2015
DOI: 10.1088/1674-1056/24/6/064204
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Algebraic and group treatments to nonlinear displaced number states and their nonclassicality features: A new approach

Abstract: Recently, nonlinear displaced number states (NDNSs) have been manually introduced, in which the deformation function f (n) has been artificially added to the well-known displaced number states (DNSs). In this paper, after expressing enough physical motivation of our procedure, four distinct classes of NDNSs are presented by applying algebraic and group treatments. To achieve this purpose, by considering the DNSs and recalling the nonlinear coherent states formalism, the NDNSs are logically defined through an a… Show more

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Cited by 4 publications
(2 citation statements)
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“…In the latter relation, the Baker-Campbell-Hausdorff (BCH) formula, applied for disentangling the bosonic operators in relation 5, has generally no application because of the complicated commutation relation [̂,̂ †] ≠ 1, unlike the relation [â,â † ] = 1 for standard bosonic operators. This challenge is overcome by considering two new auxiliary operators as [49,50] ℬ =â…”
Section: States Of Interestmentioning
confidence: 99%
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“…In the latter relation, the Baker-Campbell-Hausdorff (BCH) formula, applied for disentangling the bosonic operators in relation 5, has generally no application because of the complicated commutation relation [̂,̂ †] ≠ 1, unlike the relation [â,â † ] = 1 for standard bosonic operators. This challenge is overcome by considering two new auxiliary operators as [49,50] ℬ =â…”
Section: States Of Interestmentioning
confidence: 99%
“…In the latter relation, the Baker–Campbell–Hausdorff (BCH) formula, applied for disentangling the bosonic operators in relation (5), has generally no application because of the complicated commutation relation [scriptÂ,trueÂ]1, unlike the relation [â,trueâ]=1 for standard bosonic operators. This challenge is overcome by considering two new auxiliary operators as [ 49,50 ] truerighttrueB̂=trueâ1scriptFfalse(truen̂false),14.22636ptscriptB̂=1scriptFfalse(truen̂false)âAs a result, the two classes of generalized displacement operators can be introduced. Thus, the two sets of generators as {scriptÂ,trueB̂,trueB̂scriptÂ,Î} and {scriptB̂,trueÂ,trueÂscriptB̂,Î} can be established both satisfying the Weyl–Heisenberg Lie algebra, especially the following commutation relations truerighttrueÂ,scriptB̂trueÂ=lefttrueÂ,28.45274pt[]trueB̂,trueB̂scriptÂ=scriptB̂...…”
Section: States Of Interestmentioning
confidence: 99%