English

$\Delta N_{\text{eff}}$ and entropy production from early-decaying gravitinos

High Energy Physics - Phenomenology 2018-07-11 v1 Cosmology and Nongalactic Astrophysics High Energy Physics - Theory

Abstract

Gravitinos are a fundamental prediction of supergravity, their mass (mGm_{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 (TrhT_{\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 (μ\mu and yy) distortion eras, upcoming CMB spectral distortions bounds are highly effective in constraining the TrhmGT_{\text{rh}}-m_{G} space. For heavier gravitinos (with lifetimes shorter than a few ×106\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 (NeffN_{\text{eff}}). In this paper, we utilize the observational bounds on NeffN_{\text{eff}} to constrain gravitino decays, and hence provide new constaints on gravitinos and reheating. For gravitino masses less than 105\approx 10^5 GeV, current observations give an upper limit on the reheating scale in the range of 5×10105×1011\approx 5 \times 10^{10}- 5 \times 10^{11}GeV. For masses greater than 4×103\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.

Keywords

Cite

@article{arxiv.1706.01495,
  title  = {$\Delta N_{\text{eff}}$ and entropy production from early-decaying gravitinos},
  author = {Emanuela Dimastrogiovanni and Lawrence M. Krauss},
  journal= {arXiv preprint arXiv:1706.01495},
  year   = {2018}
}

Comments

6 pages, 1 figure