Average-fluctuation separation in energy levels in many-particle quantum systems with $k$-body interactions using $q$-Hermite polynomials

Abstract

Separation between average and fluctuation parts in the state density in many-particle quantum systems with $k$-body interactions, modeled by the $k$-body embedded Gaussian orthogonal random matrices (EGOE($k$)), is demonstrated using the method of normal mode decomposition of the spectra and also verified through power spectrum analysis, for both fermions and bosons. The smoothed state density is represented by the $q$-normal distribution ($f_{qN}$) (with corrections) which is the weight function for $q$-Hermite polynomials. As the rank of interaction $k$ increases, the fluctuations set in with smaller order of corrections in the smooth state density. They are found to be of GOE type, for all $k$ values, for both fermion and boson systems.

arXiv comment25 pages, 8 figures

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Cited by in corpus (3)

• Two species $k$-body embedded Gaussian unitary ensembles: $q$-normal form of the eigenvalue density
• Thermalization in many-fermion quantum systems with one- plus random $k$-body interactions
• Bivariate moments of the two-point correlation function for embedded Gaussian unitary ensemble with $k$-body interactions