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Titlebook: Advances in Solid State Physics; Bernhard Kramer Book 2003 Springer-Verlag Berlin Heidelberg 2003 condensed matter.condensed matter physic

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樓主: Gullet
31#
發(fā)表于 2025-3-26 21:14:26 | 只看該作者
32#
發(fā)表于 2025-3-27 04:58:31 | 只看該作者
Advances in Information Security phase coherence time extracted from the weak antilocalisation shows a pronounced plateau in a temperature region of . mK - . mK, associated with the phase breaking due to the Kondo effect. Below the Kondo temperature, the phase coherence time increases, as expected in the framework of Kondo physics
33#
發(fā)表于 2025-3-27 08:14:29 | 只看該作者
34#
發(fā)表于 2025-3-27 09:43:15 | 只看該作者
https://doi.org/10.1007/0-387-34188-9 we review recent reports on the occurrence of magnetic-field-driven metal-insulator and insulator-metal transitions, as well as the quantum Hall effect (QHE) in graphite. The experimental results suggest that the low field (~ 1 kOe) metal-insulator transition is associated with the transition betwe
35#
發(fā)表于 2025-3-27 15:55:35 | 只看該作者
Advances in Information Securitycopic conductors. Experiments on resistive quantum wires show that the non-equilibrium quasiparticle distribution function f(E,V) as a function of the quasiparticle energy . approximately obeys the scaling property, f(E,V) = f(E/V), if the transport voltage . exceeds a certain crossover scale V^*. T
36#
發(fā)表于 2025-3-27 20:15:56 | 只看該作者
37#
發(fā)表于 2025-3-27 23:04:50 | 只看該作者
https://doi.org/10.1007/0-387-34188-9ements, however, suffer from the missing momentum resolution in the strongly anisotropic CuO. plane. The problem can be partially solved by using electronic Raman scattering. Here, the response is proportional to the conductivity. Additionally, different parts of the Fermi surface can be projected o
38#
發(fā)表于 2025-3-28 02:26:35 | 只看該作者
39#
發(fā)表于 2025-3-28 09:11:30 | 只看該作者
Advances in Solid State Physics978-3-540-44838-9Series ISSN 1438-4329 Series E-ISSN 1617-5034
40#
發(fā)表于 2025-3-28 11:33:56 | 只看該作者
Walter R. Nelson,Theodore M. Jenkinsiption of electronic states in a tight-binding model and in an effective-mass or k.p scheme. Transport properties are discussed including absence of backward scattering except for scatterers with a potential range smaller than the lattice constant and its extension to multi-bands cases.
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