Dark Forces in the Visible Sector

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Aug 10, 2010 ... Dark Forces in the Visible Sector. ▫ ... Remedies by modifications in the Dark Sector physics. ▫ ... Only 2 dwarfs are observed in the void ...
Dark Forces in the Visible Sector



Great success of the standard cosmological model (LCDM)



Problems in the standard model



Remedies by modifications in the Dark Sector physics



Galactic Ghost Streams



Predictions

Tuesday, August 10, 2010

Collaborators: Ariel Keselman Jim Peebles

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Tuesday, August 10, 2010

What is the history of structure formation?

Tuesday, August 10, 2010

High Precision Cosmology

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Gravity of Dark matter is the driver of structure formation

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The Great Success of LCDM

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CMB Temperature fluctuations

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Tuesday, August 10, 2010

Tuesday, August 10, 2010

The Local Void

Only 2 dwarfs are observed in the void opposed to 15 expected in LCDM Tuesday, August 10, 2010

red=SDSS blue=HIPASS black=Karachentsev etal

Peebles & Nusser, 2010, Nature

The LV phenomenon seems to be part of a bigger problem:

Tuesday, August 10, 2010

i.e. the last 8Gyr

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Merging in Simulation

Figure 3:

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Credit Jie Wang

How do we know how much merging there is in the Universe?

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Stellar streams in the Milky Way

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Kinematics of stars a few kpc above the midplane of the disk:

if LCDM

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probably not LCDM Tuesday, August 10, 2010

Tuesday, August 10, 2010

About half of the brightest 20 galaxies with 8Mpc are pure disks just like the MW (Fisher & Kormendy 08)

Pure disk NGC4247

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Andromeda

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Therefore: There is an ``imbalance” between standard LCDM and observations on small scales.

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Partial Remedy

Increase the clustering rate on small scales!

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How do we do that?

WARNING: ONLY BETWEEN DARK MATTER PARTICLES!!!! The Baryons do not feel the extra term Tuesday, August 10, 2010

Violation of the Equivalence Principle

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Violation of the Equivalence Principle

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Violation of the Equivalence Principle

If B and E contain DM

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Acronym ReBEL=daRk Breaking Equivalence principLe

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Tuesday, August 10, 2010

Lorentz factor factor

kinetic term of the field

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relativistic Lagrangian of a particle

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History of scalar interactions (slide from J. Peebles):

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Lets simulate ReBEL

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ReBEL

LCDM

ReBEL

LCDM

Keselman, AN & Peebles 2010 Tuesday, August 10, 2010

LCDM

LCDM+LRSI

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AN, Gubser & Peebles 05

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Baryonic Fraction as a function of mass

McGaugh et. al. 09

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Baryonic Fraction as a function of mass from simulations

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Dynamics of Galactic satellites A test for ReBEL

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The Sagittarius dwarf/stream k

dis

15kpc

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Dynamics of infalling satellite halos/galaxies

Two important processes: a.

dynamical friction

b.

tidal stripping

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Dynamical friction (Chandrasekhar 44)

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Dynamical friction (Chandrasekhar 44)

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A very very side note: Time scale for orbit decay by DF: Time scale for Bondi growth of BH:

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V^3/(G^2 M rho) V^3/(G^2 Mbh rho)

Tidal Stripping Infalling small halo

R

BIG HALO Tuesday, August 10, 2010

Tidal Stripping Infalling small halo

R

BIG HALO Tuesday, August 10, 2010

Gravity alone

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Frieman & Gradwohl 93 and Kesden & Kamionkowski 2006 test

Galactic tidal streams are not symmetric when a ReBEL force is added! KK put a limit: beta