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In [[mathematics]], a '''Young symmetrizer''' is an element of the  [[group ring|group algebra]] of the [[symmetric group]], constructed in such a way that the image of the element corresponds to an [[irreducible representation]] of the symmetric group over the [[complex number]]s. A similar construction works over any field, and the resulting representations are called '''[[Specht module]]s'''. The Young symmetrizer is named after British mathematician [[Alfred Young]].
== 'Get out ==


==Definition==
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Given a finite symmetric group ''S''<sub>''n''</sub> and specific [[Young tableau]] λ corresponding to a numbered partition of ''n'', define two [[permutation group|permutation subgroups]] <math>P_\lambda</math> and <math>Q_\lambda</math> of ''S''<sub>''n''</sub> as follows:
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<ul>
:<math>P_\lambda=\{ g\in S_n : g \text{ preserves each row of } \lambda \}</math>
 
 
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and
 
 
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:<math>Q_\lambda=\{ g\in S_n : g \text{ preserves each column of } \lambda \}.</math>
 
 
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Corresponding to these two subgroups, define two vectors in the [[group algebra]] <math>\mathbb{C}S_n</math> as
 
 
</ul>
:<math>a_\lambda=\sum_{g\in P_\lambda} e_g</math>
 
and
 
:<math>b_\lambda=\sum_{g\in Q_\lambda} \sgn(g) e_g</math>
 
where <math>e_g</math> is the unit vector corresponding to ''g'', and <math>\sgn(g)</math> is the signature of the permutation. The product
 
:<math>c_\lambda := a_\lambda b_\lambda = \sum_{g\in P_\lambda,h\in Q_\lambda} \sgn(h) e_{gh}</math>
 
is the '''Young symmetrizer''' corresponding to the [[Young tableau]] λ. Each Young symmetrizer corresponds to an irreducible representation of the symmetric group, and every irreducible representation can be obtained from a corresponding Young symmetrizer. (If we replace the [[complex number]]s by more general [[field (mathematics)|field]]s the corresponding representations will not be irreducible in general.)
 
==Construction==
Let ''V'' be any [[vector space]] over the [[complex number]]s. Consider then the [[tensor product]] vector space <math>V^{\otimes n}=V \otimes V \otimes \cdots \otimes V</math> (''n'' times). Let ''S''<sub>n</sub> act on this tensor product space by permuting the indices. One then has a natural [[group ring|group algebra]] representation  <math>\mathbb{C}S_n \rightarrow \text{End} (V^{\otimes n})</math> on <math>V^{\otimes n}</math>.
 
Given a partition λ of ''n'', so that <math>n=\lambda_1+\lambda_2+ \cdots +\lambda_j</math>, then the [[image (mathematics)|image]] of <math>a_\lambda</math> is
:<math>\text{Im}(a_\lambda) := a_\lambda V^{\otimes n} \cong
\text{Sym}^{\lambda_1}\; V \otimes
\text{Sym}^{\lambda_2}\; V \otimes \cdots \otimes
\text{Sym}^{\lambda_j}\; V.
</math>
 
For instance, if <math>n =4</math>, and <math>\lambda = (2,2)</math>, with the canonical Young tableau <math>\{\{1,2\},\{3,4\}\}</math>. Then the corresponding <math>a_\lambda</math> is given by <math> a_\lambda = e_{\text{id}} + e_{(1,2)} + e_{(3,4)} + e_{(1,2)(3,4)}</math>. Let an element in <math>V^{\otimes 4}</math> be given by <math>v_{1,2,3,4}:=v_1 \otimes v_2 \otimes v_3 \otimes v_4</math>. Then
:<math> a_\lambda v_{1,2,3,4} = v_{1,2,3,4} + v_{2,1,3,4} + v_{1,2,4,3} + v_{2,1,4,3} = (v_1 \otimes v_2 + v_2 \otimes v_1) \otimes (v_3 \otimes v_4 + v_4 \otimes v_3). </math>
The latter clearly span <math> \text{Sym}^2\; V\otimes \text{Sym}^2\; V</math>.  
 
The image of <math>b_\lambda</math> is
:<math>\text{Im}(b_\lambda) \cong
\bigwedge^{\mu_1} V \otimes
\bigwedge^{\mu_2} V \otimes \cdots \otimes
\bigwedge^{\mu_k} V
</math>
where μ is the conjugate partition to λ. Here, <math>\text{Sym}^i V </math> and <math>\bigwedge^j V</math> are the [[symmetric algebra|symmetric]] and [[exterior algebra|alternating tensor product spaces]].  
 
The image <math>\mathbb{C}S_nc_\lambda</math> of <math>c_\lambda = a_\lambda \cdot b_\lambda</math> in <math>\mathbb{C}S_n</math> is an irreducible representation<ref>See {{harv|Fulton|Harris|1991|loc=Theorem 4.3, p. 46}}</ref> of ''S''<sub>n</sub>, called a [[Specht module]]. We write
:<math>\text{Im}(c_\lambda) = V_\lambda</math>  
for the irreducible representation.
 
Some scalar multiple of <math>c_\lambda</math> is idempotent, that is  <math>c^2_\lambda = \alpha_\lambda c_\lambda</math> for some rational number <math>\alpha_\lambda\in\mathbb{Q}</math>. Specifically, one finds <math>\alpha_\lambda=n! / \text{dim } V_\lambda</math>. In particular, this implies that representations of the symmetric group can be defined over the rational numbers; that is, over the rational group algebra <math>\mathbb{Q}S_n</math>.
 
Consider, for example, ''S''<sub>3</sub> and the partition (2,1). Then one has <math>c_{(2,1)} = e_{123}+e_{213}-e_{321}-e_{312}</math>
 
If ''V'' is a complex vector space, then
the images of <math>c_\lambda</math> on spaces <math>V^{\otimes d}</math> provides essentially all the finite-dimensional irreducible representations of GL(V).
 
==See also==
* [[Representation theory of the symmetric group]]
 
==Notes==
<references/>
 
==References==
* William Fulton. ''Young Tableaux, with Applications to Representation Theory and Geometry''. Cambridge University Press, 1997.
* Lecture 4 of {{Fulton-Harris}}
* [[Bruce Sagan|Bruce E. Sagan]]. ''The Symmetric Group''. Springer, 2001.
 
[[Category:Representation theory of finite groups]]
[[Category:Symmetric functions]]
[[Category:Permutations]]

Latest revision as of 14:24, 6 November 2014

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