On the electromagnetic interaction and the anomalous term in the Duffin-Kemmer-Petiau theory

A. G. Jirón Vicente, Luis B. Castro, Antonio S. de Castro, A. Obispo
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Abstract

The problem of vectorial mesons embedded in an electromagnetic field via Duffin-Kemmer-Petiau (DKP) formalism is reinvestigated. Considering the electromagnetic interaction as a minimal coupling, an incorrect value (g = 1) is identified for the gyromagnetic factor (g-factor). Furthermore, it is shown that is cumbersome to find analytical solutions due to the presence of the so-called anomalous term for the spin-1 sector of the DKP theory. Suspecting that the anomalous term results from an incomplete version of the DKP equation to describe the electromagnetic interaction, we consider the addition of a non-minimal coupling. This leads to the correct g-factor (g = 2), and as a consequence, the anomalous term becomes proportional to an external four current. As an application, the DKP equation with a static uniform magnetic field is considered, yielding the corresponding Landau levels.
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关于达芬-凯末尔-佩蒂奥理论中的电磁相互作用和反常项
通过达芬-凯默-佩蒂奥(DKP)形式主义重新研究了嵌入电磁场的矢量介子问题。将电磁相互作用视为最小耦合,发现了回旋磁因子(g-因子)的错误值(g = 1)。此外,由于 DKP 理论的自旋-1 扇区存在所谓的反常项,因此寻找解析解非常麻烦。我们怀疑反常项是由于描述电磁相互作用的 DKP 方程版本不完整造成的,因此考虑添加一个非最小耦合。这导致了正确的 g 因子(g = 2),因此,反常项变得与外部四电流成正比。作为应用,我们考虑了静态均匀磁场下的 DKP 方程,并得出了相应的朗道水平。
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