The renormalization method of Bogoljubov-Parasiuk-Hepp-Zimmermann (BPHZ) isused in order to derive the renormalized energy shift due to the gaugeinvariant K\"all\'en-Sabry diagram of the two-photon vacuum polarization (VPVP)as well as the self energy vacuum polarization S(VP)E beyond the Uehlingapproximation. It is outlined, that no outer renormalization is required forthe two-photon vacuum polarization and that only the inner renormalization hasto b e accomplished. It is shown that the so-called nongauge invariant spuriousterm is absent for a wide class of vacuum polarization (VP) diagrams if oneapplies the widely used spherical expansion of bound and free-electron propagator. This simplifies significantly calculations in bound state quantumelectrodynamis . As one result of our paper the use of the BPHZ-approach inbound state QED is established.
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机译:使用Bogoljubov-Parasiuk-Hepp-Zimmermann(BPHZ)的重归一化方法,以归因于双光子真空极化(VPVP)的规范不变K \“ all \'en-Sabry图以及概述了自能量真空极化S(VP)E超出了Uehling逼近,概述了双光子真空极化不需要外部重归一化,而仅需要完成内部重归一化,这表明所谓的非规范不变如果应用广泛使用的束缚和自由电子传播子的球形展开,则对于一大类真空极化(VP)图来说,杂散项就不存在了,这大大简化了束缚态量子电动力学的计算。作为本文的结果之一,BPHZ-建立进场状态QED。
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