symmetrizer


Let V be a vector spaceMathworldPlanetmath over a field F. Let n be an integer, where n<char⁢(F) if char⁢(F)≠0. Let Sn be the symmetric groupMathworldPlanetmathPlanetmath on {1,…,n}. The linear operator S:V⊗n→V⊗n defined by:

S=1n!⁢∑σ∈SnP⁢(σ)

is called the symmetrizer. Here P⁢(σ) is the permutation operator. It is clear that P⁢(σ)⁢S=S⁢P⁢(σ)=S for all σ∈Sn.


Let S be the symmetrizer for V⊗n. Then an order-n tensor A is symmetricPlanetmathPlanetmath (http://planetmath.org/SymmetricTensor) if and only S⁢(A)=A.

Proof
If A is then

S⁢(A)=1n!⁢∑σ∈SnP⁢(σ)⁢A=1n!⁢∑σ∈SnA=A.

If S⁢(A)=A then

P⁢(σ)⁢A=P⁢(σ)⁢S⁢(A)=P⁢(σ)⁢S⁢(A)=S⁢(A)=A

for all σ∈Sn, so A is .

The theorem says that a is an eigenvectorMathworldPlanetmathPlanetmathPlanetmath of the linear operator S corresponding to the eigenvalueMathworldPlanetmathPlanetmathPlanetmathPlanetmath 1. It is easy to verify that S2=S, so that S is a projectionPlanetmathPlanetmath onto Sn⁢(V).

Title symmetrizer
Canonical name Symmetrizer
Date of creation 2013-03-22 16:15:44
Last modified on 2013-03-22 16:15:44
Owner Mathprof (13753)
Last modified by Mathprof (13753)
Numerical id 8
Author Mathprof (13753)
Entry type Definition
Classification msc 15A04