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Self-energy of one electron in non-relativistic QED

机译:非相对论量子力学中一个电子的自能

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We investigate the self-energy of one electron coupled to a quantized radiation field by extending the ideas developed in Hainzl (Ann. H. Poincare, in press). We fix an arbitrary cutoff parameter Lambda and recover the alpha(2)-term of the self-energy, where alpha is the coupling parameter representing the fine structure constant. Thereby we develop a method which allows to expand the self-energy up to any power of alpha. This implies that perturbation theory in alpha is correct if Lambda is fix. As an immediate consequence we obtain enhanced binding for electrons. (C) 2003 Elsevier Inc. All rights reserved. [References: 12]
机译:我们通过扩展在海伦茨(Ann。H. Poincare,付印中)提出的思想来研究耦合至量化辐射场的一个电子的自能。我们固定一个任意的截止参数Lambda并恢复自能的alpha(2)项,其中alpha是代表精细结构常数的耦合参数。因此,我们开发了一种方法,该方法可以将自能量扩展到任何α幂。这意味着如果Lambda是固定的,则alpha中的扰动理论是正确的。作为直接结果,我们获得了增强的电子结合。 (C)2003 Elsevier Inc.保留所有权利。 [参考:12]

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