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arXiv quant-ph/0305049quant-ph
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关于角动量理论的注记

Remarks on the Theory of Angular Momenta

O. Chavoya-Aceves

摘要:

对应规则的严格应用表明,量子粒子的角动量算符--对应于经典的幅度$\mathbf{l}= m \mathbf{r} \wedge \mathbf{v}$ --在电磁场的存在下由$\mathbf{\hat{l}}=\mathbf{r}\wedge(-i\hbar\mathbf{\nabla} -\frac{e}{c}\mathbf{A})$给出。因此,尽管对相应的量子化规则有普遍的看法,角动量的本征值取决于电磁场的位形。作为角动量微积分和\emph{spin}理论基础的通常的对易规则$[{\hat{l}}_i,{\hat{l}}_j]=i\hbarε_{ijk}{\hat{l}}_k$--以及玻姆的EPR论证的例子--在电磁场存在的情况下是无效的。算符$\mathbf{\hat{l}}=-i\hbar\mathbf{r}\wedge\mathbf{\nabla}$的期望值不是规范不变的,它依赖于电动势的校准。

英文摘要:

A rigorous application of the correspondence rules shows that the operator of the angular momentum of a quantum particle---corresponding to the classical magnitude $\mathbf{l}= m \mathbf{r} \wedge \mathbf{v}$---is given by $\mathbf{\hat{l}}=\mathbf{r}\wedge(-i\hbar\mathbf{\nabla} -\frac{e}{c}\mathbf{A})$ in the presence of an electromagnetic field. Thus, despite the general opinion on the corresponding rules of quantization, the eigenvalues of the angular momentum depend on the configuration of the electromagnetic field. The usual rules of commutation $[{\hat{l}}_i,{\hat{l}}_j]=i\hbarε_{ijk}{\hat{l}}_k$, that are at the foundation of the calculus of angular momentum and of the theory of \emph{spin}---and Bohm's example of the EPR argument---are not valid in the presence of an electromagnetic field. The expected value of the operator $\mathbf{\hat{l}}=-i\hbar\mathbf{r}\wedge\mathbf{\nabla}$ is not gauge invariant, it depends on the calibration of the electrodynamic potentials.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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