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{{for|the concept of triality in linguistics|Grammatical number#Trial}}
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[[Image:Dynkin diagram D4.png|133px|right|thumb|The automorphisms of the Dynkin diagram D<sub>4</sub> give rise to triality in Spin(8).]]
In [[mathematics]], '''triality''' 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<sub>4</sub> and the associated [[Lie group|Lie]] [[Group (mathematics)|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]].
 
Of all [[simple Lie group]]s, Spin(8) has the most symmetrical [[Dynkin diagram]], D<sub>4</sub>. 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]] ''S''<sub>3</sub> which acts by permuting the three legs. This gives rise to an ''S''<sub>3</sub> group of outer automorphisms of Spin(8). This [[automorphism group]] permutes the three 8-dimensional [[irreducible representation]]s of Spin(8); these being the [[vector (geometric)|vector]] representation and two [[chirality (mathematics)|chiral]] [[spin representation]]s. These automorphisms do not project to automorphisms of SO(8). The vector representation – the natural action of SO(8) (hence Spin(8)) on <math>K^8</math> – is also known as the "defining module", while the chiral spin representations are also known as "half-spin representations", and all three of these are [[fundamental representation]]s.
 
No other Dynkin diagram has an automorphism group of order greater than 2; for other D<sub>''n''</sub> (corresponding to other even Spin groups, Spin(2''n'')), there is still the automorphism corresponding to switching the two half-spin representations, but these are not isomorphic to the vector representation.
 
Roughly speaking, symmetries of the Dynkin diagram lead to automorphisms of the [[Bruhat-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 "geometric triality".
 
The exceptional 3-fold symmetry of the <math>D_4</math> diagram also gives rise to the [[Steinberg group (Lie theory)|Steinberg group]] [[³D₄]].
 
==General formulation==
 
A duality between two vector spaces over a field '''F''' is a [[nondegenerate]] [[bilinear map]]
:<math> V_1\times V_2\to \mathbb F,</math>
i.e., for each nonzero vector ''v'' in one of the two vector spaces, the pairing with ''v'' is a nonzero [[linear functional]] on the other.
 
Similarly, a triality between three vector spaces over a field '''F''' is a nondegenerate [[multilinear map|trilinear map]]
:<math> V_1\times V_2\times V_3\to \mathbb F,</math>
i.e., each nonzero vector in one of the three vector spaces induces a duality between the other two.
 
By choosing vectors ''e''<sub>''i''</sub> in each ''V''<sub>''i''</sub> on which the trilinear map 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 ''V'', the triality may be reexpressed as a bilinear multiplication
:<math> V \times V \to V</math>
where each ''e''<sub>''i''</sub> corresponds to the identity element in ''V''. The nondegeneracy condition now implies that ''V'' is a [[division algebra]]. It follows that ''V'' has dimension 1, 2, 4 or 8. If further '''F'''&nbsp;=&nbsp;'''R''' and the identification of ''V'' with its dual is given  by positive definite inner product, ''V'' is a [[normed division algebra]], and is therefore isomorphic to '''R''', '''C''', '''H''' or&nbsp;'''O'''.
 
Conversely, the normed division algebras immediately give rise to trialities by taking each ''V''<sub>''i''</sub> equal to the division algebra, and using the inner product on the algebra to dualize the multiplication into a trilinear form.
 
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).
 
==References==
 
* [[John Frank Adams]] (1981), ''Spin(8), Triality, F<sub>4</sub> and all that'', in "Superspace and supergravity", edited by Stephen Hawking and Martin Roček, Cambridge University Press, pages 435&ndash;445.
* [[John Frank Adams]] (1996), ''Lectures on Exceptional Lie Groups'' (Chicago Lectures in Mathematics), edited by Zafer Mahmud and Mamora Mimura, University of Chicago Press, ISBN 0-226-00527-5.
 
==External links==
*[http://math.ucr.edu/home/baez/octonions/node7.html Spinors and Trialities] by John Baez
*[http://homepages.wmich.edu/~drichter/zometriality.htm Triality with Zometool] by David Richter
 
 
 
[[Category:Lie groups]]
[[Category:Spinors]]

Latest revision as of 23:52, 25 September 2014

The author is recognized by the title of Numbers Lint. Playing baseball is the hobby he will by no means stop doing. Years ago we moved to North Dakota and I adore each day living here. My working day occupation is a librarian.

Here is my web blog - meal delivery service (continue reading this..)