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Calculations of the dominant long-range, spin-independent contributions to the interaction energy between two nonrelativistic Dirac fermions from double-boson exchange of spin-0 and spin-1 bosons with spin-dependent couplings

机译:计算主要的远程,自旋独立贡献   两个非相对论狄拉克费米子之间的相互作用能量   具有自旋相关的spin-0和spin-1玻色子的双玻色子交换   联轴器

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摘要

Various theories beyond the Standard Model predict new particles with massesin the sub-eV range with very weak couplings to ordinary matter which canpossess spin-dependent couplings to electrons and nucleons. Present laboratoryconstraints on exotic spin-dependent interactions with pseudoscalar and axialcouplings for exchange boson masses between meV and eV are very poor comparedto constraints on spin-independent interactions in the same mass range arisingfrom spin-0 and spin-1 boson exchange. It is therefore interesting to analyzein a general way how one can use the strong experimental bounds onspin-independent interactions to also constrain spin-dependent interactions byconsidering higher-order exchange processes. The exchange of a pair of bosonsbetween two fermions with spin-dependent couplings will possess contributionswhich flip spins twice and thereby generate a polarization-independentinteraction energy which can add coherently between two unpolarized objects. Inthis paper we derive the dominant long-range contributions to the interactionenergy between two nonrelativistic spin-1/2 Dirac fermions from double exchangeof spin-0 and spin-1 bosons proportional to couplings of the form $g_P^{4}$,$g_S^{2}g_P^{2}$, and $g_V^{2}g_A^{2}$. Our results for $g_P^{4}$ are inagreement with previous calculations that have appeared in the literature. Wedemonstrate the usefulness of this analysis to constrain spin-dependentcouplings by presenting the results of a reanalysis of data from a short-rangegravity experiment to derive an improved constraint on $(g^N_{P})^2$, thepseudoscalar coupling for nucleons, in the range between $40$ and $200~\mu$m ofabout a factor of 5 compared to previous limits. The spin-independentcontribution from 2-boson exchange with axial-vector couplings requires specialtreatment and will be explored in another paper.
机译:超出标准模型的各种理论预测,新粒子的质量在亚eV范围内,与普通物质的耦合非常弱,这可能导致电子和核子自旋相关的耦合。与在同质量范围内自旋0和自旋1玻色子交换引起的与自旋无关的相互作用的约束相比,目前在实验室上对与拟标量和轴向耦合的异质自旋依赖的相互作用进行限制,以在meV和eV之间交换玻色子质量。因此,有趣的是,以一种通用的方式来分析人们如何可以利用自旋无关的相互作用的强大实验界限,通过考虑更高阶的交换过程来限制自旋依赖性的相互作用。在两个费米子之间以自旋相关的耦合交换一对玻色子将具有贡献,该贡献使自旋翻转两次,从而产生可以独立地在两个非极化对象之间相干添加的极化无关的相互作用能。在本文中,我们通过自旋0和自旋1玻色子的两次交换与形式为$ g_P ^ {4} $,$ g_S的耦合成比例,得出了对两个非相对论自旋1/2 Dirac费米子相互作用能的主要长期贡献。 ^ {2} g_P ^ {2} $和$ g_V ^ {2} g_A ^ {2} $。我们对$ g_P ^ {4} $的结果与文献中出现的先前计算不一致。通过展示短程重力实验的数据重新分析结果,得​​出对$(g ^ N_ {P})^ 2 $的改进约束(核子的准标量耦合),来证明这种分析对约束自旋依赖性耦合的有效性。在40美元到200美元之间的范围是以前的限制的5倍。 2玻色子交换与轴向矢量耦合的自旋无关贡献需要特殊处理,并将在另一篇论文中进行探讨。

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