Dispersion Law of the Form $ε(p)=\hbar^2p^2/2m +\widetilde V(p)-\widetilde V(0)$ for Elementary Excitations of Nonideal Fermi Gas in the Pair Interaction Approximation $(i\leftrightarrow j)$, $V(|x_i-x_j|)$

Details Dispersion Law of the Form $ε(p)=\hbar^2p^2/2m +\widetilde V(p)-\widetilde V(0)$ for Elementary Excitations of Nonideal Fermi Gas in the Pair Interaction Approximation $(i\leftrightarrow j)$, $V(|x_i-x_j|)$ Dispersion Law of the Form $ε(p)=\hbar^2p^2/2m +\widetilde V(p)-\widetilde V(0)$ for Elementary Excitations of Nonideal Fermi Gas in the Pair Interaction Approximation $(i\leftrightarrow j)$, $V(|x_i-x_j|)$

2007-10-02

arxiv.org/abs/0710.0537v2

Physics

Mathematical Physics

Latex, 21 p

Scientific paper

We give a derivation of the dispersion law $\epsilon(p)=\hbar^2p^2/2m
+\widetilde V(p)-\widetilde V(0)$, where $\widetilde V(p)$ is the Fourier
transform of the pair interaction potential $V(r)$. (The interaction between
particles $x_i$ and $x_j$ is $V(|x_i-x_j|)$.)

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