2008/05/31 by Joachim Brand, Tania J. Haigh, U. Zülicke +1
Chemistry · Mathematics · Physics and Astronomy · #Bose–Einstein condensate #Chemistry #Cold Atom Physics and Bose-Einstein Condensates #Composite material #Computer science #Condensed matter physics #Coupling (piping) #Materials science #Mathematical analysis #Mathematics #Physics #Quantum, superfluid, helium dynamics #Ring (chemistry) #Sign (mathematics) #Stability (learning theory) #Strong Light-Matter Interactions #quant-ph
paper · pdf · doi:10.1103/physreva.81.025602
published as Phys. Rev. A 81, 025602 (2010) · 4 pages, comment on Phys. Rev. Lett. 98, 050401 (2007) [arXiv:quant-ph/0609133v2]
arxiv created 2009/08/16 · openalex publication_date 2010/02/08 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We revisit recent claims about the instability of nonrotating tunnel coupled annular Bose-Einstein condensates leading to the emergence of angular momentum Josephson oscillation [Phys. Rev. Lett. 98, 050401 (2007)]. It was predicted that all stationary states with uniform density become unstable in certain parameter regimes. By careful analysis, we arrive at a different conclusion. We show that there is a stable nonrotating and uniform ground state for any value of the tunnel coupling and repulsive interactions. The instability of an excited state with \ensuremathπ phase difference between the condensates can be interpreted in terms of the familiar snake instability. We further discuss the sign of the tunnel coupling through a separating barrier, which carries significance for the nature of the stationary states. It is found to always be negative for physical reasons.