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Communications in Theoretical Physics

Two-Mode Wigner Operator in 〈ξ| Representation and 〈τ| Representation

Song Tong-Qiang, Fan Hong-Yi

Published Dec 15, 2001• 0 citations
Publisher

Abstract

We derive the two-mode Wigner operator in the 〈ξ| representation and 〈τ| representation, where |ξ〉 is the common eigenvector of the mass-weighted relative coordinate and the mass-combinatorial momentum, and |τ〉 is the common eigenvector of the mass-weighted relative coordinate and the mass-combinatorial momentum. As an application, we calculate the Wigner function of some two-mode state.

DOI
10.1088/0253-6102/36/6/695

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We derive the two-mode Wigner operator in the 〈ξ| representation and 〈τ| representation, where |ξ〉 is the common eigenvector of the mass-weighted relative coordinate and the mass-combinatorial momentum, and |τ〉 is the common eigenvector of the mass-weighted relative coordinate and the mass-combinatorial momentum. As an application, we calculate the Wigner function of some two-mode state.
We construct four linear composite operators for a two-particle system and give common eigenvectors of those operators. The technique of integration within an ordered product (IWOP) of operators is employed to prove that those common eigenvectors are complete and orthonormal. Therefore, a new two-mode intermediate momentum-coordinate representation which involves quantum entanglement for a two-particle system is proposed and applied to some two-body dynamic problems. Moreover, the pure-state density matrix |ξ 1 , ξ 2 〉 C,D C,D 〈ξ 1 , ξ 2 | is a Radon transform of Wigner operator.
The explicit form of the common eigenstates| τ ⟩ of the mass-weighted relative coordinate μ 2 Q 1 - μ 1 Q 2 and the mass-combinatorial momentum μ 1 P 1 + μ 2 P 2 of two particles is given. On the basis of| τ ⟩ and their conjugate states| ξ ⟩, we find that there exist new differential completeness relations (DCR). The applications of the new DCR in deriving the normally ordered two-mode squeezing operators for the mass-related coordinates and momenta are demonstrated. Throughout the discussion the technique of differentiation within an ordered product of operators is fully employed.
We give the explicit form of the common eigenstate \ensuremath{\Vert}\ensuremath{\xi}〉 of the center-of-mass coordinate ${\mathrm{\ensuremath{\mu}}}_{1}$Q1{\mathit{Q}}_{1}Q1​+${\mathrm{\ensuremath{\mu}}}_{2}$Q2{\mathit{Q}}_{2}Q2​ and the mass-weighted relative momentum ${\mathrm{\ensuremath{\mu}}}_{2}$P1{\mathit{P}}_{1}P1​-${\mathrm{\ensuremath{\mu}}}_{1}$P2{\mathit{P}}_{2}P2​ of two particles, which is more complicated than the common eigenstate of the other pair of commutative operators Q2{\mathit{Q}}_{2}Q2​-Q1{\mathit{Q}}_{1}Q1​ and P1{\mathit{P}}_{1}P1​+P2{\mathit{P}}_{2}P2​. The orthonormal and completeness relation of \ensuremath{\Vert}\ensuremath{\xi}〉 are investigated easily by virtue of the technique of integration within an ordered product of operators. The normally ordered squeezing operator for ${\mathrm{\ensuremath{\mu}}}_{1}$Q1{\mathit{Q}}_{1}Q1​+${\mathrm{\ensuremath{\mu}}}_{2}$Q2{\mathit{Q}}_{2}Q2​ and ${\mathrm{\ensuremath{\mu}}}_{2}$P1{\mathit{P}}_{1}P1​-${\mathrm{\ensuremath{\mu}}}_{1}$P2{\mathit{P}}_{2}P2​ is also derived by using the \ensuremath{\Vert}\ensuremath{\xi}〉 representation.