14
Enhancement of DM relic density from the late time DM conversions Ze-Peng Liu, Yue-Liang Wu, and Yu-Feng Zhou (arXiv: 1101.4148)

Enhancement of DM relic density from the late time DM conversions

Embed Size (px)

DESCRIPTION

Enhancement of DM relic density from the late time DM conversions. Ze-Peng Liu, Yue-Liang Wu, and Yu-Feng Zhou (arXiv: 1101.4148). 2-component case. The effective cross section A interesting limit Approximate form. Themal evolution. Thermal equilibrium with SM - PowerPoint PPT Presentation

Citation preview

Page 1: Enhancement of DM relic density from the late time DM conversions

Enhancement of DM relic density from the late time

DM conversions

Ze-Peng Liu, Yue-Liang Wu, and Yu-Feng Zhou(arXiv: 1101.4148)

Page 2: Enhancement of DM relic density from the late time DM conversions

2-component case The effective cross section

A interesting limit

Approximate form

Page 3: Enhancement of DM relic density from the late time DM conversions

• Thermal equilibrium with SM

1. Decouple from SM, but still in equilibrium with each other

1. Late time DM conversion at large z2. Slow conversion characterized by r(z)

3. Crossing point

3. Complete decouple (freeze-out) after

Themal evolution

Freeze-out condition

Y1(z) increased eventually

Page 4: Enhancement of DM relic density from the late time DM conversions

Numerical Result

Equilibrium• Equilibrium density Y2

Page 5: Enhancement of DM relic density from the late time DM conversions

Numerical Result

Equilibrium• Equilibrium density Y2• Equilibrium density Y1

Page 6: Enhancement of DM relic density from the late time DM conversions

Numerical Result

Equilibrium• Equilibrium density Y2• Equilibrium density Y1If no conversion• Decoupling of Y2• Decoupling of Y1

Page 7: Enhancement of DM relic density from the late time DM conversions

Numerical Result

Equilibrium• Equilibrium density Y2• Equilibrium density Y1If no conversion• Decoupling of Y2• Decoupling of Y1With conversion• Evolution of Y2• Evolution of Y1

Page 8: Enhancement of DM relic density from the late time DM conversions

Numerical Result

Equilibrium• Equilibrium density Y2• Equilibrium density Y1If no conversion• Decoupling of Y2• Decoupling of Y1With conversion• Evolution of Y2• Evolution of Y1• Evolution of Y1+Y2

Page 9: Enhancement of DM relic density from the late time DM conversions

Conditions for a large boost factor

• Large internal degree of freedom of Y2: • Small mass difference:

• Cross sections satisfy:

Approximate expression for the boost factor

Page 10: Enhancement of DM relic density from the late time DM conversions

boost factor (B)

B vs mass difference B vs relative cross sections

Page 11: Enhancement of DM relic density from the late time DM conversions

A simple 2CDM Model

Add to the SM

Page 12: Enhancement of DM relic density from the late time DM conversions

A simple 2CDM Model

Add to the SM

mediators

Page 13: Enhancement of DM relic density from the late time DM conversions

A simple 2CDM ModelCross sections

Other processes are suppressed by p-wave.

Enhanced by the resonance

Page 14: Enhancement of DM relic density from the late time DM conversions

Summary

In multi-DM models, DM conversion can significantly modify the thermal evolution of each DM component.

The relic density of the DM component may not always inversely proportional to it’s annihilation cross section. Through conversions from heavier DM components, the relic density of light DM can be enhanced, leading to large boost factors.

The boost factor is independent of DM relative velocity. For generic models with large conversion rate the boost fact can reach the value required by PAMELA etc.