1974
DOI: 10.1088/0305-4470/7/2/012
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Motions in a Bose condensate. III. The structure and effective masses of charged and uncharged impurities

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Cited by 27 publications
(31 citation statements)
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“…21) and(5.24), we obtain that R h , R Ψ → 0 as W X 1 ,Q → 0. Consequently Dh cu (W 0 ) = H (W 0 ) and DΨ(t ,W 0 ) = Ψ 1 (t ,W 0 ).…”
mentioning
confidence: 78%
“…21) and(5.24), we obtain that R h , R Ψ → 0 as W X 1 ,Q → 0. Consequently Dh cu (W 0 ) = H (W 0 ) and DΨ(t ,W 0 ) = Ψ 1 (t ,W 0 ).…”
mentioning
confidence: 78%
“…However, they allow us to track the universal mechanical aspects of the vortex-matter interaction, taking place in idealized quantum mixtures. Similar models were used in the past to understand qualitatively the behavior of electron bubbles in liquid helium [22,24]. Various extensions can be incorporated into the formalism, if necessary, to investigate the effects caused by the nonlocal interactions of particles and finite temperatures.…”
Section: Theorymentioning
confidence: 99%
“…In a series of papers (see, e.g., [GR74], [JR82], [JPR86], [BaMa88], [BGMP89], [PR91], [PN93], [KR95a], [KR95b]), particular attention has been paid to a special class of solutions of (1.1), namely the traveling waves. These are solutions of the form Φ(x, t) = ψ(x − cty), where y ∈ S N −1 is the direction of propagation and c ∈ R * is the speed of the traveling wave.…”
Section: Using the Madelung Transformation φ(X T) = ρ(X T)ementioning
confidence: 99%
“…(1.1) is an extremely active research field at the moment. This equation, with the considered non-zero conditions at infinity, is relevant in a large variety of physical problems such as superconductivity, superfluidity in Helium II, phase transitions and Bose-Einstein condensates ( [BGMP89], [BaMa88], [Be08], [Co98], [GR74], [Gro63], [IoSm78], [JR82], [JPR86]). In nonlinear optics, it appears in the context of dark solitons, that is, localized waves which exist on a stable continuous background ([KiLD98], [KPS95]).…”
Section: Introductionmentioning
confidence: 99%