1992
DOI: 10.1080/09500349214552231
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Ultrashort Optical Pulse Propagation in Nonlinear Non-resonance Medium

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Cited by 30 publications
(15 citation statements)
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“…The continuing experimental progress in the study of the wave dynamics of FCPs in nonlinear optical media has paved the way for the development of new theoretical approaches to model their propagation in physical systems. Three classes of main dynamical models for FCPs have been put forward: (i) the quantum approach [48][49][50][51][52], (ii) the refinements within the framework of SVEA of the nonlinear Schrödinger-type envelope equations [53][54][55][56][57][58][59][60][61][62][63], and the non-SVEA models [64][65][66][67][68][69][70][70][71][72][73][74][75][76][77][78][79][80][81][82]. Extremely short pulses can be described by solving directly the Maxwell-Bloch equations for a two-level system.…”
Section: Introductionmentioning
confidence: 99%
“…The continuing experimental progress in the study of the wave dynamics of FCPs in nonlinear optical media has paved the way for the development of new theoretical approaches to model their propagation in physical systems. Three classes of main dynamical models for FCPs have been put forward: (i) the quantum approach [48][49][50][51][52], (ii) the refinements within the framework of SVEA of the nonlinear Schrödinger-type envelope equations [53][54][55][56][57][58][59][60][61][62][63], and the non-SVEA models [64][65][66][67][68][69][70][70][71][72][73][74][75][76][77][78][79][80][81][82]. Extremely short pulses can be described by solving directly the Maxwell-Bloch equations for a two-level system.…”
Section: Introductionmentioning
confidence: 99%
“…In parallel to the fast experimental progress in the study of the formation of few-cycle pulses (FCPs) in nonlinear optical media new theoretical approaches to model their propagation in a lot of physical settings were developed. It is to be noticed that three classes of main dynamical models for FCPs have been put forward in the past years: (i) the quantum approach [9][10][11][12], (ii) the refinements within the framework of slowly varying envelope approximation (SVEA) of the nonlinear Schrödinger-type envelope equations [13][14][15][16][17][18][19][20], and the non-SVEA models [21][22][23][24][25][26][27][28][29][30][31][32][33][34][35]. It was therefore found in these earlier studies that the propagation of FCPs in Kerr-type nonlinear optical media can be described beyond the SVEA by using the modified Korteweg-de Vries (mKdV) [27,28], sine-Gordon (sG) [29,30], or mKdV-sG equations [31][32][33].…”
Section: Introductionmentioning
confidence: 99%
“…In particular, the propagation of a linearly polarized USP was considered in Refs. [2,12] in the framework of the material model based on the Duffing oscillators, the nonlinear response of the medium being cubic. The propagation of a linearly polarized USP in a dispersive medium was modeled by means of quadratically nonlinear oscillators in Ref.…”
Section: Introductionmentioning
confidence: 99%