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Titlebook: Dispersion Forces I; Macroscopic Quantum Stefan Yoshi Buhmann Book 2012 Springer-Verlag Berlin Heidelberg 2012 Atom-field interactions.Ato

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21#
發(fā)表于 2025-3-25 04:05:57 | 只看該作者
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發(fā)表于 2025-3-25 10:28:32 | 只看該作者
The Beginnings of Cancer in the Cellrnatively, the Lorentz force can be expressed in terms of the Maxwell stress tensor whose quantum average leads to a surface-integral form of the Casimir force. Its use is illustrated by calculating the force between two perfectly reflecting or magnetoelectric parallel plates.
23#
發(fā)表于 2025-3-25 12:32:10 | 只看該作者
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發(fā)表于 2025-3-25 19:40:23 | 只看該作者
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發(fā)表于 2025-3-25 20:35:49 | 只看該作者
Introduction: Dispersion Forces,naming conventions are discussed. The relevance of these forces in various fields of science is pointed out. An overview is given to the different approaches and methods for calculating and measuring van der Waals, Casimir–Polder and Casimir forces.
26#
發(fā)表于 2025-3-26 03:20:04 | 只看該作者
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發(fā)表于 2025-3-26 06:57:43 | 只看該作者
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發(fā)表于 2025-3-26 11:30:04 | 只看該作者
,Casimir–Polder Forces on Ground-State Atoms,lar coupling schemes show that the potential of an electric atom in an arbitrary arrangement of magnetoelectric bodies can be given in terms of the atomic polarisability and the classical Green’s tensor. The results are extended to magnetic atoms where the magnetisability plays a crucial role. The C
29#
發(fā)表于 2025-3-26 14:52:49 | 只看該作者
Van der Waals Forces Between Ground-State Atoms,e aid of Feynman diagrams, the interaction is shown to depend on the classical Green’s tensor as well as the polarisabilities of the atoms. The calculation is extended to the magnetoelectric case by including all possible combinations of electric, para- and diamagnetic atoms. After discussing the va
30#
發(fā)表于 2025-3-26 16:52:41 | 只看該作者
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