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arXiv quant-ph/0512140quant-phgr-qchep-ph
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一个简单的五维Dirac粒子波动方程

A Simple Five-Dimensional Wave Equation for a Dirac Particle

N. Redington, M. A. K. Lodhi

摘要:

在五维空间中构造了一阶相对论波动方程。它的解是八分量旋量,可以解释为四维时空中的单粒子费米子波函数。使用“圆柱条件”(去除对第五坐标的显式依赖)将每个八分量解简化为一对服从狄拉克方程的退化四分量旋量。这种五维方法用于获得自由粒子和在库仑势中运动的粒子的解。结果表明,在圆柱条件下,所得结果与Dirac方程的结果相同。另一方面,如果没有圆柱体条件,方程预测了一些有趣的新现象。它意味着标量势的存在,对于零质量粒子,它导致了一个四维费米子方程,类似于麦克斯韦方程。

英文摘要:

A first-order relativistic wave equation is constructed in five dimensions. Its solutions are eight-component spinors, which are interpreted as single-particle fermion wave functions in four-dimensional spacetime. Use of a ``cylinder condition'' (the removal of explicit dependence on the fifth coordinate) reduces each eight-component solution to a pair of degenerate four-component spinors obeying the Dirac equation. This five-dimensional method is used to obtain solutions for a free particle and for a particle moving in the Coulomb potential. It is shown that, under the cylinder condition, the results are the same as those from the Dirac equation. Without the cylinder condition, on the other hand, the equation predicts some interesting new phenomena. It implies the existence of a scalar potential, and for zero-mass particles it leads to a four-dimensional fermionic equation analogous to Maxwell's equation with sources.

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