter around galaxies andclusters, the difference would be striking.

The manifestly different observed satellite

populations around galaxies of different lu-minosities and expected approximately self-similar populations of satellite subhalos aroundhalos of different mass is known as the sub-structure problem. [19, 20, 16]. In the case ofthe best studied satellite systems of the Milky

2

Thursday, October 8, 2009

Page 4: Dark Matter Substructure and Dwarf Galactic Satellites

Via Lactea Movies can be found at the following url

• http://www.ucolick.org/%7Ediemand/vl/movies.html

Thursday, October 8, 2009

Page 5: Dark Matter Substructure and Dwarf Galactic Satellites

Luminous Satellite Galaxies

Thursday, October 8, 2009

Page 6: Dark Matter Substructure and Dwarf Galactic Satellites

Circular Velocity and Slopes

m0.6

Thursday, October 8, 2009

Page 7: Dark Matter Substructure and Dwarf Galactic Satellites

Defining the “Substructure Problem”

“The substructure problem can be stated as the discrepancy in the slopes of the circular velocity and mass functions inferred for observed satellites of the Milky Way and the slopes of these functions predicted for dark matter subhalos in the MW-sized host halos formed in the concordance cosmology”

m0.6

ΛCDM

Thursday, October 8, 2009

Page 8: Dark Matter Substructure and Dwarf Galactic Satellites

Different Cosmology

• Suppressing density fluctuations

• Warm Dark Matter

Thursday, October 8, 2009

Page 9: Dark Matter Substructure and Dwarf Galactic Satellites

Galaxy Formation Subhalo Suppression

• Gas photoevaporated after reionization

• Supernovae Feedback

• Satellites could be in larger halos

Thursday, October 8, 2009

Page 10: Dark Matter Substructure and Dwarf Galactic Satellites

Conclusions

• Models and Observation do not agree

• Satellites could be mostly dark

• If satellites are dark, need low star forming efficiency

• Mass-dependent suppression mechanism

Thursday, October 8, 2009

Page 11: Dark Matter Substructure and Dwarf Galactic Satellites

Luminous Satellite Models

• Threshold Galaxy Formation

• Selective Galaxy Formation

Thursday, October 8, 2009

Page 12: Dark Matter Substructure and Dwarf Galactic Satellites

Subhalo Populations

Vmax = max(

Gm(<r)r

)1/2

m(< r) = 4π∫

ρ(r)r2dr

Thursday, October 8, 2009

Page 13: Dark Matter Substructure and Dwarf Galactic Satellites

Luminous Satellites (Cont.)

Thursday, October 8, 2009