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Erratum: Quantum mechanics of a constrained electrically charged particle in the presence of electric currents [Phys. Rev. A 80, 052109 (2009)]

机译:勘误:存在电流时受约束的带电粒子的量子力学[Phys。 Rev. A 80,052109(2009)]

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摘要

In our article, we used the following definition of the extrinsic curvature tensor Kij [1] (following the notation in our article): VI l; N/ —Kii. However, in our article, after Eq. (17), the sign of the extrinsic curvature tensor followed the convention V11 iNi = Kii but did not correct for the change in the sign of the extrinsic curvature. When we correct for this missed minus sign, the divergence of the electromagnetic vector potential A in Eqs. (18), (23), and (26) reads V ;1*2A3M)*,(t"11 Ali + 83A3 — where * denotes the wave function and M is the mean curvature in the surface M . If we choose not to fix the electromagnetic gauge, the last term in this expression apparently cancels a corresponding term that appears in the A3 V1* term in the Schrodinger equation. This cancellation apparently removes a possible unphysical contribution to the orbital magnetic moment of the particle. This leaves us with the same expression for the Schrodinger equation in an unfixed electromagnetic gauge as the one in Ref. [2], thus leaving the impression that there is no coupling between curvature and electromagnetic field,
机译:在我们的文章中,我们使用了外在曲率张量Kij [1]的以下定义(遵循本文中的表示法): N / —基伊。但是,在我们的文章中,等式之后。 (17),外曲率张量的符号遵循惯例V11 iNi = Kii,但没有校正外曲率符号的变化。当我们校正这个丢失的负号时,电磁矢量势A的方差为Eqs。 (18),(23)和(26)读取V; 1 * 2A3M)*,(t“ 11 Ali + 83A3 —其中*表示波函数,M是表面M的平均曲率。为了固定电磁量规,该表达式中的最后一项显然抵消了Schrodinger方程中A3 V1 *项中出现的相应项,这种抵消显然消除了对粒子轨道磁矩的可能的非物理影响。在不固定的电磁量规中对Schrodinger方程的表达式与参考文献[2]中的表达式相同,因此给人的印象是曲率与电磁场之间没有耦合,

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