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素粒子論研究

Renormalization Condition on Self-Energy at Two-Loop Level for Trapped Atomic Gas (熱場の量子論とその応用)

雅彦 奥村, Y. Yamanaka

Published Feb 20, 2005• 0 citations
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Renormalization Condition on Self-Energy at Two-Loop Level for Trapped Atomic Gas

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Dynamics of a Trapped Bose-Condensed Gas at Finite Temperatures (熱場の量子論とその応用)

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Bose-Einstein condensates in toroidal traps: Instabilities, swallow-tail loops, and self-trapping

Soheil Baharian, Gordon Baym

We study the stability and dynamics of an ultracold bosonic gas trapped in a toroidal geometry and driven by rotation in the absence of dissipation. We first delineate, via the Bogoliubov mode expansion, the regions of stability and the nature of instabilities of the system for both repulsive and attractive interaction strengths. To study the response of the system to variations in the rotation rate, we introduce a ``disorder'' potential, breaking the rotational symmetry. We demonstrate the breakdown of adiabaticity as the rotation rate is slowly varied and find forced tunneling between the system's eigenstates. The nonadiabaticity is signaled by the appearance of a swallow-tail loop in the lowest-energy level, a general sign of hysteresis. Then, we show that this system is in one-to-one correspondence with a trapped gas in a double-well potential and thus exhibits macroscopic quantum self-trapping. Finally, we show that self-trapping is a direct manifestation of the behavior of the lowest-energy level.

arXiv:1211.2276•Physical Review A•Jan 17, 2013•37 citations

RENORMALIZATION CONDITION IN TRAPPED BOSE-EINSTEIN CONDENSATION

Masahiko Okumura, Y. Yamanaka

素粒子論研究•Jan 1, 2004•0 citations
We study the stability and dynamics of an ultracold bosonic gas trapped in a toroidal geometry and driven by rotation in the absence of dissipation. We first delineate, via the Bogoliubov mode expansion, the regions of stability and the nature of instabilities of the system for both repulsive and attractive interaction strengths. To study the response of the system to variations in the rotation rate, we introduce a ``disorder'' potential, breaking the rotational symmetry. We demonstrate the breakdown of adiabaticity as the rotation rate is slowly varied and find forced tunneling between the system's eigenstates. The nonadiabaticity is signaled by the appearance of a swallow-tail loop in the lowest-energy level, a general sign of hysteresis. Then, we show that this system is in one-to-one correspondence with a trapped gas in a double-well potential and thus exhibits macroscopic quantum self-trapping. Finally, we show that self-trapping is a direct manifestation of the behavior of the lowest-energy level.