Doubt in the quantum harmonic oscillator

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SUMMARY

The discussion centers on the quantum harmonic oscillator, specifically the properties of the annihilation operator ##a## and the creation operator ##a^{\dagger}## as outlined in Sakurai's text. The number operator ##N = a^{\dagger}a## is established as having eigenstates ##|n \rangle## with eigenvalues ##n##, leading to the conclusion that ##a | n \rangle## results in an eigenstate of ##N## with eigenvalue ##n - 1##. The participant questions the necessity of a non-degenerate spectrum for ##N## and the Hamiltonian in this context, seeking clarity on the physical implications of degeneracy in the harmonic oscillator's spectrum.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly the harmonic oscillator model.
  • Familiarity with operator algebra, specifically annihilation and creation operators.
  • Knowledge of eigenvalues and eigenstates in quantum systems.
  • Basic grasp of quantum textbooks, such as Sakurai's and Griffiths' works.
NEXT STEPS
  • Study the derivation of the quantum harmonic oscillator using Griffiths' textbook.
  • Explore the implications of degeneracy in quantum systems and its physical significance.
  • Investigate the role of the Hamiltonian in quantum mechanics and its relationship to the spectrum of operators.
  • Review the mathematical framework of eigenvalue problems in quantum mechanics.
USEFUL FOR

Students and professionals in quantum mechanics, particularly those studying the harmonic oscillator, quantum operators, and eigenvalue problems. This discussion is beneficial for anyone seeking a deeper understanding of the implications of degeneracy in quantum systems.

Lebnm
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I was reviewing the harmonic oscillator with Sakurai. Using the annihilation and the creation operators ##a## and ##a^{\dagger}##, and the number operator ##N = a^{\dagger}a##, with ##N |n \rangle = n | n \rangle##, he showed that ##a | n \rangle## is an eigenstate of ##N## with eigenvalue ##n - 1##, so he concludes that ##a | n \rangle \propto | n - 1 \rangle##. But, to it be true, the spectrum of ##N## should be non-degenerated, shouldn't it? Is this true? Can I proof this?
 
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You already label the eigen values by their energy, which relies on that the eigenvalues are non-degenerate.
 
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So, in the definition of the eigenstates of ##N##, I am imposing that they are non-degenerated, right? Is there some physical reason to do this? I can't see why the spectrum of ##N##, and consequently the spectrum of the hamiltonian, need to be non-degenerated in a harmonic oscillator.
 
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Lebnm said:
I can't see why the spectrum of ##N##, and consequently the spectrum of the hamiltonian, need to be non-degenerated in a harmonic oscillator.
You'll have to look in an introductory textbook, such as Griffiths.
 

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