4.6 Article

Many body density of states of a system of non interacting spinless fermions

Journal

NEW JOURNAL OF PHYSICS
Volume 25, Issue 6, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.1088/1367-2630/acd8e5

Keywords

density of states; spinless fermions; quantum many body systems; many body density of states

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In this work, a new approach is introduced to evaluate the many-body density of states (MBDoS) in the general case of non-interacting systems of identical quantum particles. The method utilizes the principal component analysis of a filling matrix to expand the many-body spectrum as a weighted sum of singular vectors of the filling matrix. The weighting coefficients only involve renormalized energies obtained from the single body spectrum. The effectiveness of this method is demonstrated in two classes of problems.
The modeling of out-of-equilibrium many-body quantum systems requires to go beyond low-energy physics and single or few bodies densities of states. Many-body localization, presence or lack of thermalization and quantum chaos are examples of phenomena in which states at different energy scales, including highly excited ones, contribute to dynamics and therefore affect the system's properties. Quantifying these contributions requires the many-body density of states (MBDoS), a function whose calculation becomes challenging even for non-interacting identical particles due to the difficulty to enumerate accessible states while enforcing the exchange symmetry. In the present work, we introduce a new approach to evaluate the MBDoS in the general case of non-interacting systems of identical quantum particles. The starting point of our method is the principal component analysis of a filling matrix F describing how N particles can be distributed into L single-particle energy levels. We show that the many body spectrum can be expanded as a weighted sum of singular vectors of the filling matrix. The weighting coefficients only involve renormalized energies obtained from the single body spectrum. We illustrate our method in two classes of problems that are mapped into spinless fermions : (i) non-interacting electrons in a homogeneous tight-binding model in 1D and 2D, and (ii) interacting spins in a chain under a transverse field.

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