Energy values of a half harmonic oscillator

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SUMMARY

The discussion focuses on the energy values and wave functions of a "half" harmonic oscillator, specifically how they differ from those of a full harmonic oscillator. The key point is that the half harmonic oscillator has an infinite wall potential at x=0, which alters the boundary conditions for the wave functions. Consequently, only the odd eigenstates of the full harmonic oscillator are applicable for the half oscillator, leading to missing energy levels for even states such as E_2 and E_4. The time-independent Schrödinger equation must be adapted to reflect these new boundary conditions.

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  • Understanding of the time-independent Schrödinger equation
  • Familiarity with harmonic oscillator models in quantum mechanics
  • Knowledge of boundary conditions in quantum systems
  • Concept of eigenstates and their properties in quantum mechanics
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  • Study the time-independent Schrödinger equation for different boundary conditions
  • Explore the properties of eigenstates in quantum mechanics
  • Investigate the implications of infinite potential walls on wave functions
  • Compare energy levels of odd and even states in full harmonic oscillators
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Students and professionals in quantum mechanics, particularly those studying wave functions and boundary conditions in quantum systems, as well as researchers focusing on harmonic oscillator models.

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energy values of a "half" harmonic oscillator

This is the full question:
Find the solution to the "half" harmonic oscillator:
http://img241.imageshack.us/img241/9181/02bt7.jpg
Compare the energy values and wave functions with those of the full harmonic oscillator. Why are some of the full solutions present and some missing in the "half" problem?

I'm having some trouble figuring out how to find a solution for the wave function of a "half" harmonic oscillator. I can picture what this would look like, since if we "halved" a harmonic oscillator the left end point for energy levels E_1, E_3, E_5 and so on wouldn't be any good since the left end point would no longer be zero at the boundary.

I'm having some trouble figuring out how I should adapt the time-indepedent Schrödinger equation to these new boundaries because the book we use only mentions it briefly in the appendix. I don't even know what equation to look at because when I searched it online I got an equation that looked different from my book.
 
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You have to assume an infinite wall potential at ##x=0##. That's what makes the potential "half" harmonic. This means the eigenfunctions must vanish at ##x=0## and be appropriate for the full harmonic oscillator for ##x>0##. Can you figure out what these are? Hint: The eigenstates of the full harmonic oscillator are even and odd functions in ##x##.
 

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