arXiv subjects
Publications and source records attributed to R. V. Romanov.
Let $μ$ be a measure on the real line $\mathbb{R}$ such that $\int_{\mathbb{R}}\frac{dμ(t)}{1+t^2} < \infty$ and let $a>0$. Assume that the norms $\|f\|_{L^2(\mathbb{R})}$ and $\|f\|_{L^2(μ)}$ are comparable for functions $f$ in the Paley-Wiener space $PW_{a}$ and that $PW_a$ is dense in $L^2(μ)$. We reconstruct the canonical Hamiltonian system $JX' = zHX$ such that $μ$ is the spectral measure for this system.
Using for unperturbed electron and phonon Hamiltonians a representation by the Jacobi matrices a one-dimensional model of the electron-phonon interaction is constructed. In frame of the model the polaron and scattering spectral bands are calculated explicitly as well as the corresponding states. An explicit formula for the polaron effective mass is derived and the fit of model parameters is suggested. A connection of the model with the description of phonon degrees of freedom for quantum wires is discussed.