Here we pursue the more rigorous approach to the claim that the property quantized according to mℓ is Lz
(a) Starling with a straightforward application of the chain rule,
use the transformations given in Table 7.2 to show that
(b) Recall that L ≡ r × p. From the z-component of this famous formula and the definitions of the operators for px and py, argue that the operator for Lz is - .
(c) What now allows us to say that our azimuthal solution e*"t* has a well-defined z-component of angular momentum and that its value .
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