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arXiv 2408.16474hep-th
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恒定场中N光子振幅的低能极限:第二部分

Low-energy limit of N-photon amplitudes in a constant field: Part II

Misha A. Lopez-Lopez

AI总结:

本文利用世界线形式体系推导了标量和旋量QED在恒定背景场中N光子振幅低能极限的级数表示,将其化为单一固有时积分,并在恒定交叉场下得到含阶乘函数的紧凑表达式及用伯努利数和旋量积表示的所有螺旋度分量。

摘要:

我们采用世界线形式体系,推导了标量QED和旋量QED在恒定背景场中N光子振幅低能极限的级数表示。随后,这些振幅被写为单一固有时积分的形式。当考虑恒定交叉场时,上述级数表示会终止。这使得我们能够为这些特定振幅获得更紧凑的表达式,其中在固定参数下,固有时积分的结果呈现阶乘函数的形式。此外,我们推导了这些振幅的所有螺旋度分量,并用伯努利数和旋量积显式地表示出来。

英文摘要:

We employ the worldline formalism to derive a series representation of the low-energy limit of the N -photon amplitude in a constant background field for both scalar and spinor QED. The amplitudes are then written in terms of a single proper-time integral. The above-mentioned series representation terminates when considering a constant crossed field. This allows us to obtain even more compact expressions for these particular amplitudes for which the result of the proper-time integral, for fixed parameters, takes the form of a factorial function. In addition, we derive all helicity components of these amplitudes and express them explicitly in terms of Bernoulli numbers and spinor products.

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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