Representation operator

Irreducible operators applied to an irreducible orthonormal basis

Let π‘ˆ :𝐺 β†’GL(𝑉) be a unitary representation with its decomposition into irreps. Let {Oπœ‡π‘–}π‘‘πœ‡π‘–=1 be irreducible operators transforming in Ξ“πœ‡ and {|π‘’πœˆπ›Όπ‘—βŸ©}π‘‘πœˆπ‘—=1 be an irreducible orthonormal basis transforming in Ξ“πœˆ. Then Oπœ‡π‘–|π‘’πœˆπ›Όπ‘—βŸ© transform under 𝐺 in the product representation Ξ“πœ‡βŠ—πœˆ (within the same carrier space)

π‘ˆ(𝑔)Oπœ‡π‘–|π‘’πœˆπ›Όπ‘—βŸ©=π‘ˆ(𝑔)Oπœ‡π‘–π‘ˆ(𝑔)β€ π‘ˆ(𝑔)|π‘’πœˆπ›Όπ‘—βŸ©=βˆ‘π‘˜Oπ‘˜Ξ“πœ‡π‘˜π‘–(𝑔)βˆ‘β„“|π‘’πœˆπ›Όβ„“βŸ©Ξ“πœˆβ„“π‘—=βˆ‘π‘˜,β„“Oπ‘˜|π‘’πœˆπ›Όβ„“βŸ©Ξ“πœ‡π‘˜π‘–(𝑔)Ξ“πœˆβ„“π‘—

which may then be expanded in a decomposed reΓ€lization using the Clebsch-Gordan coΓ«fficients.

Oπœ‡π‘–|π‘’πœˆπ›Όπ‘—βŸ©=|𝑖,π‘—βŸ©=βˆ‘πœ†;𝛽,β„“|𝛼,πœ†,β„“βŸ©βŸ¨π›Ό,πœ†,β„“|𝑖,π‘—βŸ©πœ‡βŠ—πœˆ

giving rise to the Wigner-Eckart theorem.


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