4 problems

Let $H(\alpha)$ be the Fröhlich polaron Hamiltonian, and let $M(\alpha)$ denote the effective mass of the particle–field system, defined as the inverse of the second derivative at…

Strong-coupling effective mass conjecture. The effective mass satisfies

Quantum correction conjecture. The same formula should hold when $\Omega=\mathbb{R}^3$ as $\alpha\to\infty$.

Pekar's conjecture.