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Titlebook: Correlation Effects in Low-Dimensional Electron Systems; Proceedings of the 1 Ayao Okiji,Norio Kawakami Conference proceedings 1994 Springe

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樓主: Weber-test
21#
發(fā)表于 2025-3-25 04:27:06 | 只看該作者
Melina Aparici,Elisa Rosado,Joan Pereratum group structure, and the interpretation of the model as the generalization of an ideal gas (of “spinons”) to the case of .. Some recent results on its dynamical correlation function are discussed, and conjectured extensions of these remarkably simple results to the .(.) model, and to the related
22#
發(fā)表于 2025-3-25 10:00:15 | 只看該作者
Shengnan Zhao,Jun Ma,Chaoran Cuihe problem is analyzed in terms of random matrices and of the evolution of their eigenvalues under changes of parameters. The robustness of bulk space-time correlations of a many particle system to changing boundary conditions is suggested to be at the root of the universality. The explicit density-
23#
發(fā)表于 2025-3-25 15:35:53 | 只看該作者
24#
發(fā)表于 2025-3-25 16:16:21 | 只看該作者
Zeitlichkeit und Fleischlichkeitactional quantum Hall effect (FQHE). Under the chiral constraint the model describes characteristic properties of edge states for the FQHE. In particular the excitation spectrum is classified in terms of the topological-order matrix of the FQHE.
25#
發(fā)表于 2025-3-25 20:54:04 | 只看該作者
26#
發(fā)表于 2025-3-26 01:45:47 | 只看該作者
27#
發(fā)表于 2025-3-26 04:38:20 | 只看該作者
28#
發(fā)表于 2025-3-26 12:09:39 | 只看該作者
Zeitlichkeit und Fleischlichkeit the Kondo problem: the ordinary Anderson model, the orbitally degenerate Anderson model and the multi-channel Kondo model. The calculations for the multi-channel Kondo model are further extended to the case at finite temperatures by means of Yang and Yang’s method developed in one-dimensional inter
29#
發(fā)表于 2025-3-26 13:41:09 | 只看該作者
30#
發(fā)表于 2025-3-26 18:24:15 | 只看該作者
Individuierung als ?Trieb“ und Affekttate has been studied extensively but it does not have spin-charge separation explicitly. On the other hand, another type of variational wave function is considered, which has the spin-charge separation and is easy to extend to higher dimensions. This trial state has spinless fermions as the charge
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