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Titlebook: Strategische Führungsinformationssysteme; Theoretische Grundla Ulrich Grimm (Professor für ABWL, Vorstandsvorsitz Book 1995 Betriebswirtsch

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發(fā)表于 2025-3-25 06:03:29 | 只看該作者
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發(fā)表于 2025-3-25 09:43:21 | 只看該作者
23#
發(fā)表于 2025-3-25 15:25:57 | 只看該作者
Erich Christian von Kimakowitzkey to explaining excessive charged particle production, recently observed at the Large Hadron Collider. Furthermore, the analyses at finite baryon density indicate that the energy available for QGP production is larger than the amount conventionally assumed. .978-4-431-56188-0978-4-431-54798-3Series ISSN 2190-5053 Series E-ISSN 2190-5061
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發(fā)表于 2025-3-26 03:06:20 | 只看該作者
does not need to invoke quantum mechanics and the correspondence pr- ciple in order to exclude the unphysical solutions (runaway and pre-acc- eration solutions). Rather, as he discovered, the derivation of the classical equations of motion from the Maxwell-Lorentz equations is invalid when the time rate of ch978-0-387-73967-0Series ISSN 0940-7677
27#
發(fā)表于 2025-3-26 07:58:05 | 只看該作者
Armin Birkenbeullized to obtain a nonzero bare mass and consistent force and power equations of motion. By looking at the Lorentz model of the electron as a charged insulator, general expressions are . for the binding forces that Poincaré . to hold the charge distribution together. A careful examination of the clas
28#
發(fā)表于 2025-3-26 08:40:52 | 只看該作者
Angelika Kreitellized to obtain a nonzero bare mass and consistent force and power equations of motion. By looking at the Lorentz model of the electron as a charged insulator, general expressions are . for the binding forces that Poincaré . to hold the charge distribution together. A careful examination of the clas
29#
發(fā)表于 2025-3-26 16:03:57 | 只看該作者
30#
發(fā)表于 2025-3-26 20:00:23 | 只看該作者
e of the redefined stress-momentum-energy tensors recover the secondary binding forces necessary to hold the accelerating charge to the surface of the insulator. Thus, redefining the electromagnetic momentum-energy seems an unattractive alternative to the deterministic binding forces, bare mass, and
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