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arXiv 0705.2789quant-ph
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磁场中的欧几里德共振

Euclidean resonance in a magnetic field

B. Ivlev

摘要:

我们发现Wigner共振隧穿与在静态磁场中穿过静态势垒的隧穿类似,在Wigner隧穿过程中,电子遇到一个经典允许的区域,在这个区域中,电子的能量与分立能级重合,而在磁场中,势垒在隧穿方向上是一个常数。沿着隧穿路径形成某些区域,在这些区域中,用经典语言来说,垂直于隧穿的运动的动能是负的。这些区域起到势阱的作用,其中离散的能级可以与电子能量一致。这种在特定磁场下发生的现象被称为欧几里得共振,并且基本上取决于在垂直于隧穿的方向上的势的形状。在欧几里得共振条件下,长距离的壁下运动是可能的。

英文摘要:

An analogy between Wigner resonant tunneling and tunneling across a static potential barrier in a static magnetic field is found. Whereas in the process of Wigner tunneling an electron encounters a classically allowed regions, where a discrete energy level coincides with its energy, in the magnetic field a potential barrier is a constant in the direction of tunneling. Along the tunneling path the certain regions are formed, where, in the classical language, the kinetic energy of the motion perpendicular to tunneling is negative. These regions play a role of potential wells, where a discrete energy level can coincide with the electron energy. Such phenomenon, which occurs at the certain magnetic field, is called Euclidean resonance and substantially depends on a shape of potential forces in the direction perpendicular to tunneling. Under conditions of Euclidean resonance a long distance underbarrier motion is possible.

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