有灵感
发表于 2025-3-21 19:40:58
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consent
发表于 2025-3-21 22:12:09
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细菌等
发表于 2025-3-22 04:05:41
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新娘
发表于 2025-3-22 06:00:13
Dirk Husmeier PhDt this can actually only be the case at . = ., at any finite temperature the ions will be deflected from their equilibrium positions and at a given time . there will be no periodic potential anymore. The consequences of this are to be examined in this chapter.
commensurate
发表于 2025-3-22 09:12:35
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FANG
发表于 2025-3-22 14:06:19
Dirk Husmeier PhDon in one dimension; Monte Carlo methods are also introduced and results are presented. Finally, band magnetism is discussed and the Stoner theory of band magnetism is derived from the Hubbard model in a mean field approximation. The giant magnetoresistance (GMR) effect is explained as a current app
phytochemicals
发表于 2025-3-22 18:22:13
Dirk Husmeier PhDic field to matter in a perturbative way, Rabi oscillations and the optical Stark effect are treated. The semiconductor Bloch equations for the occupation probabilities and the polarization taking into account the Coulomb interaction between the electrons (or between the electrons in the conduction
ALB
发表于 2025-3-22 22:01:56
Dirk Husmeier PhD spin-orbit coupling on surface states is treated. In this context the class of the recently detected topological insulators, materials of significant importance for spin electronics, are discussed. Particular emphasis, hereby, is laid on the new type of topologically protected surface states with w
吹牛大王
发表于 2025-3-23 05:27:07
Dirk Husmeier PhDelopment of a detailed understanding of the surface electronic structure. On the theoretical side, the general approach is similar to that for the bulk crystal: In essence the one-electron approximation is used and one tries to solve the Schrödinger equation for an electron near the surface. A varie
obligation
发表于 2025-3-23 09:18:49
Dirk Husmeier PhDms per cm. must be studied against the background of about 10. atoms present in a bulk volume of one cm.. In surface and interface physics the appropriate geometry for a scattering experiment is thus the reflection geometry. Furthermore, only particles that do not penetrate too deeply into the solid