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Current-Phase Relation of a Bose-Einstein Condensate Flowing Through a Weak Link

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arxiv 0912.3209 v1 pith:F4XBUZCG submitted 2009-12-16 cond-mat.quant-gas quant-ph

Current-Phase Relation of a Bose-Einstein Condensate Flowing Through a Weak Link

classification cond-mat.quant-gas quant-ph
keywords current-phaserelationbarrierbarriersdeltabose-einsteincondensatedifference
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We study the current-phase relation of a Bose-Einstein condensate flowing through a repulsive square barrier by solving analytically the one dimensional Gross-Pitaevskii equation. The barrier height and width fix the current-phase relation $j(\delta\phi)$, which tends to $j\sim\cos(\delta\phi/2)$ for weak barriers and to the Josephson sinusoidal relation $j\sim\sin(\delta\phi)$ for strong barriers. Between these two limits, the current-phase relation depends on the barrier width. In particular, for wide enough barriers, we observe two families of multivalued current-phase relations. Diagrams belonging to the first family, already known in the literature, can have two different positive values of the current at the same phase difference. The second family, new to our knowledge, can instead allow for three different positive currents still corresponding to the same phase difference. Finally, we show that the multivalued behavior arises from the competition between hydrodynamic and nonlinear-dispersive components of the flow, the latter due to the presence of a soliton inside the barrier region.

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  1. Kibble-Zurek Mechanism and Current-Phase Relation in a Holographic Josephson Junction

    hep-th 2026-07 conditional novelty 5.0

    In a holographic superfluid ring quenched through its transition, the weak-link current follows J = Jmax sin(Δφ), with Jmax exponentially sensitive to junction width, depth, and final temperature.