A natural solution to the gravitino overabundance problem

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A natural solution to the gravitino overabundance problem Based on the work : R symmetry and gravitino abundance, I. Dalianis, Phys. Rev. D 85 061130(R) (2012) Ioannis Dalianis National Technical University of Athens Corfu Summer School 20/9/2012

Outline Supersymmetry breaking sectors generically have a global U(1) R symmetry, exact or approximate R Symmetry must be broken in order for Majorana gaugino masses to be generated However, R Symmetry can be restored at finite temperature R Symmetry restoration implies suppressed gaugino masses hence, a suppressed generation rate of gravitinos from the heat bath We derive a new formula for the relic abundance of gravitinos produced by scattering in the thermal plasma that does not depend on the reheating temperature I. Dalianis- Corfu 2012 2

FrameWork The discovery of a SM-like Higgs supports the ElectroWeak scale Supersymmetry (susy) Local Susy theories predict the existence of the gravitino The Early Universe was in thermal equilibrium A Supersymmetric Universe means that the thermal bath contains the Standard Model and their Supersymmetric Partners I. Dalianis- Corfu 2012 3

SUPERSYMMERY (SUSY) BREAKING I. Dalianis- Corfu 2012 4

Stable Gravitino Relic Abundance Scatterings in the thermal plasma and decays of thermalized particles Scatterings, the dominant contribution: Non thermal decays (Model Dependent) Thermalized gravitinos (?) I. Dalianis- Corfu 2012 5

Thermal Production of Gravitinos the textbook formula: The gravitino abundance is essentially linear in the reheating temperature: Ellis, Kim, Nanopoulos, Phys.Lett.B (1984) Morroi, Murayama, Yamaguchi, Phys.Lett.B (1993) Bolz, Brandenburg, Buchmueller, Nucl.Phys.B (2001) Pradler, Steffen, Phys. Rev. D (2007) Rychkov, Strumia, Phys. Rev. D (2007) I. Dalianis- Corfu 2012 6

A Dynamic Mass Spectrum, Symmetries, Heat Bath The susy breaking sector is dynamic. The standard paradigm of gauge mediation: Sparticle Masses: Gauginos: R-Charged Spurion Charged Messengers Sfermions: I. Dalianis- Corfu 2012 7

R Symmetry In the Thermalized The U(1)-R symmetry can be restored at high temperatures The characteristic temperature of the R-phase transition I.Dalianis and Z.Lalak, JHEP (2010) 045 Universe The VEV tends to the zero -> R-Symmetry restoration! I. Dalianis- Corfu 2012 8

The Regulative Role of the R Symmetry We define the R-breaking parameter: The expected suppression of the gaugino masses: The cross section is modulated: I. Dalianis- Corfu 2012 9

(New) Light Gravitino Abundance from Scatterings in the Thermal Plasma I. Dalianis, Phys. Rev. D 85 061130(R) (2012) After computing the yield We find the gravitino abundance: where I. Dalianis- Corfu 2012 10

(New) Light Gravitino Abundance from Scatterings in the Thermal Plasma I. Dalianis, Phys. Rev. D 85 061130(R) (2012) After computing the yield We find the gravitino abundance: Substituting I. Dalianis- Corfu 2012 11

Gravitino Abundance VS Reheating Temperature I. Dalianis- Corfu 2012 12

Implications The reheating temperature constraints are relaxed several orders of magnitude. No contradiction with thermal Leptogenesis The gravitino production depends essentially on the hidden sector and not on the MSSM parameters The gravitino abundance gives us a direct insight into the hidden sector and the dynamics of susy breaking (interplay with data from colliders) If the (conventional) freeze out temperature for the gravitinos is then the gravitinos do not equilibrate (there is no freeze out temperature) General (standard) models of gauge mediation predict the observed dark matter abundance for gravitinos I. Dalianis- Corfu 2012 13

Gravitino Dark Matter Abundance The gravitino does not overclose the universe if I. Dalianis- Corfu 2012 14

Thermally Favourable Gauge Mediation I.Dalianis and Z.Lalak, Phys. Lett. B (2011) 385 The Yukawa coupling at the messenger superpotenial: A large part of the parameter space makes the susy breaking vacuum thermally attractive I. Dalianis- Corfu 2012 15

Predicted Dark Matter Abundance The gravitino accounts for the bulk dark matter of the universe if I. Dalianis- Corfu 2012 16

Cosmology - Collider Interplay Collider data will select/exclude parts of the parameter space constrained by cosmological arguments I. Dalianis- Corfu 2012 17

Natural Dark Matter Candidates The neutralino case: I. Dalianis- Corfu 2012 18

Natural Dark Matter Candidates The neutralino case: The gravitino case: I. Dalianis- Corfu 2012 19

Gravitino: A Natural and Compelling Dark Matter Candidate The gravitino abundance: Thank you! I. Dalianis- Corfu 2012 20

Thermal Effects The potential at T=0 The potential at finite temperature I.Dalianis and Z.Lalak,JHEP (2010) 045 I. Dalianis- Corfu 2012 21

KKLT uplifted by Matter Superpotentials I. Dalianis- Corfu 2012 22