Finite Well Potential - Unbound eigenfunction

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SUMMARY

The discussion centers on the characteristics of unbound standing wave eigenfunctions in a finite square well potential. It establishes that for an unbound particle with total energy E greater than the potential V, the eigenfunction inside the well is represented as Asin(k0x), while outside the well it takes the form Bsin(k1x + φ). The wave number k0 is greater than k1, indicating a higher frequency inside the well. The amplitude of the eigenfunction is shown to decrease within the well, countering initial intuitions about particle behavior.

PREREQUISITES
  • Understanding of the Time Independent Schrödinger Equation
  • Familiarity with finite square well potential concepts
  • Knowledge of wave functions and their properties
  • Basic quantum mechanics principles, including energy states
NEXT STEPS
  • Study the implications of wave function amplitude in quantum mechanics
  • Explore the mathematical derivation of eigenfunctions in finite square wells
  • Investigate the relationship between energy levels and wave function behavior
  • Learn about the harmonic oscillator and its eigenstates for comparative analysis
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Students and educators in quantum mechanics, physicists analyzing wave functions, and anyone interested in the behavior of particles in potential wells.

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Homework Statement



From qualitative arguments, make a sketch of the form of a typical unbound standing wave eigenfunction for a finite square well potential.

An unbound particle is one which has total energy E greater than the Potential V of the well

Is the amplitude of the oscillation the same in all regions?

Homework Equations



Using the Time Independent Schrödinger Equation we see that:

The Attempt at a Solution



Inside well: Solution is of form [tex]Asin(k_0x)[/tex] where [tex]k_0 = \sqrt{2mE/\hbar^2}[/tex]

Outside well: Solution is of from [tex]Bsin(k_1x + \phi)[/tex] where [tex]k_1 = \sqrt{2m(E-V)/\hbar^2}[/tex] where [tex]\phi[/tex] is the phase shift which can be adjusted to satisfy the boundary conditions.

So inside the well, the wave number of the eigenfunction should be greater than the eigenfunction outside the well. This should mean that the eigenfunction's frequency inside the well is higher.

I've looked around and I found this http://vnatsci.ltu.edu/s_schneider/physlets/main/finite_sqr_well.shtml" . You can look at the unbound states by clicking and dragging your mouse on the black bar on the right with the green lines.

It suggests that the amplitude of the eigenfunction should decrease when inside the quantum well.

I thought the amplitude of the eigenfunction should give you an indication of the probability of finding the particle in that particular region. If so, shouldn't the amplitude be slightly higher inside the well?
 
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The intuitive explanation is that inside the well, the particle has more energy relative to the floor of the well. It therefore moves faster, which means it spends less time inside the well than outside.

However, this intuition sometimes fails miserably (i.e. for the lower-energy states of the harmonic oscillator). It's always best to do the math and compare the amplitudes of the relevant waves.
 

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