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		<title>List of disproved mathematical ideas</title>
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		<summary type="html">&lt;p&gt;81.167.104.3: Removed factual inaccuracy.&lt;/p&gt;
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&lt;div&gt;The &#039;&#039;&#039;topological entanglement entropy&#039;&#039;&#039;{{ref|KitaevPreskill}} {{ref|LevinWen}}, usually denoted by &#039;&#039;γ&#039;&#039;, is a number characterizing many-body states that possess [[topological order]].  &lt;br /&gt;
The short form  &#039;&#039;topological entropy&#039;&#039; is often used, although the same name in [[ergodic theory]] refers to an unrelated mathematical concept (see [[topological entropy]]).&lt;br /&gt;
&lt;br /&gt;
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 &lt;br /&gt;
long range quantum entanglements.&lt;br /&gt;
&lt;br /&gt;
Given a [[topological order|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 &#039;&#039;L&#039;&#039;, within an infinite two-dimensional topologically ordered state, has the following form for large &#039;&#039;L&#039;&#039;:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; S_L \; \longrightarrow \; \alpha L -\gamma +\mathcal{O}(L^{-\nu}) \; , \qquad  \nu&amp;gt;0 \,\!&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&#039;&#039;-γ&#039;&#039; is the topological entanglement entropy.&lt;br /&gt;
&lt;br /&gt;
The topological entanglement entropy is equal to the logarithm of the total [[quantum dimension]] of the quasiparticle excitations of the state.  &lt;br /&gt;
&lt;br /&gt;
For example, the simplest fractional quantum Hall states, the Laughlin states at filling fraction 1/&#039;&#039;m&#039;&#039;, have &#039;&#039;γ&#039;&#039; = ½log(&#039;&#039;m&#039;&#039;).  The &#039;&#039;Z&#039;&#039;&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; fractionalized states, such as topologically ordered states of &lt;br /&gt;
&#039;&#039;Z&#039;&#039;&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt; spin-liquid, [[quantum dimer models]] on non-bipartite lattices, and Kitaev&#039;s [[toric code]] state, are characterized &#039;&#039;γ&#039;&#039; = log(2).&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
&lt;br /&gt;
*[[Quantum topology]]&lt;br /&gt;
*[[Topological defect]]&lt;br /&gt;
*[[Topological order]]&lt;br /&gt;
*[[Topological quantum field theory]]&lt;br /&gt;
*[[Topological quantum number]]&lt;br /&gt;
*[[Topological string theory]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
{{Nofootnotes|date=April 2008}}&lt;br /&gt;
===Introduction of the measure===&lt;br /&gt;
#{{note|KitaevPreskill}} Topological Entanglement Entropy, Alexei Kitaev and John Preskill, [http://link.aps.org/abstract/PRL/v96/e110404  Phys. Rev. Lett. &#039;&#039;&#039;96&#039;&#039;&#039;, 110404 (2006)].&lt;br /&gt;
#{{note|LevinWen}} Detecting Topological Order in a Ground State Wave Function, Michael Levin and Xiao-Gang Wen,  [http://link.aps.org/abstract/PRL/v96/e110405 Phys. Rev. Lett. &#039;&#039;&#039;96&#039;&#039;&#039;, 110405 (2006)].&lt;br /&gt;
&lt;br /&gt;
===Calculations for specific topologically ordered states===&lt;br /&gt;
&lt;br /&gt;
* M. Haque, O. Zozulya and K. Schoutens; Phys. Rev. Lett. &#039;&#039;&#039;98&#039;&#039;&#039;, 060401 (2007).&lt;br /&gt;
* S. Furukawa and G. Misguich, Phys. Rev. B &#039;&#039;&#039;75&#039;&#039;&#039;, 214407 (2007).&lt;br /&gt;
&lt;br /&gt;
{{physics-stub}}&lt;br /&gt;
[[Category:Condensed matter physics]]&lt;br /&gt;
[[Category:Statistical mechanics]]&lt;/div&gt;</summary>
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