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		<title>Triality</title>
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		<summary type="html">&lt;p&gt;2601:152:202:6D10:9981:FAC9:98A2:BC74: /* General formulation */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Short description|Relationship between certain vector spaces}}&lt;br /&gt;
{{for|the concept of triality in linguistics|Grammatical number#Trial}}&lt;br /&gt;
{{no footnotes|date=July 2017}}&lt;br /&gt;
[[Image:Dynkin diagram D4.png|133px|right|thumb|The automorphisms of the Dynkin diagram D&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; give rise to triality in Spin(8).]]&lt;br /&gt;
In [[mathematics]], &#039;&#039;&#039;triality&#039;&#039;&#039; is a relationship among three [[vector space]]s, analogous to the [[duality (mathematics)|duality]] relation between [[dual vector space]]s. Most commonly, it describes those special features of the [[Dynkin diagram]] D&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and the associated [[Lie group]] [[Spin(8)]], the [[Double covering group|double cover]] of 8-dimensional rotation group [[SO(8)]], arising because the group has an [[outer automorphism]] of order three. There is a geometrical version of triality, analogous to [[Duality (projective geometry)|duality in projective geometry]].&lt;br /&gt;
&lt;br /&gt;
Of all [[simple Lie group]]s, Spin(8) has the most symmetrical Dynkin diagram, D&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;. The diagram has four nodes with one node located at the center, and the other three attached symmetrically. The [[symmetry group]] of the diagram is the [[symmetric group]] &#039;&#039;S&#039;&#039;&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; which acts by permuting the three legs. This gives rise to an &#039;&#039;S&#039;&#039;&amp;lt;sub&amp;gt;3&amp;lt;/sub&amp;gt; group of outer automorphisms of Spin(8). This [[automorphism group]] permutes the three 8-dimensional [[irreducible representation]]s of Spin(8); these being the &#039;&#039;vector&#039;&#039; representation and two [[chirality (mathematics)|chiral]] &#039;&#039;spin&#039;&#039; representations. These automorphisms do not project to automorphisms of SO(8). The vector representation—the natural action of SO(8) (hence Spin(8)) on {{math|&#039;&#039;F&#039;&#039;&amp;lt;sup&amp;gt;8&amp;lt;/sup&amp;gt;}}—consists over the real numbers of [[Euclidean space|Euclidean 8-vectors]] and is generally known as the &amp;quot;defining module&amp;quot;, while the chiral spin representations are also known as [[spinor|&amp;quot;half-spin representations&amp;quot;]], and all three of these are [[fundamental representation]]s.&lt;br /&gt;
&lt;br /&gt;
No other connected Dynkin diagram has an automorphism group of order greater than 2; for other D&amp;lt;sub&amp;gt;&#039;&#039;n&#039;&#039;&amp;lt;/sub&amp;gt; (corresponding to other even Spin groups, Spin(2&#039;&#039;n&#039;&#039;)), there is still the automorphism corresponding to switching the two half-spin representations, but these are not isomorphic to the vector representation.&lt;br /&gt;
&lt;br /&gt;
Roughly speaking, symmetries of the Dynkin diagram lead to automorphisms of the [[Tits building]] associated with the group.  For [[special linear group]]s, one obtains projective duality.  For Spin(8), one finds a curious phenomenon involving 1-, 2-, and 4-dimensional subspaces of 8-dimensional space, historically known as &amp;quot;geometric triality&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
The exceptional 3-fold symmetry of the D&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; diagram also gives rise to the [[Steinberg group (Lie theory)|Steinberg group]] [[3D4|&amp;lt;sup&amp;gt;3&amp;lt;/sup&amp;gt;D&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt;]].&lt;br /&gt;
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==General formulation==&lt;br /&gt;
&lt;br /&gt;
A duality between two vector spaces over a field {{mvar|F}} is a non-degenerate [[bilinear form]]&lt;br /&gt;
:&amp;lt;math&amp;gt; V_1\times V_2\to F,&amp;lt;/math&amp;gt;&lt;br /&gt;
i.e., for each non-zero vector {{mvar|v}} in one of the two vector spaces, the pairing with {{mvar|v}} is a non-zero [[linear functional]] on the other.&lt;br /&gt;
&lt;br /&gt;
Similarly, a triality between three vector spaces over a field {{mvar|F}} is a non-degenerate [[multilinear form|trilinear form]]&lt;br /&gt;
