2010
DOI: 10.1063/1.3501027
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A Schwinger disentangling theorem

Abstract: Baker–Campbell–Hausdorff formulas are exceedingly useful for disentangling operators so that they may be more easily evaluated on particular states. We present such a disentangling theorem for general bilinear and linear combinations of multiple boson creation and annihilation operators. This work generalizes a classical result of Schwinger.

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Cited by 4 publications
(7 citation statements)
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“…The following lemma is similar to the commutation relations for bilinear functions of annihilation and creation operators (see, for example, [26,Appendix B] and [45,Lemma 4.2]), whose exponentials are considered in Schwinger's theorems [8].…”
Section: A Commutator For Quadratic Forms Of Quantum Variables Satisfmentioning
confidence: 99%
See 1 more Smart Citation
“…The following lemma is similar to the commutation relations for bilinear functions of annihilation and creation operators (see, for example, [26,Appendix B] and [45,Lemma 4.2]), whose exponentials are considered in Schwinger's theorems [8].…”
Section: A Commutator For Quadratic Forms Of Quantum Variables Satisfmentioning
confidence: 99%
“…There is an analogy between (C6) (and its application to (C9)) and the factorizations in [8,Eqs. (5), (6)].…”
Section: A Commutator For Quadratic Forms Of Quantum Variables Satisfmentioning
confidence: 99%
“…Lemma 1 Suppose the OQHO, governed by the linear QSDE (9), is driven by the input fields in the vacuum state. Then the QCF Φ for the system variables in (26) satisfies a linear functional equation…”
Section: Linear Quantum Stochastic Systemsmentioning
confidence: 99%
“…which gives rise to the field-related term 2Θ M T JM = − 1 2 BJB T Θ −1 in the matrix A in (13). The other part i[H, X] = 2Θ RX of the drift vector AX in the QSDE (9) comes from the quadratic nature of the Hamiltonian H in (8) in combination with the CCRs (5) and describes the internal dynamics of the system variables which they would have if the system were isolated from the environment. Also, the representation of the dispersion matrix B = −i[X, L T ] of the QSDE (9) in (13) follows from the linear dependence of the coupling operators in (8) on the system variables and the CCRs (5).…”
Section: Linear Quantum Stochastic Systemsmentioning
confidence: 99%
See 1 more Smart Citation