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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Short description|Phase of matter defined by global structural properties}}&lt;br /&gt;
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{{Quantum matter backlink|Materials}}&lt;br /&gt;
[[Book:Quantum Collection/Matter (by scale)|← Back to Matter by scale]]&lt;br /&gt;
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A &amp;#039;&amp;#039;&amp;#039;topological phase&amp;#039;&amp;#039;&amp;#039; is a [[Physics:Quantum matter/phase|phase]] of [[Physics:Quantum matter/matter|matter]] characterized by global structural properties that remain unchanged under continuous deformations.&lt;br /&gt;
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&amp;lt;div style=&amp;quot;float:right; border:1px solid #e0d890; background:#fff8cc; padding:6px; margin:0 0 1em 1em; width:320px;&amp;quot;&amp;gt;&lt;br /&gt;
[[File:Topological_insulator.png|300px]]&lt;br /&gt;
&amp;lt;div style=&amp;quot;font-size:90%;&amp;quot;&amp;gt;Topological materials exhibit robust edge states determined by global properties.&amp;lt;/div&amp;gt;&lt;br /&gt;
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== Description ==&lt;br /&gt;
Unlike conventional phases, which are defined by local order (such as crystal structure), topological phases are defined by global features of the system. These features are robust against local disturbances.&lt;br /&gt;
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Topological phases can give rise to special states at the boundaries of materials, which remain stable even in the presence of imperfections.&lt;br /&gt;
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== Properties ==&lt;br /&gt;
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* defined by global structure&lt;br /&gt;
* robust against perturbations&lt;br /&gt;
* not characterized by local order&lt;br /&gt;
* linked to [[Physics:Quantum fields/symmetry|symmetry]]&lt;br /&gt;
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=See also=&lt;br /&gt;
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also/Matter}}&lt;br /&gt;
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=References=&lt;br /&gt;
{{reflist|3}}&lt;br /&gt;
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{{Author|Harold Foppele}}&lt;br /&gt;
{{Sourceattribution|Physics:Quantum materials/topological phase|1}}&lt;/div&gt;</summary>
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