论文标题
超对称场旋转角
Hypersymmetry field rotation angle
论文作者
论文摘要
该论文确定了断裂（HYSY）破裂的极限能量。根据衡量理论，介导Spin-0玻色子的相互作用必须无质量。 Hysy理论预测了大规模的中间玻色子。本文描述的高度对称场旋转证明了hysy介导的玻色子的质量。中间玻色子的质量必须由hysy群体的动态自发破裂产生。 Hysy旋转在速度依赖性D场中进行。田地的衍生旋转是由速度V的自发对称性断裂和在D场中的第三个投影（产生了场s玻色子的质量）的速度。后者代表了朝向目标粒子的方向上发射玻色子粒子的真实且有效的速度。讨论的（虚拟）金石玻色子的质量可以通过HIGGS（BEH）机制来消除。根据标准模型（SM）相互作用S对称组和（SM SM）Hysy组的同时存在，应将其玻色子一起转换。 HYSY的自发分解可能允许进行不影响研究系统的身体状态的转换。本文描述了一种场变化，该野外玻色子的质量，使SM和Hysy玻色子质量一起旋转，同时使SM玻色子完好无损。结果是一个角度，通过产生场的速度的进进机制来表征hysy。与已知的SM中间玻色子相比，Hysy中间玻色子没有固定质量。 Hysy中间玻色子的质量（作为速度依赖性量规d的量子d）的质量取决于其介导相互作用的颗粒的相对速度。因此，衍生的进动角是该速度的函数。
The paper determines the limit energy under which hypersymmetry (HySy) is broken. According to gauge theories, interaction mediating spin-0 bosons must be massless. The theory of HySy predicted massive intermediate bosons. Hypersymmetry field rotation, described in this paper, justifies the mass of the HySy mediating boson. The mass of intermediate bosons must arise from dynamical spontaneous breaking of the group of HySy. HySy rotation is performed in the velocity-dependent D field. The derived rotation of the field is defined by the spontaneous symmetry breaking and precession of the velocity v around its third projection in the D field (that produced the mass of the field s bosons). The latter represents the real and effective velocities of a boson-emitting particle in the direction towards a target particle. The mass of the discussed (fictitious) Goldstone bosons can be removed by the unitarity gauge condition through Higgs (BEH) mechanism. According to the simultaneous presence of a Standard Model (SM) interaction s symmetry group and the (beyond SM) HySy group, their bosons should be transformed together. Spontaneous breakdown of HySy may allow performing a transformation that does not influence the SM physical state of the investigated system. The paper describes a field transformation that eliminates the mass of the intermediate bosons, rotates the SM- and HySy bosons masses together while leaving the SM bosons intact. The result is an angle that characterises the HySy by a precession mechanism of the velocity that generates the field. In contrast to the known SM intermediate bosons, the HySy intermediate bosons have no fixed mass. The mass of the HySy intermediate bosons (that appear as quanta of a velocity-dependent gauge field D) depends on the relative velocity of the particles whose interaction they mediate. So, the derived precession angle is a function of that velocity.