:&amp;lt;math&amp;gt; V_1\times V_2\times V_3\to F,&amp;lt;/math&amp;gt;&lt;br /&gt;
i.e., each non-zero vector in one of the three vector spaces induces a duality between the other two.&lt;br /&gt;
&lt;br /&gt;
By choosing vectors {{math|&#039;&#039;e&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;i&#039;&#039;&amp;lt;/sub&amp;gt;}} in each {{math|&#039;&#039;V&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;i&#039;&#039;&amp;lt;/sub&amp;gt;}} on which the trilinear form evaluates to 1, we find that the three vector spaces are all [[isomorphism|isomorphic]] to each other, and to their duals. Denoting this common vector space by {{mvar|V}}, the triality may be re-expressed as a [[algebra over a field|bilinear multiplication]]&lt;br /&gt;
:&amp;lt;math&amp;gt; V \times V \to V&amp;lt;/math&amp;gt;&lt;br /&gt;
where each {{math|&#039;&#039;e&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;i&#039;&#039;&amp;lt;/sub&amp;gt;}} corresponds to the identity element in {{mvar|V}}. The non-degeneracy condition now implies that {{mvar|V}} is a [[composition algebra]]. It follows that {{mvar|V}} has dimension 1, 2, 4 or 8. If further {{math|1=&#039;&#039;F&#039;&#039; = [[real number|&#039;&#039;&#039;R&#039;&#039;&#039;]]}} and the form used to identify {{mvar|V}} with its dual is [[definite quadratic form|positive definite]], then {{mvar|V}} is a [[Hurwitz&#039;s theorem (composition algebras)|Euclidean Hurwitz algebra]], and is therefore isomorphic to [[real numbers|&#039;&#039;&#039;R&#039;&#039;&#039;]], [[complex numbers|&#039;&#039;&#039;C&#039;&#039;&#039;]], [[quaternions|&#039;&#039;&#039;H&#039;&#039;&#039;]] or&amp;amp;nbsp;[[octonions|&#039;&#039;&#039;O&#039;&#039;&#039;]].&lt;br /&gt;
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Conversely, composition algebras immediately give rise to trialities by taking each {{math|&#039;&#039;V&#039;&#039;&amp;lt;sub&amp;gt;&#039;&#039;i&#039;&#039;&amp;lt;/sub&amp;gt;}} equal to the algebra, and [[tensor contraction|contracting]] the multiplication with the inner product on the algebra to make a trilinear form.&lt;br /&gt;
&lt;br /&gt;
An alternative construction of trialities uses spinors in dimensions 1, 2, 4 and 8. The eight-dimensional case corresponds to the triality property of Spin(8).&lt;br /&gt;
&lt;br /&gt;
== See also ==&lt;br /&gt;
* [[Triple product]], may be related to the 4-dimensional triality (on [[quaternion]]s)&lt;br /&gt;
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==References==&lt;br /&gt;
&lt;br /&gt;
* [[John Frank Adams]] (1981), &#039;&#039;Spin(8), Triality, F&amp;lt;sub&amp;gt;4&amp;lt;/sub&amp;gt; and all that&#039;&#039;, in &amp;quot;Superspace and supergravity&amp;quot;, edited by Stephen Hawking and Martin Roček, Cambridge University Press, pages 435&amp;amp;ndash;445.&lt;br /&gt;
* [[John Frank Adams]] (1996), &#039;&#039;Lectures on Exceptional Lie Groups&#039;&#039; (Chicago Lectures in Mathematics), edited by Zafer Mahmud and Mamora Mimura, University of Chicago Press, {{isbn|0-226-00527-5}}.&lt;br /&gt;
&lt;br /&gt;
==Further reading==&lt;br /&gt;
* {{cite book | last1=Knus | first1=Max-Albert | last2=Merkurjev | first2=Alexander | author2-link=Alexander Merkurjev | last3=Rost | first3=Markus | author3-link=Markus Rost | last4=Tignol | first4=Jean-Pierre| author-link4=Jean-Pierre Tignol  | title=The book of involutions | others=With a preface by J. Tits | zbl=0955.16001 | series=Colloquium Publications | publisher=[[American Mathematical Society]] | volume=44 | location=Providence, RI | year=1998 | isbn=0-8218-0904-0 }}&lt;br /&gt;
* {{cite book | title=The Finite Simple Groups | volume=251 | series=[[Graduate Texts in Mathematics]] | first=Robert | last=Wilson | authorlink=Robert Arnott Wilson | publisher=[[Springer-Verlag]] | year=2009 | isbn=978-1-84800-987-5 | zbl=1203.20012 }}&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
*[http://math.ucr.edu/home/baez/octonions/node7.html Spinors and Trialities] by John Baez&lt;br /&gt;
*[http://homepages.wmich.edu/~drichter/zometriality.htm Triality with Zometool] by David Richter&lt;br /&gt;
&lt;br /&gt;
[[Category:Lie groups]]&lt;br /&gt;
[[Category:Spinors]]&lt;/div&gt;</summary>
		<author><name>2601:152:202:6D10:9981:FAC9:98A2:BC74</name></author>
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