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Group Orthogonality Theorem


The group orthogonality theorem applies to a finite group G of group order h and pairwise inequivalent irreducible representations Gamma_i on complex vector spaces of dimensions l_i. Choose realizations by unitary matrices. Then

 sum_(R in G)Gamma_i(R)_(mn)Gamma_j(R)_(m^'n^')^*=h/(sqrt(l_il_j))delta_(ij)delta_(mm^')delta_(nn^'),

where the sum is over all group elements R, Gamma_i(R)_(mn) is the entry in row m and column n of the matrix Gamma_i(R), * denotes complex conjugate, and the delta symbols are Kronecker deltas. The proof is nontrivial and may be found in Eyring et al. (1944).


See also

Group, Group Character, Irreducible Representation

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References

Eyring, H.; Walter, J.; and Kimball, G. E. Quantum Chemistry. New York: Wiley, p. 371, 1944.

Referenced on Wolfram|Alpha

Group Orthogonality Theorem

Cite this as:

Weisstein, Eric W. "Group Orthogonality Theorem." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/GroupOrthogonalityTheorem.html

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