Dynamics of spinor Bose-Einstein condensate subject to dissipation

We investigate the internal dynamics of the spinor Bose-Einstein condensates subject to dissipation by solving the Lindblad master equation. It is shown that for the condensates without dissipation its dynamics always evolve along a specific orbital in the phase space of (no, O) and display three ki...

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Bibliographic Details
Published inChinese physics B Vol. 25; no. 4; pp. 69 - 73
Main Author 庞曼曼 郝亚江
Format Journal Article
LanguageEnglish
Published 01.04.2016
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ISSN1674-1056
2058-3834
1741-4199
DOI10.1088/1674-1056/25/4/040501

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Summary:We investigate the internal dynamics of the spinor Bose-Einstein condensates subject to dissipation by solving the Lindblad master equation. It is shown that for the condensates without dissipation its dynamics always evolve along a specific orbital in the phase space of (no, O) and display three kinds of dynamical properties including Josephson-like oscil- lation, self-trapping-like oscillation, and 'running phase'. In contrast, the condensates subject to dissipation will not evolve along the specific dynamical orbital. If component-1 and component-(-1) dissipate at different rates, the magnetization m will not conserve and the system transits between different dynamical regions. The dynamical properties can be exhibited in the ohase soace of (nn, θ, m).
Bibliography:spinor Bose-Einstein condensates, dissipation, master equation
We investigate the internal dynamics of the spinor Bose-Einstein condensates subject to dissipation by solving the Lindblad master equation. It is shown that for the condensates without dissipation its dynamics always evolve along a specific orbital in the phase space of (no, O) and display three kinds of dynamical properties including Josephson-like oscil- lation, self-trapping-like oscillation, and 'running phase'. In contrast, the condensates subject to dissipation will not evolve along the specific dynamical orbital. If component-1 and component-(-1) dissipate at different rates, the magnetization m will not conserve and the system transits between different dynamical regions. The dynamical properties can be exhibited in the ohase soace of (nn, θ, m).
11-5639/O4
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ISSN:1674-1056
2058-3834
1741-4199
DOI:10.1088/1674-1056/25/4/040501