2000
DOI: 10.1016/s0301-0104(00)00258-5
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An extended SU(2) model for coupled Morse oscillators

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Cited by 64 publications
(82 citation statements)
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“…Here b † i (b i ) with i = 1, 2 are creation and annihilation operators acting on the Morse eigenfunctions [57]. The anhar-monization (59) is equivalent to consider the linear approximation [29,30,60] …”
Section: Force Constants In the Algebraic Approachmentioning
confidence: 99%
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“…Here b † i (b i ) with i = 1, 2 are creation and annihilation operators acting on the Morse eigenfunctions [57]. The anhar-monization (59) is equivalent to consider the linear approximation [29,30,60] …”
Section: Force Constants In the Algebraic Approachmentioning
confidence: 99%
“…The exact connection of the U (2) model with the Morse and Pöschl-Teller potentials was established in Refs. [29,30,33]. This connection opened up the possibility of obtaining force constants from the optimized values of Hamiltonian parameters [31,32,40].…”
Section: Introductionmentioning
confidence: 98%
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“…For simplicity, we have assumed that the system is one dimensional (x and E point in the same direction) and neglected the transverse nature of the electromagnetic field and any magnetic effects. By identifying the number states |n with the Morse eigenfunctions φ n (x) and comparing the matrix elements [13] φ n+α |x|φ n and φ n+α |p|φ n of the position x and the momentum p operators with those of the deformed boson operators n + α|(A † ) α |n and n − α|A α |n we may obtain expressions for x and p in terms ofn, A and A † ,…”
Section: Interaction With a Driving Fieldmentioning
confidence: 99%
“…The coefficients f ij , g ij , are functions of the excitation number operatorn and are given by [13] …”
Section: Interaction With a Driving Fieldmentioning
confidence: 99%