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arXiv 1209.2663hep-phastro-ph.HEhep-thnucl-th
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强磁场中的真空双折射:(I)所有朗道能级的光子偏振张量

Vacuum birefringence in strong magnetic fields: (I) Photon polarization tensor with all the Landau levels

Koichi Hattori, Kazunori Itakura

摘要:

在强磁场中传播的光子受到称为“真空双折射”的现象的影响,其中两个物理模式的折射率都偏离1并且彼此不同。利用Schwinger的本征时间方法计算了光子在静态均匀磁场中的真空极化张量,得到了关于本征时间变量的解析二重积分的级数表示.结果表示为已知函数的无穷和,这可以解释为所有朗道费米子能级的求和。每个贡献从无限多个朗道水平产生一个运动学条件以上的贡献有一个虚部。这表明一个足够能量的光子衰变成一个费米子-反费米子对,并具有相应的朗道能级指数。由于我们没有采用任何近似,因此我们的结果适用于光子动量的整个运动学区域和任何大小的外磁场中折射率的计算。

英文摘要:

Photons propagating in strong magnetic fields are subject to a phenomenon called the "vacuum birefringence" where refractive indices of two physical modes both deviate from unity and are different from each other. We compute the vacuum polarization tensor of a photon in a static and homogeneous magnetic field by utilizing Schwinger's proper-time method, and obtain a series representation as a result of double integrals analytically performed with respect to proper-time variables. The outcome is expressed in terms of an infinite sum of known functions which is plausibly interpreted as summation over all the Landau levels of fermions. Each contribution from infinitely many Landau levels yields a kinematical condition above which the contribution has an imaginary part. This indicates decay of a sufficiently energetic photon into a fermion-antifermion pair with corresponding Landau level indices. Since we do not resort to any approximation, our result is applicable to the calculation of refractive indices in the whole kinematical region of a photon momentum and in any magnitude of the external magnetic field.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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