9.6. Use the fact that all vectors must transform the same way under rotations to establish that any vector operator V must satisfy the commutation relations [Î, V;]=ihVy [΂, v‚1=-ihV, [Î, V-]= 0
9.6. Use the fact that all vectors must transform the same way under rotations to establish that any vector operator V must satisfy the commutation relations [Î, V;]=ihVy [΂, v‚1=-ihV, [Î, V-]= 0
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