Representation operator
Irreducible operators applied to an irreducible orthonormal basis
Let π :πΊ βGL(π) be a unitary representation with its decomposition into irreps.
Let {Oππ}πππ=1 be irreducible operators transforming in Ξπ and {|πππΌπβ©}πππ=1 be an irreducible orthonormal basis transforming in Ξπ.
Then Oππ|πππΌπβ© transform under πΊ in the product representation Ξπβπ (within the same carrier space)
π(π)Oππ|πππΌπβ©=π(π)Oπππ(π)β π(π)|πππΌπβ©=βπOπΞπππ(π)ββ|πππΌββ©Ξπβπ=βπ,βOπ|πππΌββ©Ξπππ(π)Ξπβπ
which may then be expanded in a decomposed reΓ€lization using the Clebsch-Gordan coΓ«fficients.
Oππ|πππΌπβ©=|π,πβ©=βπ;π½,β|πΌ,π,ββ©β¨πΌ,π,β|π,πβ©πβπ
giving rise to the Wigner-Eckart theorem.
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