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arXiv 1204.5337hep-ph
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基本自旋1/2,1和3/2粒子的电磁多极矩

Electromagnetic multipole moments of elementary spin-1/2, 1, and 3/2 particles

E. G. Delgado-Acosta, M. Kirchbach, M. Napsuciale, S. Rodríguez

摘要:

我们研究多极分解的电磁流自旋1/2,1,3/2粒子描述的拉格朗日方程,旨在重现代表特定的波动方程是二阶的动量,出现在最近阐述庞加莱协变投影仪方法。我们计算了上述自旋的电多极子的旋量,四矢量,和四矢量旋量表示,参加最一般的非拉格朗日自旋3/2电流,这是允许的洛伦兹不变性是三阶的动量和构造的线性电流等效的相同的多极矩的其中之一。我们的结论是,这种非拉格朗日电流不一定比出现在协变投影方法的两项电流更一般。我们比较我们的结果与传统的Proca,和Rarita Schwinger框架。最后,我们通过将自旋为1和自旋为3/2分别置于(1,0)$\oplus$(0,1)和(3/2,0)$\oplus$(0,3/2)单自旋表示中来测试多极子的表示依赖性。我们观察代表独立的电荷单极子和磁偶极子,在较高的多极子,这原来是代表依赖。特别是,我们发现双矢量$(1,0)\oplus (0,1)$的特点是与$(1/2,1/2)$中发现的电四极矩符号相反,因此,与$W$玻色子的电四极矩符号相反。我们的发现指出,$ρ$介子可以转换为反对称张量的一部分,$a_{1}$介子类作为其代表同伴的可能性。

英文摘要:

We study multipole decompositions of the electromagnetic currents of spin-1/2, 1, and 3/2 particles described in terms of Lagrangians designed to reproduce representation specific wave equations which are second order in the momenta and which emerge within the recently elaborated Poincaré covariant projector method. We calculate the electric multipoles of the above spins for the spinor, the four-vector, and the four-vector--spinor representations, attend to the most general non-Lagrangian spin-3/2 currents which are allowed by Lorentz invariance to be of third order in the momenta and construct the linear current equivalent of identical multipole moments of one of them. We conclude that such non-Lagrangian currents are not necessarily more general than the two-term currents emerging within the covariant projector method. We compare our results with those of the conventional Proca-, and Rarita-Schwinger frameworks. Finally, we test the representation dependence of the multipoles by placing spin-1 and spin-3/2 in the respective (1,0)$\oplus$(0,1), and (3/2,0)$\oplus$(0,3/2) single-spin representations. We observe representation independence of the charge monopoles and the magnetic dipoles, in contrast to the higher multipoles, which turn out to be representation dependent. In particular, we find the bi-vector $(1,0)\oplus (0,1)$ to be characterized by an electric quadrupole moment of opposite sign to the one found in $(1/2,1/2)$, and consequently, to the $W$ boson. Our finding points toward the possibility that the $ρ$ meson could transform as part of an antisymmetric tensor with an $a_{1}$ meson-like state as its representation companion.

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