Let U = e iG 3 e iG2 e iG3 , where (a ,, )
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Let U = eiG3αeiG2β eiG3γ, where (a ,β, γ) are the Eulerian angles. In order that U represent a rotation (a ,β, γ), what are the commutation rules that must be satisfied by the Gk? Relate G to the angular-momentum operators.
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To understand the commutation rules that the Gk operators must satisfy in order for U to represent a rotation we need to examine the properties of the ...View the full answer
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