The rigid rotator and Angular momentum.

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SUMMARY

The discussion centers on the relationship between spherical harmonics, angular momentum operators \(\hat{L}\) and \(\hat{L}_z\), and the rigid rotator model in quantum mechanics. It is established that while spherical harmonics are simultaneous eigenfunctions of \(\hat{L}\) and \(\hat{L}_z\), the three-fold degeneracy of the state with \(l=1\) indicates that the values of \(L\) and \(L_z\) cannot be determined simultaneously if the system is in a superposition of different \(m\) states. However, since \(\hat{L}^2\) and \(\hat{L}_z\) commute, both \(l\) and \(m\) can be measured independently when the system is not in superposition.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly angular momentum.
  • Familiarity with spherical harmonics and their properties.
  • Knowledge of quantum operators, specifically \(\hat{L}\) and \(\hat{L}_z\).
  • Concept of degeneracy in quantum states.
NEXT STEPS
  • Study the properties of spherical harmonics in quantum mechanics.
  • Learn about the commutation relations of angular momentum operators.
  • Explore the concept of superposition in quantum states.
  • Investigate the rigid rotator model and its applications in quantum mechanics.
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Students and professionals in quantum mechanics, physicists studying angular momentum, and anyone interested in the mathematical foundations of quantum systems.

siddharth5129
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If spherical harmonics are simultaneous eigenfunctions of \hat{L} and \hat{L}_{z}, then that means for a state at which l=1, and where you have three possible values of m (1, 0 , -1) that the value of L and L_{z} cannot really be determined simultaneously. Because the three fold degeneracy of the state implies that the rigid rotator exists in a three dimensional subspace with the eigenkets given by the three spherical harmonics determined by l=1. Is this true, or am I getting something wrong? My textbook says that they can be determined simultaneously, but I'm pretty sure this is only true if the particle exists in a state given by one of the eigen-kets of the degenerate subspace.
 
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siddharth5129 said:
If spherical harmonics are simultaneous eigenfunctions of \hat{L} and \hat{L}_{z}, then that means for a state at which l=1, and where you have three possible values of m (1, 0 , -1) that the value of L and L_{z} cannot really be determined simultaneously. Because the three fold degeneracy of the state implies that the rigid rotator exists in a three dimensional subspace with the eigenkets given by the three spherical harmonics determined by l=1.
I've having a hard time understanding your argument here. But the rotation of a rigid rotor is described by \hat{L}^2, and since \hat{L}^2 and \hat{L}_z commute, it is always possible to measure both ##l## and ##m##. That said, if the system is in a superposition of different ##m## states, with the same value of ##l##, then of course upon measurement only a single value of ##m## will be obtained and the rotor will "collapse" to that particular ##l,m## state, which does not affect the possibility of measuring ##l## independently.
 
yeah. that makes sense. I was confusing myself. Thanks.
 

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