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Macroscopic quantum tunneling of two coupled particles in the presence of a transverse magnetic field

机译:在横向磁场中两个耦合粒子的宏观量子隧穿

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Two coupled particles of identical mass but opposite charge are studied, with a constant transverse external magnetic field and an external potential, interacting with a bath of harmonic oscillators. We show that the problem cannot be mapped to a one-dimensional problem like the one in Ao (Phys. Rev. Lett. 72, 1898 (1994)), it strictly remains two-dimensional. We calculate the effective action both for the case of linear coupling to the bath and without a linear coupling using imaginary time path integral at finite temperature. At zero temperature we use Leggett's prescription to derive the effective action. In the limit of zero magnetic field we recover a two-dimensional version of the result derived in Chudnovsky (Phys. Rev. B, 54, 5777 (1996)) for the case of two identical particles. We find that in the limit of strong dissipation, the effective action reduces to a two-dimensional version of the Caldeira-Leggett form in terms of the reduced mass and the magnetic field. The case of ohmic dissipation with the motion of the two particles damped by the ohmic frictional constant η is studied in detail.
机译:研究了质量相等但电荷相反的两个耦合粒子,它们具有恒定的横向外部磁场和外部电势,并与谐波振荡器的浴相互作用。我们表明,该问题不能像Ao中的一维问题(Phys。Rev. Lett。72,1898(1994))那样映射到一维问题,它严格地保持二维。我们使用有限温度下的假想时间路径积分,计算了与熔池线性耦合的情况和没有线性耦合情况下的有效作用。在零温度下,我们使用Leggett的处方得出有效的作用。在零磁场的极限下,对于两个相同的粒子,我们恢复了Chudnovsky推导的结果的二维形式(Phys。Rev. B,54,5777(1996))。我们发现,在强耗散的极限内,就减小的质量和磁场而言,有效作用减小为Caldeira-Leggett形式的二维形式。详细研究了欧姆耗散的情况,其中两个粒子的运动受到欧姆摩擦常数η的阻尼。

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