2013
DOI: 10.1103/physreve.88.042916
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Effective equations for matter-wave gap solitons in higher-order transversal states

Abstract: We demonstrate that an important class of nonlinear stationary solutions of the three-dimensional (3D) Gross-Pitaevskii equation (GPE) exhibiting nontrivial transversal configurations can be found and characterized in terms of an effective one-dimensional (1D) model. Using a variational approach we derive effective equations of lower dimensionality for BECs in (m,n(r)) transversal states (states featuring a central vortex of charge m as well as n(r) concentric zero-density rings at every z plane) which provide… Show more

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Cited by 13 publications
(14 citation statements)
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“…Dipole modes have been previously studied in diverse 1D and 2D settings [38], including vortex dipoles created in a common plane [31][32][33]. In 3D, such dipole structures can be approximately described by assuming that a quasi-1D dark soliton is embedded into an originally symmetric 3D mode around its midplane (z = 0), as suggested in a different context in [6]. In particular, for the fundamental states (S = 0) approximated by the TFA expression (6), the respective antisymmetric solution can be easily found from equation (2), assuming that the width of the dark soliton in the z direction is much smaller than the intrinsic scale of the TFA mode, i.e., μ is large enough: For the vortex states, a similar approximation is available too, but its applicability condition does not hold around the inner hole of the vortex.…”
Section: Dipole (Antisymmetric) Modesmentioning
confidence: 99%
See 1 more Smart Citation
“…Dipole modes have been previously studied in diverse 1D and 2D settings [38], including vortex dipoles created in a common plane [31][32][33]. In 3D, such dipole structures can be approximately described by assuming that a quasi-1D dark soliton is embedded into an originally symmetric 3D mode around its midplane (z = 0), as suggested in a different context in [6]. In particular, for the fundamental states (S = 0) approximated by the TFA expression (6), the respective antisymmetric solution can be easily found from equation (2), assuming that the width of the dark soliton in the z direction is much smaller than the intrinsic scale of the TFA mode, i.e., μ is large enough: For the vortex states, a similar approximation is available too, but its applicability condition does not hold around the inner hole of the vortex.…”
Section: Dipole (Antisymmetric) Modesmentioning
confidence: 99%
“…Self-trapping of three-dimensional (3D) confined modes (solitons or, more properly, solitary waves) in optics [1][2][3], Bose-Einstein condensates (BECs) [4][5][6], ferromagnetic media [7], superconductors [8], semiconductors [9], baryonic matter [10], and general field theory [11,12] is a fundamental problem of nonlinear physics. An apparent condition is that an attractive, or self-focusing, nonlinearity is necessary for the creation of localized states; however, the attractive cubic nonlinearity simultaneously gives rise to collapse [13] of localized modes in higher-dimensional settings and, additionally, to strong azimuthal modulational instability of states with intrinsic vorticity [14], thus making the search for stable 3D fundamental and topological solitons in materials with the cubic (Kerr) nonlinearity a challenging issue.…”
Section: Introductionmentioning
confidence: 99%
“…Gap solitons with (m, n r ) = (0, 0) have been rarely considered in the literature [57,58]. They feature a nontrivial radial topology and require a more elaborate treatment [58]. The inset in Fig.…”
Section: Gap Soliton Familiesmentioning
confidence: 99%
“…In spite of the fact that there have been an intensive research about vortices and solitons in scalar BECs, as far as we know, the study of topological structures showing junctions between them has not been performed. Only a particular configuration of this type has been addressed in the context of an effective low-dimensional model in trapped condensates [17]. Note that in a trapped BEC without dark solitons stable vortex lines which do not form loops have to end at the condensate boundary.…”
Section: Introductionmentioning
confidence: 99%