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Titlebook: Anderson Localization and Its Ramifications; Disorder, Phase Cohe Tobias Brandes,S. Kettemann Book 2003 Springer-Verlag Berlin Heidelberg 2

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樓主: industrious
41#
發(fā)表于 2025-3-28 16:00:58 | 只看該作者
Transfer Matrix Studies of Left-Handed Materials,nstituents but by the shape and distribution of specific patterns included in them. They were originally introduced to control the electromagnetic wave propagation [1, 2]. Not only dielectric [1, 2] but also metallic structures [3, 4, 5] were proposed for applications in the microwave and infrared regions.
42#
發(fā)表于 2025-3-28 21:18:37 | 只看該作者
43#
發(fā)表于 2025-3-28 22:56:14 | 只看該作者
44#
發(fā)表于 2025-3-29 05:59:40 | 只看該作者
45#
發(fā)表于 2025-3-29 09:48:20 | 只看該作者
46#
發(fā)表于 2025-3-29 13:03:43 | 只看該作者
Vincent Lai Ming Yip,Munir Pirmohamedssigned to the critical points. For example, due to the divergence of the localisation length ξ(.)∝|.-..}., the width Δ of the longitudinal conductivity peaks emerging at the transitions is expected to exhibit power-law scaling with respect to temperature, system size, or an externally applied frequency.
47#
發(fā)表于 2025-3-29 16:33:15 | 只看該作者
Circumventing Drug Interactions,g nonzero relative angular momenta) at sufficiently low temperatures in a perturbation theory. This becomes an exact statement for dilute enough electron gas, where p-wave pairing (with the relative angular momentum = 1) should arise, as far as the static interaction is concerned [2, 3].
48#
發(fā)表于 2025-3-29 21:49:04 | 只看該作者
Catia Marzolini,Manuel Battegay,David Backso directed to randomly and periodically distorted one-dimensional systems. In one dimension, an infinitesimal amount of disorder (with backscattering contributions) leads to a localized ground state for non-interacting electrons, but with interaction [5] or for special realizations of the disorder [6, 7] this result may change.
49#
發(fā)表于 2025-3-30 02:04:33 | 只看該作者
50#
發(fā)表于 2025-3-30 04:07:37 | 只看該作者
,Superconductivity from the Repulsive Electron Interaction – from 1D to 3D,g nonzero relative angular momenta) at sufficiently low temperatures in a perturbation theory. This becomes an exact statement for dilute enough electron gas, where p-wave pairing (with the relative angular momentum = 1) should arise, as far as the static interaction is concerned [2, 3].
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