Spin effects from Four Bosons EM

R. Doria, L. Mendes
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Abstract

Electromagnetism is the theory of electric charge and spin. Our study is on a spin-valued four bosons electromag- netism. An EM under the charge exchange {+, 0, −} intermediated by four bosons {AμI } ≡ {Aμ, Uμ, V ± μ } where Aμ means the usual photon, Uμ a massive photon, V ± μ charged photons. EM should express electric charge and spin together. Understand from first principles on the spin role in the electric and magnetic properties of particles. Theoretically, the spin is a space-time physical entity derived from Lorentz group. Phenomenologically, it appears as a vectorial entity inserted in the magnetic moment and electric dipole. A theoretical closure between them is expected. A spin-valued four bosons EM is constituted by introducing Lorentz group Lie Algebra valued fields. Consider the quadruplet fields as A I μ = A I μ,κλ(Σκλ)αβ where (Σκλ)αβ is the Lorentz generator. It provides spin as an intrinsec entity compatible with relativity and group theory. Similarly to the non-abelian gauge theory, where Aμa = Aμata, one incorporates the spin valued field through a Lie algebra. From first principles. Electric charge and spin are unified under a constructivist Lagrangian. Spin effects arestudied through equations of motion and Bianchi identities. Enlarging the EM for interactions beyond electric charge. Four types are derived. Usual electric charge interaction, neutral interaction, electric charge and spin, neutral and spin. A formalism is expressed. The spin valued performance is related through a Lagrangian. Spin interactions are derived. The magnetic moment and electric dipole are expressed by vectors S~ and ~s respectivity. They are able to couple spin with granular and collective fields strengths. Developing interacting terms constitutive as B~ · S~, E~ · ~s, ~e · S~ and so on. Faraday interaction between magnetic field and photon is reproduced from first principles.
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电磁四玻色子的自旋效应
电磁学是关于电荷和自旋的理论。我们研究的是自旋值四玻色子电磁学。由四个玻色子 {AμI } 介导的电荷交换 {+, 0, -} 下的电磁学≡ {Aμ, Uμ, V ± μ },其中 Aμ 表示普通光子,Uμ 表示大质量光子,V ± μ 表示带电光子。电磁应同时表示电荷和自旋。从第一原理上理解自旋在粒子的电性和磁性中的作用。从理论上讲,自旋是洛伦兹群衍生出来的时空物理实体。从现象上看,它是插入磁矩和电偶极子的矢量实体。它们之间的理论闭合是意料之中的。自旋值四玻色子电磁场是通过引入洛伦兹群列代数值场构成的。将四玻色子场视为 A I μ = A I μ,κλ(Σκλ)αβ,其中 (Σκλ)αβ 是洛伦兹发生器。它提供了与相对论和群论兼容的自旋内部实体。与 Aμa = Aμata 的非阿贝尔规理论类似,我们通过一个李代数纳入了自旋有价场。从第一原理出发电荷和自旋统一于建构主义拉格朗日之下。通过运动方程和比安奇等式研究自旋效应。为电荷以外的相互作用扩大电磁。推导出四种类型。通常的电荷相互作用、中性相互作用、电荷与自旋、中性与自旋。表达了一种形式主义。通过拉格朗日将自旋值性能联系起来。得出了自旋相互作用。磁矩和电偶极子由矢量 S~ 和 ~s 表示。它们能够将自旋与颗粒场和集合场强度耦合。发展相互作用的构成项为 B~ - S~、E~ - ~s、~e - S~等。从第一原理再现了磁场与光子之间的法拉第相互作用。
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