Rotational invariance and degeneracy (quantum mechanics)

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SUMMARY

The discussion centers on the proof that if a Hamiltonian H is invariant under all rotations, then its eigenstates are also eigenstates of the angular momentum operator L², exhibiting a degeneracy of 2l+1. Key equations referenced include L_z|l,m⟩=m|l,m⟩ and the ladder operators L₊ and L₋. The solution approach can be executed in either a generic Hilbert space for general rotations or specifically in a 3D real Hilbert space.

PREREQUISITES
  • Understanding of quantum mechanics, specifically angular momentum operators
  • Familiarity with Hilbert space concepts
  • Knowledge of eigenstates and eigenvalues in quantum systems
  • Proficiency in using ladder operators in quantum mechanics
NEXT STEPS
  • Study the properties of angular momentum in quantum mechanics
  • Learn about the representation of rotation operators in Hilbert space
  • Explore the implications of degeneracy in quantum systems
  • Investigate the mathematical formulation of ladder operators and their applications
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Students and researchers in quantum mechanics, particularly those focusing on angular momentum and rotational invariance in quantum systems.

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Homework Statement




Show that if a Hamiltonian H is invariant under all rotations, then the eigenstates of H are also eigenstates of L^{2} and they have a degeneracy of 2l+1.


Homework Equations



The professor told us to recall that

J: \vec{L}=(L_x,L_y,L_z)

L_z|l,m\rangle=m|l,m\rangle

L_\pm=L_x\pm iL_y

L_\pm|l,m\rangle= \hbar\sqrt{l(l+1)-m(m\pm1)} |l,m\pm 1\rangle


The Attempt at a Solution



I have been reading as much materials as I can, but I still have no clue at all on how to solve it at this moment. Can anyone help? Thank you so much!
 
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I solved it!

Thank goodness! I have solved it now.

One can do the calculations in either generic Hilbert space for general rotations or in 3D real Hilbert space.
 

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