Realistic Inflation in No-Scale $U(1)_R$ Symmetric Flipped $SU(5)$

TL;DR

This paper constructs and analyzes inflationary models within a supersymmetric flipped $SU(5)$ framework with $U(1)_R$ symmetry, showing compatibility with Planck data and addressing reheating, leptogenesis, and proton decay constraints.

Contribution

It presents two inflation models in a no-scale supergravity context with $U(1)_R$ symmetry, demonstrating their viability and phenomenological consistency.

Findings

Both models agree with Planck 2018 data.

Tensor-to-scalar ratio is very small, especially in hybrid inflation.

Reheating temperatures are compatible with leptogenesis constraints.

Abstract

We have realized non-minimal Higgs inflation and standard hybrid inflation in the supersymmetric flipped $SU(5)$ model with $U(1)_R$ symmetry using the no-scale form of the K\"{a}hler potential. In non-minimal Higgs inflation the waterfall Higgs field plays the role of inflaton, and in standard hybrid inflation the gauge singlet field $S$ is employed as an inflaton. The predictions of both models are in good agreement with the Planck 2018 data. For numerical calculations we have fixed the gauge symmetry breaking scale, $M$, around $2\times 10^{16}$ GeV. In both models the inflaton field values are constrained below $m_P$. The tensor to scalar ratio $r$ in non-minimal inflation is of the order of $10^{-3}$ and for standard hybrid inflation $r$ is tiny, of order $10^{-15} - 10^{-4}$. The scalar spectral index in both cases lie within the Planck 1-$\sigma$ bounds, and the running of the scalar spectral index lies in the range, $-dn_s/d\ln k \sim 6\times 10^{-4}$ for non-minimal model and $10^{-9} - 10^{-3}$ for the standard hybrid model. A realistic scenario of reheating and non-thermal leptogenesis is employed with reheat temperature $T_r \sim 10^9$ GeV for non-minimal model and $10^{6} - 10^{10}$~GeV for standard hybrid model. The $R$-symmetry plays a vital role in forbidding rapid proton decay, but at the same time it also suppresses terms responsible for generating right handed neutrino masses. A realistic scenario of right handed neutrino masses is obtained by considering effective $R$ symmetry breaking at the nonrenormalizable level with adequate suppression of rapid proton decay.