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Titlebook: Critical Phenomena in Loop Models; Adam Nahum Book 2015 Springer International Publishing Switzerland 2015 CP^{n-1} Model.Completely-packe

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11#
發(fā)表于 2025-3-23 13:30:59 | 只看該作者
https://doi.org/10.1007/978-3-663-02783-6The loop models at . have the special property that the nodes are uncorrelated (in the absence of the extra interaction described in the previous chapter) so that the critical behaviour is purely geometrical.
12#
發(fā)表于 2025-3-23 15:32:47 | 只看該作者
13#
發(fā)表于 2025-3-23 18:06:03 | 只看該作者
14#
發(fā)表于 2025-3-24 01:57:01 | 只看該作者
15#
發(fā)表于 2025-3-24 03:03:01 | 只看該作者
16#
發(fā)表于 2025-3-24 09:54:36 | 只看該作者
Completely Packed Loop Models,We begin with a class of three-dimensional loop models that show transitions between two types of phase—one with infinite loops, and one with only short loops.
17#
發(fā)表于 2025-3-24 13:36:18 | 只看該作者
Topological Terms, Quantum Magnets and Deconfined Criticality,We saw in the previous chapter that the completely-packed loop models are described by lattice magnets in which the Boltzmann weight is generically complex.
18#
發(fā)表于 2025-3-24 16:15:45 | 只看該作者
The Statistics of Vortex Lines,The loop models at . have the special property that the nodes are uncorrelated (in the absence of the extra interaction described in the previous chapter) so that the critical behaviour is purely geometrical.
19#
發(fā)表于 2025-3-24 20:39:32 | 只看該作者
Loop Models with Crossings in 2D,It is tempting to think that two-dimensional critical phenomena are completely classified and understood, thanks to conformal field theory and other exact techniques, but this is far from true.
20#
發(fā)表于 2025-3-24 23:26:17 | 只看該作者
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