What Energy Maximizes Neutron Trapping in a Finite Square Well?

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SUMMARY

The discussion focuses on determining the optimal energy level for a neutron to maximize its probability of being trapped in a finite square well, characterized by depth V0 and width 2a. The integral of the wavefunction squared, t0}^{t1}∫-a^{a} |Ψ(x,t)|² dx dt, is critical in assessing the neutron's interaction with the potential well. The initial energy E0 of the neutron must be optimized to enhance this integral, thereby increasing the likelihood of photon emission and energy reduction. The relationship between the neutron's energy and the time taken to cross the well is also a key factor in this analysis.

PREREQUISITES
  • Understanding of quantum mechanics, specifically wavefunctions and potential wells.
  • Familiarity with the concept of bound and free particles in quantum systems.
  • Knowledge of integrals and their applications in probability density functions.
  • Basic principles of photon emission and energy transitions in quantum particles.
NEXT STEPS
  • Explore the mathematical formulation of finite square wells in quantum mechanics.
  • Study the implications of wavefunction behavior on particle trapping in potential wells.
  • Investigate the relationship between energy levels and time of flight in quantum systems.
  • Learn about photon emission processes and their effects on particle energy states.
USEFUL FOR

Students of quantum mechanics, physicists studying particle interactions, and researchers focused on neutron behavior in potential wells will benefit from this discussion.

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Free particle --> bound particle

Homework Statement



A free neutron meets a finite square well of depth V_{0}, and width 2a centered around origo.

However, the probability that the neutron emits a photon when it meets the potential well, and thus decreasing its energy is proportional to the integral \int^{t_{1}}_{t_{0}}\int^{a}_{-a} |\Psi(x,t)|^{2} dx dt. Where t_{1}-t_{0} is the time it takes the neutron to cross the well.

The question then is: "What energy is the most advantageous for the neutron to have, in order to be trapped by the potential well?"


The Attempt at a Solution


The initial energy is E_{0}, the energy of the photon is E_{p}

I'm guessing I have to find a value for E_{0}, so as to make the integral a large as possible.
 
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Is there some form of ψ here that you are neglecting to tell us (like it is the wavefunction of the neutron)? If ψ is independent of E (or E0), then I don't see how it would make a difference (unless it's as silly as to realize to treat the neutron classically, so that t1-t0 depends inversely on the square root of E, which it may be, since it talks about "the time it takes the neutron to cross the well").
 

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