2004
DOI: 10.1007/s10773-004-7707-2
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Nonlinear Jaynes?Cummings Model of Atom?Field Interaction

Abstract: Interaction of a two-level atom with a single mode of electromagnetic field including Kerr nonlinearity for the field and intensity-dependent atom-field coupling is discussed. The Hamiltonian for the atom-field system is written in terms of the generators of a closed algebra, which has SU(1,1) and Heisenberg-Weyl algebras as limiting cases. Eigenstates and eigenvalues of the Hamiltonian are constructed. With the field being in a coherent state initially, the dynamical behavior of atomic inversion, field statis… Show more

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Cited by 40 publications
(24 citation statements)
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“…A coupling proportional to 1/(a † a) 1/2 has also been used [22] in a tripartite model, motivated by the fact that this form arises naturally in the context of diagonal-state representations of the density matrix in a restricted Hilbert space where the zero-photon state is absent [23]. An intensity-dependent coupling of the form (1+κ a † a) 1/2 , 0 ≤ κ ≤ 1 has been shown [24] to lead to a closed-form expression for the mean photon energy. Here κ = 0 reduces to the Heisenberg-Weyl algebra for the field operators, while κ = 1 leads to the SU(1, 1) algebra for (nonlinear combinations of) these operators [25].…”
Section: Introductionmentioning
confidence: 99%
“…A coupling proportional to 1/(a † a) 1/2 has also been used [22] in a tripartite model, motivated by the fact that this form arises naturally in the context of diagonal-state representations of the density matrix in a restricted Hilbert space where the zero-photon state is absent [23]. An intensity-dependent coupling of the form (1+κ a † a) 1/2 , 0 ≤ κ ≤ 1 has been shown [24] to lead to a closed-form expression for the mean photon energy. Here κ = 0 reduces to the Heisenberg-Weyl algebra for the field operators, while κ = 1 leads to the SU(1, 1) algebra for (nonlinear combinations of) these operators [25].…”
Section: Introductionmentioning
confidence: 99%
“…The commutator [K m , K † m ] = 2K 0 , with K 0 = ka † a + 1 2 , which is identity when k = 0. These deformed operators form a closed algebra, with Heisenberg-Weyl and SU(1,1) as limiting cases in k [27]. Under the action of these operators, the number states transform as follows,…”
Section: Hamiltonian For Nonlinearly Coupled Cavitiesmentioning
confidence: 99%
“…The last term containing the coupling constant J describes an intensity-dependent interaction between the two cavities. Such interaction terms have been considered in the context of intensity-dependent atom-field coupling [27].…”
Section: Hamiltonian For Nonlinearly Coupled Cavitiesmentioning
confidence: 99%
“…The JCM and its generalizations have been reported in the literature [12][13][14]; the atom-field interaction naturally leads to the entangled state. Throughout the recent five decades, the JCM has been generalized using the Kerr nonlinearity [15,16], intensity-dependent coupling [17][18][19][20], multi-photon transitions [21][22][23], and the atomic motion with the classical homogenous gravitational field [24].…”
Section: Introductionmentioning
confidence: 99%