Abstract

Gravitinos are a fundamental prediction of supergravity, their mass ($m_{G}$) is informative of the value of the SUSY breaking scale, and, if produced during reheating, their number density is a function of the reheating temperature ($T_{\text{rh}}$). As a result, constraining their parameter space provides in turn significant constraints on particles physics and cosmology. We have previously shown that for gravitinos decaying into photons or charged particles during the ($\mu$ and $y$) distortion eras, upcoming CMB spectral distortions bounds are highly effective in constraining the $T_{\text{rh}}-m_{G}$ space. For heavier gravitinos (with lifetimes shorter than a few $\times10^6$ sec), distortions are quickly thermalized and energy injections cause a temperature rise for the CMB bath. If the decay occurs after neutrino decoupling, its overall effect is a suppression of the effective number of relativistic degrees of freedom ($N_{\text{eff}}$). In this paper, we utilize the observational bounds on $N_{\text{eff}}$ to constrain gravitino decays, and hence provide new constaints on gravitinos and reheating. For gravitino masses less than $\approx 10^5$ GeV, current observations give an upper limit on the reheating scale in the range of $\approx 5 \times 10^{10}- 5 \times 10^{11}$GeV. For masses greater than $\approx 4 \times 10^3$ GeV they are more stringent than previous bounds from BBN constraints, coming from photodissociation of deuterium, by almost 2 orders of magnitude.

Highlights

  • The gravitino is predicted in supergravity as the spin 3=2 superpartner of the graviton

  • Because of the sensitivity we have demonstrated here of gravitino bounds to number of relativistic degrees of freedom (Neff), a tightening of the bounds on Neff coming from upcoming cosmic microwave background (CMB) observations should allow significantly improved parameter space restrictions for postinflation gravitino production and decay

  • Entropy transfers to the CMB bath from heavy particles, decaying after neutrino decoupling, suppress the ratio of the neutrino-to-CMB temperatures thereafter or, in other words, the effective number of relativistic species, Neff, with respect to its standard model prediction (Neff ≃ 3.046). This would be the case for unstable gravitinos decaying in the pre-distortion eras

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Summary

INTRODUCTION

The gravitino is predicted in supergravity as the spin 3=2 superpartner of the graviton (see e.g., [1] for a review). The importance of constraining the reheating temperature cannot be overstated: Trh is one of handful of macroscopic parameters describing the transition from an early phase of accelerated expansion (inflation) to the radiation-dominated era and it sets a lower bound on the energy scale of inflation (e.g., [2]) Because of their potentially large masses, gravitinos can have significant cosmological impacts [3]. This work is organized as follows: in Sec. II we briefly review results for the thermal production of gravitinos during reheating and we formally introduce the relation between ΔNeff and model parameters; in Sec. III we compute ΔNeff from gravitino decays and place constraints on the reheating temperature and gravitino mass parameter space; in Sec. IV we comment on implications for gravitinos of future constraints on Neff arising from measurements of CMB anisotropies and LSS observations

GRAVITINO DECAYS AND COSMOLOGY
ENTROPY INJECTION AND ΔNeff CONSTRAINTS
CONCLUSIONS AND OUTLOOK
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