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arXiv 2011.06588hep-thgr-qc
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弯曲时空中的经典双拷贝:来自双伴随标量的微扰杨-米尔斯理论

The classical double copy in curved spacetimes: Perturbative Yang-Mills from the bi-adjoint scalar

Siddharth G. Prabhu

AI总结:

本研究构建弯曲时空经典场的双拷贝形式,建立双伴随标量与杨-米尔斯方程微扰解的全阶映射,验证其平直空间极限与规范无关性,拓展了双拷贝理论的适用范围。

摘要:

我们构建了适用于弯曲时空经典场的一种双拷贝形式,建立了位置空间中双伴随标量方程微扰解与杨-米尔斯方程微扰解之间的对应关系。在线性阶层面,我们证明在最大对称时空背景下,两类解之间存在映射:通过对双伴随标量解作用合适的微分算子,即可得到所有杨-米尔斯解。基于该线性映射的存在性,我们进一步证明,任意微扰阶的杨-米尔斯方程解都可以用对应的双伴随标量解表示。这种全阶映射与平直空间的BCJ双拷贝类似,适用于所有可开展微扰展开的弯曲时空。我们验证了这些结果具有正确的平直空间极限,且该对应关系不依赖于规范选择。

英文摘要:

We formulate a version of the double copy for classical fields in curved spacetimes. We provide a correspondence between perturbative solutions to the bi-adjoint scalar equations and those of the Yang-Mills equations in position space. At the linear level, we show that there exists a map between these solutions for maximally symmetric spacetime backgrounds, that provides every Yang-Mills solution by the action of an appropriate differential operator on a bi-adjoint scalar solution. Given the existence of a linearized map, we show that it is possible to cast the solutions of the Yang-Mills equations at arbitrary perturbation order in terms of the corresponding bi-adjoint scalar solutions. This all-order map is reminiscent of the flat space BCJ double copy, and works for any curved spacetime where the perturbative expansion holds. We show that these results have the right flat space limit, and that the correspondence is agnostic to the choice of gauge.

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