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Thermal Inflation and the Moduli Problem

6 Pith papers cite this work. Polarity classification is still indexing.

6 Pith papers citing it
abstract

In supersymmetric theories a field can develop a vacuum expectation value $M \gg 10^3\,{\rm GeV}$, even though its mass $m$ is of order $10^2$ to $10^3\,{\rm GeV}$. The finite temperature in the early Universe can hold such a field at zero, corresponding to a false vacuum with energy density $ V_0 \sim m^2 M^2 $. When the temperature falls below $V_0^{1/4}$, the thermal energy density becomes negligible and an era of thermal inflation begins. It ends when the field rolls away from zero at a temperature of order $m$, corresponding to of order 10 $e$-folds of inflation which does not affect the density perturbation generated during ordinary inflation. Thermal inflation can solve the Polonyi/moduli problem if $M$ is within one or two orders of magnitude of $10^{12}\,{\rm GeV}$.

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2026 5 2024 1

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representative citing papers

WIMP-like Dark Matter Without Thermalization At Freeze-Out

hep-ph · 2026-05-19 · unverdicted · novelty 7.0

Hidden-sector dark matter achieves standard thermal relic abundance via early decoupling with temperature-matched freeze-out, enabling WIMP-like cross sections without late-time thermalization.

Kaon Portal to Freeze-in Dark Matter

hep-ph · 2026-05-07 · unverdicted · novelty 7.0

Freeze-in dark matter produced by kaons in low-reheating cosmologies requires larger couplings at lower reheating temperatures, directly linking the relic density to observable rates in rare kaon decay experiments.

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