For a class of polaron-type models, the energy-momentum relation is bounded below by the vacuum overlap and spectral gap, the effective mass equals the inverse limiting variance of the path measure, and vanishing variance characterizes absence of ground states at large momentum.
Effective Mass of the Fr\"ohlich Polaron and the Landau-Pekar-Spohn Conjecture
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abstract
We prove that there is a constant $\overline C\in (0,\infty)$ such that the effective mass $m(\alpha)$ of the Fr\"ohlich Polaron satisfies $m(\alpha) \geq \overline C \alpha^4$, which is sharp according to a long-standing prediction of Landau-Pekar [19] from 1948 and of Spohn [36] from 1987. The method of proof, which demonstrates how the sharp quartic divergence rate of $m(\alpha)$ appears in a natural way, is based on analyzing the Gaussian representation of the Polaron measure and that of the associated tilted Poisson point process developed in [26]. Additionally, our technique here leads to accompanying results including, 1) an explicit identification of local interval process from [26] in the strong coupling limit in terms of functionals of the Pekar process [27], 2) strict monotonicity of the effective mass $m(\alpha)$ for all $\alpha>0$ and 3) the quartic divergence of $m(\alpha)$ for a generalized class of Polaron type interactions.
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Lower bound on the energy-momentum relation of the polaron
For a class of polaron-type models, the energy-momentum relation is bounded below by the vacuum overlap and spectral gap, the effective mass equals the inverse limiting variance of the path measure, and vanishing variance characterizes absence of ground states at large momentum.