2000
DOI: 10.1238/physica.topical.084a00081
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Cross Phase Modulation Induced Pulse Splitting ? the Optical Axe

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Cited by 9 publications
(12 citation statements)
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“…These propagate without dispersion [6], are robust to collisions with other bright solitary matter-waves and with slowly varying external potentials [7,8], and have center-of-mass trajectories welldescribed by effective particle models [9][10][11]. Such solitonlike properties are due to the mean-field description of an atomic BEC reducing to the nonlinear Schrödinger equation in a homogeneous, quasi-one-dimensional (quasi-1D) limit, which for the case of attractive interactions supports the bright soliton solutions well-known in the context of nonlinear optics [12][13][14][15][16]. The quasi-1D limit is experimentally challenging for attractive condensates [17], but solitary wave dynamics remain highly soliton-like outside this limit [3,8].…”
mentioning
confidence: 60%
“…These propagate without dispersion [6], are robust to collisions with other bright solitary matter-waves and with slowly varying external potentials [7,8], and have center-of-mass trajectories welldescribed by effective particle models [9][10][11]. Such solitonlike properties are due to the mean-field description of an atomic BEC reducing to the nonlinear Schrödinger equation in a homogeneous, quasi-one-dimensional (quasi-1D) limit, which for the case of attractive interactions supports the bright soliton solutions well-known in the context of nonlinear optics [12][13][14][15][16]. The quasi-1D limit is experimentally challenging for attractive condensates [17], but solitary wave dynamics remain highly soliton-like outside this limit [3,8].…”
mentioning
confidence: 60%
“…These excitations are soliton-like in the sense that they propagate without dispersion [6], are robust to collisions with both other bright solitary matter-waves and slowly varying external potentials [7,8], and have center-of-mass trajectories which are well-described by effective particle models [9][10][11]. They derive these soliton-like properties from their analogousness to the bright soliton solutions of the focusing nonlinear Schrödinger equation (NLSE) [12][13][14][15][16], to which the mean-field description of an atomic BEC reduces in an effectively unconfined, quasi-one-dimensional (quasi-1D) limit. Although the quasi-1D limit is experimentally challenging for attractive condensates [17], bright solitary matterwave dynamics remain highly soliton-like outside this limit [3,8].…”
Section: Introductionmentioning
confidence: 99%
“…This is equivalent, in the continuum limit of an infinite number of waveguides, to splitting a soliton in the Gross-Pitaevskii equation (GPE) at a δ-function potential barrier [36]. In the optics community this phenomenon has been called the "optical axe" [16]. Incomplete/bound state splitting has been considered in the context of soliton molecule formation [22], within a mean-field de-scription, and also in the context of many-body quantum mechanical descriptions: in the latter it has been demonstrated that macroscopic quantum superpositions of solitary waves could be created, offering intriguing possibilities for future atom interferometry experiments [20,21].…”
Section: Introductionmentioning
confidence: 99%
“…They derive these solitonlike properties from their analogousness to the bright soliton solutions of the focusing nonlinear Schrödinger equation (NLSE), to which the mean-field description of an atomic BEC reduces in a homogeneous, quasione-dimensional (quasi-1D) limit. These bright soliton solutions of the 1D focusing NLSE have been extensively explored in nonlinear optics, both in the context of solitons in optical fibers [10][11][12][13][14] and as stable structures existing in arrays of coupled waveguides [15,16] which are described by a discretized NLSE. Although the quasi-1D limit is experimentally challenging for attractive condensates [17], bright solitary matter-wave dynamics remain highly solitonlike outside this limit [3,6].…”
Section: Introductionmentioning
confidence: 99%
“…When, in nonlinear optics, the soliton exists in an inhomogeneous array of discrete waveguides, the soliton can be reflected, split or captured at the position of the inhomogeneity [29][30][31]. This is equivalent, in the continuum limit of an infinite number of waveguides, to splitting a soliton in the GPE at a δ-function [29] -a phenomenon which has been called the "optical axe" [14]. Such splitting has been considered in the context of soliton molecule formation [21], within a mean-field description, and also in the context of many-body quantum mechanical descriptions: in the latter it has been demonstrated that macroscopic quantum superpositions of solitary waves could be created, offering intriguing possibilities for future atom interferometry experiments [19,20].…”
Section: Introductionmentioning
confidence: 99%