Deduce if the spectrum is discrete/continuous from the potential

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SUMMARY

The discussion centers on determining the conditions under which a one-dimensional potential results in discrete or continuous energy levels. Specifically, the potential v(r) = 1/r (for r > 0), as exemplified by the hydrogen atom, indicates that for energy levels E > 0, a continuous spectrum arises, while E < 0 leads to discrete energy levels. This behavior is attributed to the potential approaching zero as r approaches infinity, resulting in bound states for negative energy and scattering states for positive energy. The user seeks a more comprehensive proof of this phenomenon, referencing Sakurai's coursebook and noting exceptions in certain systems as described in Ballentine.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly energy levels and potentials.
  • Familiarity with the concept of bound states versus scattering states.
  • Knowledge of the mathematical treatment of potentials in quantum systems.
  • Basic proficiency in interpreting quantum mechanical texts, such as Sakurai and Ballentine.
NEXT STEPS
  • Research the mathematical proof of energy levels in one-dimensional potentials, focusing on the Schrödinger equation.
  • Study the concept of bound states and scattering states in greater detail.
  • Explore exceptions to the general rules of energy levels in quantum systems, particularly those mentioned in Ballentine.
  • Examine the implications of potentials that do not approach zero at infinity.
USEFUL FOR

Students and professionals in quantum mechanics, particularly those studying energy levels in one-dimensional potentials, as well as educators seeking to clarify these concepts for learners.

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I have one-dimensional problem with a one-dimensional potential
I want to know the energy domains that will result in discrete energy levels and the energy domains that will result in continuous energy levels
I have one-dimensional problem with a one-dimensional potential
I want to know the energy domains that will result in discrete energy levels and the energy domains that will result in continuous energy levels

In my lecture, my professor gave the example of v(r) = 1/r (r>0) (hydrogen atom basically). he told us that we can know immediately that for E>0 we will get continuous spectrum and for E<0 discrete spectra.
As far as I understood him, its because when r goes to infinity V goes to 0.

I would like to know the full explanation and why it works (some sort of proof would be nice ).
I tried to look for a decent explanation in Sakurai ( the coursebook) but unfortunately, I couldn't find one
 
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saar321412 said:
Summary: I have one-dimensional problem with a one-dimensional potential
I want to know the energy domains that will result in discrete energy levels and the energy domains that will result in continuous energy levels

I have one-dimensional problem with a one-dimensional potential
I want to know the energy domains that will result in discrete energy levels and the energy domains that will result in continuous energy levels

In my lecture, my professor gave the example of v(r) = 1/r (r>0) (hydrogen atom basically). he told us that we can know immediately that for E>0 we will get continuous spectrum and for E<0 discrete spectra.
As far as I understood him, its because when r goes to infinity V goes to 0.

I would like to know the full explanation and why it works (some sort of proof would be nice ).
I tried to look for a decent explanation in Sakurai ( the coursebook) but unfortunately, I couldn't find one
If you assume for simplicity that the potential goes to ##0## at infinity, then ##E < 0## results in bound states that have a discrete spectrum. And ## E > 0## results in scattering states that typically have a continuous spectrum.

You could search online for a proof of this.
 
Interestingly enough, there are actually systems where positive energy bound states are emebedded in the continuous spectrum. See ballentine.
 
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