等效原理测试,等效定理,和新的远程力

Pierre Fayet
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引用次数: 5

摘要

我们讨论了由自旋为1或自旋为0的粒子介导的新的远程力的可能存在。如果将它们的效应与引力的效应加在一起,它们可能会导致对等效原理的明显违反。虽然在一个新的自旋为1u的玻色子的耦合中,矢量部分通常涉及B和L电流的组合,但也可能存在轴向部分。如果新的力具有有限范围λ,则其强度与1/(λ 2f2)成正比,F为额外的U(1)对称破坏尺度。令人惊讶的是,粒子物理实验可以提供对这种新力的约束,即使它非常弱,相应的规范耦合非常小(⪡10−19!)。“等效定理”表明,即使规范耦合消失,自旋为1的非常轻的U玻色子通常也不会解耦,而是表现为自旋为0的准无质量粒子,具有与1/F成比例的伪标量耦合。类似地,在超对称理论中,一个自旋为32的非常轻的引力子可能被探测为一个自旋为12的准无质量的金态引力子,尽管牛顿引力常数GN非常小,但前提是超对称破缺尺度不是太大。在ψ和y衰变中搜索这样的U玻色子限制了F大于电弱尺度(在粒子物理中,如果F足够大,U实际上会变成一个轴子,准“不可见”)。这为相应的新力及其相关的EP违反提供了强有力的约束。我们还简要讨论了新的自旋相关力。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Equivalence principle tests, equivalence theorems, and new long-range forces

We discuss the possible existence of new long-range forces mediated by spin-1 or spin-0 particles. By adding their effects to those of gravity, they could lead to apparent violations of the equivalence principle. While the vector part in the couplings of a new spin-1 U boson involves, in general, a combination of the B and L currents, there may also be, in addition, an axial part as well. If the new force has a finite range λ, its intensity is proportional to 1/(λ2F2), F being the extra U(1) symmetry-breaking scale.

Quite surprisingly, particle physics experiments can provide constraints on such a new force, even if it is extremely weak, the corresponding gauge coupling being extremely small (⪡10−19!). An ‘equivalence theorem’ shows that a very light spin-1 U boson does not in general decouple even when its gauge coupling vanishes, but behaves as a quasi-massless spin-0 particle, having pseudoscalar couplings proportional to 1/F. Similarly, in supersymmetric theories, a very light spin-32 gravitino might be detectable as a quasi-massless spin-12 goldstino, despite the extreme smallness of Newton's gravitational constant GN, provided that the supersymmetry-breaking scale is not too large.

Searches for such U bosons in ψ and ϒ decays restrict F to be larger than the electroweak scale (the U actually becoming, as an axion, quasi ‘invisible’ in particle physics for sufficiently large F). This provides strong constraints on the corresponding new force and its associated EP violations. We also discuss briefly new spin-dependent forces.

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