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Titlebook: Vacuum Structure in Intense Fields; H. M. Fried,Berndt Müller Book 1991 Plenum Press, New York 1991 Potential.Renormalization group.electr

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31#
發(fā)表于 2025-3-26 22:07:19 | 只看該作者
32#
發(fā)表于 2025-3-27 03:30:08 | 只看該作者
Application of the Proper-Time Method to Non-Perturbative Effects in QEDcided in this written version to concentrate on the topic of Schwinger’s proper time representation for the electron’s Green function and its possible application to the understanding of the GSI experiments. I have, however, attempted to retain the pedagogical flavor of the lectures as they were originally given.
33#
發(fā)表于 2025-3-27 07:19:16 | 只看該作者
34#
發(fā)表于 2025-3-27 11:01:20 | 只看該作者
35#
發(fā)表于 2025-3-27 14:46:45 | 只看該作者
36#
發(fā)表于 2025-3-27 17:50:52 | 只看該作者
37#
發(fā)表于 2025-3-27 23:17:06 | 只看該作者
New QED, the GSI Peaks, and Background Fieldsund electromagnetic fields can induce the phase transition, and we present some new, direct, affirmative evidence that field configurations similar to those in the experiments can lead to spontaneous mass generation.
38#
發(fā)表于 2025-3-28 03:12:43 | 只看該作者
Quantum Electrodynamical Corrections in Critical Fields an . -expansion of the vacuum polarization graph. The dominant effect is provided by the Uehling contribution being visualized by the first diagram on the right hand side. It is linear in the external field and thus of order .(.).
39#
發(fā)表于 2025-3-28 08:42:13 | 只看該作者
40#
發(fā)表于 2025-3-28 11:21:28 | 只看該作者
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