Sharp values of wavefunction in polar coordinates

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The discussion focuses on demonstrating that the wavefunction ψ(r,θ,φ) = R(r)sinθe^{iφ} yields sharp values for the magnitude and z-component of orbital angular momentum. To achieve sharpness for Lz, the eigenfunction condition -iħ(dψ/dφ) = Lzψ must be satisfied, indicating that the radial function R(r) does not affect the outcome. Participants suggest calculating expectation values to clarify the sharp values of angular momentum. The conversation highlights the importance of understanding the eigenfunction condition in the context of quantum mechanics. Overall, the thread emphasizes the relationship between wavefunctions and angular momentum properties.
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Homework Statement


Consider the function in polar coordinates

ψ(r,θ,\phi) = R(r)sinθe^{i\phi}

Show by direct calculation that ψ returns sharp values of the magnitude and z-component of the orbital angular momentum for any radial function R(r). What are these sharp values?

The Attempt at a Solution



I -think- for L_{z} to be sharp, you have to impose the eigenfunction condition

-i\hbar \frac{dψ}{d\phi} = L_{z}ψ

which means that the radial function R(r) would cancel with itself if you were to rearrange the above for L_{z}. However I could have completely the wrong idea here.
 
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How about calculating the expectation values corresponding to "the magnitude and z-component of the orbital angular momentum "?
 

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