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Nuclear Physics A

A new representation for the density matrix

G. Ramachandran, M. V. N. Murthy

Published Mar 1, 1980• 16 citations
Publisher
DOI
10.1016/0375-9474(80)90058-5

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In this paper, a new representation of the Wigner function for a quantum system in the phase space is proposed. The new representation is of the form W=Sp⁡[ρW]W=\operatorname{Sp}\left[ ρ\mathcal{W} \right]W=Sp[ρW], where ρρρ is the density matrix, and W\mathcal{W}W is the universal density matrix. The density matrix ρρρ for each quantum system is different, and the universal matrix W\mathcal{W}W is the same for any quantum system. Thus, the matrix W\mathcal{W}W has a fundamental character. In the work, the elements of the universal matrix W\mathcal{W}W were found explicitly and their properties were investigated. The diagonal elements of the matrix W\mathcal{W}W are the Wigner functions of the harmonic oscillator, which do not introduce dissipation into the quantum system. The off-diagonal elements of the matrix W\mathcal{W}W contain frequency oscillations responsible for dissipations in the quantum systems.
The NNN-representability problem for the first- and second-order density matrices is considered when NNN is an odd integer. Attention is restricted to those density matrices derivable from functions whose natural spin orbitals have certain paired properties. Neither pairing of spatial orbitals nor special spin properties are required in general, but they are discussed as special cases. New sufficient conditions for NNN-representability of the first-order density matrix are given. The second-order density matrix is studied in detail. Special cases in which the NNN-representability problem for the second-order density matrix can be solved are considered.