The commutator $$\left[ {{L_z},\,{Y_{lm}}\left( {\theta ,\,\phi } \right)} \right],$$ where Lz is the z component of the orbital angular momentum and $${{Y_{lm}}\left( {\theta ,\,\phi } \right)}$$ is a spherical harmonic, is
A. $$l\left( {l + 1} \right)\hbar $$
B. $$ - m\hbar $$
C. $$m\hbar $$
D. $$ + l\hbar $$
Answer: Option C
Related Questions on Quantum Mechanics
A. In the ground state, the probability of finding the particle in the interval $$\left( {\frac{L}{4},\,\frac{{3L}}{4}} \right)$$ is half
B. In the first excited state, the probability of finding the particle in the interval $$\left( {\frac{L}{4},\,\frac{{3L}}{4}} \right)$$ is half This also holds for states with n = 4, 6, 8, . . . .
C. For an arbitrary state $$\left| \psi \right\rangle ,$$ the probability of finding the particle in the left half of the well is half
D. In the ground state, the particle has a definite momentum
A. (e-ax1 - e-ax2)
B. a(e-ax1 - e-ax2)
C. e-ax2 (e-ax1 - e-ax2)
D. None of the above

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