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・ Topological Boolean algebra
・ Topological category
・ Topological censorship
・ Topological combinatorics
・ Topological complexity
・ Topological conjugacy
・ Topological data analysis
・ Topological defect
・ Topological degeneracy
・ Topological degree theory
・ Topological derivative
・ Topological divisor of zero
・ Topological drugs
・ Topological dynamics
・ Topological entropy
Topological entropy in physics
・ Topological excitations
・ Topological fluid dynamics
・ Topological functioning model
・ Topological game
・ Topological graph
・ Topological graph theory
・ Topological group
・ Topological half-exact functor
・ Topological index
・ Topological indistinguishability
・ Topological insulator
・ Topological K-theory
・ Topological manifold
・ Topological map


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Topological entropy in physics : ウィキペディア英語版
Topological entropy in physics
The topological entanglement entropy , usually denoted by ''γ'', is a number characterizing many-body states that possess topological order.
The short form ''topological entropy'' is often used, although the same name in ergodic theory refers to an unrelated mathematical concept (see topological entropy).
A non-zero topological entanglement entropy reflects the presence of long range quantum entanglements in a many-body quantum state. So the topological entanglement entropy links topological order with pattern of
long range quantum entanglements.
Given a topologically ordered state, the topological entropy can be extracted from the asymptotic behavior of the Von Neumann entropy measuring the quantum entanglement between a spatial block and the rest of the system. The entanglement entropy of a simply connected region of boundary length ''L'', within an infinite two-dimensional topologically ordered state, has the following form for large ''L'':
: S_L \; \longrightarrow \; \alpha L -\gamma +\mathcal(L^) \; , \qquad \nu>0 \,\!
''-γ'' is the topological entanglement entropy.
The topological entanglement entropy is equal to the logarithm of the total quantum dimension of the quasiparticle excitations of the state.
For example, the simplest fractional quantum Hall states, the Laughlin states at filling fraction 1/''m'', have ''γ'' = ½log(''m''). The ''Z''2 fractionalized states, such as topologically ordered states of
''Z''2 spin-liquid, quantum dimer models on non-bipartite lattices, and Kitaev's toric code state, are characterized ''γ'' = log(2).
==See also==

*Quantum topology
*Topological defect
*Topological order
*Topological quantum field theory
*Topological quantum number
*Topological string theory

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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