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		<title>imported&gt;The Nth User: /* Ring theory */ Made link more specific (i.e., made it a section link)</title>
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		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;Ring theory: &lt;/span&gt; Made link more specific (i.e., made it a section link)&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{inline |date=May 2024}}&lt;br /&gt;
In [[abstract algebra]], the term &amp;#039;&amp;#039;&amp;#039;associator&amp;#039;&amp;#039;&amp;#039; is used in different ways as a measure of the [[associativity|non-associativity]] of an [[algebraic structure]]. Associators are commonly studied as [[triple system]]s.&lt;br /&gt;
&lt;br /&gt;
== Ring theory ==&lt;br /&gt;
&lt;br /&gt;
For a [[non-associative ring]] or [[non-associative algebra|algebra]] &amp;#039;&amp;#039;R&amp;#039;&amp;#039;, the &amp;#039;&amp;#039;&amp;#039;associator&amp;#039;&amp;#039;&amp;#039; is the [[multilinear map]] &amp;lt;math&amp;gt;[\cdot,\cdot,\cdot] : R \times R \times R \to R&amp;lt;/math&amp;gt; given by&lt;br /&gt;
: &amp;lt;math&amp;gt;[x,y,z] = (xy)z - x(yz).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Just as the [[Commutator#Ring theory|commutator]] &lt;br /&gt;
: &amp;lt;math&amp;gt;[x, y] = xy - yx&amp;lt;/math&amp;gt;&lt;br /&gt;
measures the degree of [[commutativity|non-commutativity]], the associator measures the degree of non-associativity of &amp;#039;&amp;#039;R&amp;#039;&amp;#039;.&lt;br /&gt;
For an [[associative ring]] or [[associative algebra|algebra]] the associator is identically zero.&lt;br /&gt;
&lt;br /&gt;
The associator in any ring obeys the identity&lt;br /&gt;
: &amp;lt;math&amp;gt;w[x,y,z] + [w,x,y]z = [wx,y,z] - [w,xy,z] + [w,x,yz].&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The associator is [[alternating form|alternating]] precisely when &amp;#039;&amp;#039;R&amp;#039;&amp;#039; is an [[alternative ring]].&lt;br /&gt;
&lt;br /&gt;
The associator is symmetric in its two rightmost arguments when &amp;#039;&amp;#039;R&amp;#039;&amp;#039; is a [[pre-Lie algebra]].&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;nucleus&amp;#039;&amp;#039;&amp;#039; is the [[set (mathematics)|set]] of elements that associate with all others: that is, the &amp;#039;&amp;#039;n&amp;#039;&amp;#039; in &amp;#039;&amp;#039;R&amp;#039;&amp;#039; such that&lt;br /&gt;
: &amp;lt;math&amp;gt;[n,R,R] = [R,n,R] = [R,R,n] = \{0\} \ .&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The nucleus is an associative subring of &amp;#039;&amp;#039;R&amp;#039;&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
== Quasigroup theory ==&lt;br /&gt;
&lt;br /&gt;
A [[quasigroup]] &amp;#039;&amp;#039;Q&amp;#039;&amp;#039; is a set with a [[binary operation]] &amp;lt;math&amp;gt;\cdot : Q \times Q \to Q&amp;lt;/math&amp;gt; such that for each &amp;#039;&amp;#039;a&amp;#039;&amp;#039;, &amp;#039;&amp;#039;b&amp;#039;&amp;#039; in &amp;#039;&amp;#039;Q&amp;#039;&amp;#039;,&lt;br /&gt;
the equations &amp;lt;math&amp;gt;a \cdot x = b&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;y \cdot a = b&amp;lt;/math&amp;gt; have unique solutions &amp;#039;&amp;#039;x&amp;#039;&amp;#039;, &amp;#039;&amp;#039;y&amp;#039;&amp;#039; in &amp;#039;&amp;#039;Q&amp;#039;&amp;#039;. In a quasigroup &amp;#039;&amp;#039;Q&amp;#039;&amp;#039;, the associator is the map &amp;lt;math&amp;gt;(\cdot,\cdot,\cdot) : Q \times Q \times Q \to Q&amp;lt;/math&amp;gt; defined by the equation&lt;br /&gt;
: &amp;lt;math&amp;gt;(a\cdot b)\cdot c = (a\cdot (b\cdot c))\cdot (a,b,c)&amp;lt;/math&amp;gt;&lt;br /&gt;
for all &amp;#039;&amp;#039;a&amp;#039;&amp;#039;, &amp;#039;&amp;#039;b&amp;#039;&amp;#039;, &amp;#039;&amp;#039;c&amp;#039;&amp;#039; in &amp;#039;&amp;#039;Q&amp;#039;&amp;#039;. As with its ring theory analog, the quasigroup associator is a measure of nonassociativity of &amp;#039;&amp;#039;Q&amp;#039;&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
== Higher-dimensional algebra ==&lt;br /&gt;
&lt;br /&gt;
In [[higher-dimensional algebra]], where there may be non-identity [[morphism]]s between algebraic expressions, an &amp;#039;&amp;#039;&amp;#039;associator&amp;#039;&amp;#039;&amp;#039; is an [[isomorphism]]&lt;br /&gt;
: &amp;lt;math&amp;gt; a_{x,y,z} : (xy)z \mapsto x(yz).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== Category theory ==&lt;br /&gt;
&lt;br /&gt;
In [[category theory]], the associator expresses the associative properties of the internal product [[functor]] in [[monoidal category|monoidal categories]].&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
&lt;br /&gt;
* [[Commutator]]&lt;br /&gt;
* [[Non-associative algebra]]&lt;br /&gt;
* [[Quasi-bialgebra]]&amp;amp;nbsp;– discusses the &amp;#039;&amp;#039;Drinfeld associator&amp;#039;&amp;#039;&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* {{cite journal |title=Identities for the Associator in Alternative Algebras |first1=M. |last1=Bremner |first2=I. |last2=Hentzel |journal=Journal of Symbolic Computation |volume=33 |issue=3 |date=March 2002 |pages=255–273 |doi=10.1006/jsco.2001.0510 |citeseerx=10.1.1.85.1905 }}&lt;br /&gt;
* {{cite book |first=Richard D. |last=Schafer |title=An Introduction to Nonassociative Algebras |url=https://archive.org/details/introductiontono0000scha |url-access=registration |year=1995 |orig-date=1966 |publisher=Dover |isbn=0-486-68813-5 }}&lt;br /&gt;
&lt;br /&gt;
[[Category:Non-associative algebra]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{algebra-stub}}&lt;/div&gt;</summary>
		<author><name>imported&gt;The Nth User</name></author>
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