Massive stochastic Schwinger production in de Sitter
Determine the full massive de Sitter noise kernel and characterize its relation to the non-perturbative constant-field Schwinger result, including the dependence on the fermion mass, spacetime curvature, and the ratio of the mass to the Hubble scale.
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For $m\neq0$, however, the comparison is less direct. Already in flat spacetime the quadratic kernel develops the pair-production threshold $\sqrt{-K2}\ \geq\ 2m$, while in de Sitter the corresponding massive stochastic kernel is considerably more involved: massive QED is not conformally invariant, the fermion modes are no longer plane waves, and the kernel acquires genuine dependence on $m/H$ and on the spacetime curvature. Consequently, the simple massless comparison between the soft stochastic limit and the constant-field result does not carry over in any straightforward way. A proper comparison therefore requires the full massive de Sitter noise kernel, which we do not compute here. We leave the detailed analysis of the massive stochastic regime and its relation to the non-perturbative constant-field Schwinger result for future work.