Finite Well Potential - Unbound eigenfunction

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The discussion centers on the characteristics of unbound standing wave eigenfunctions in a finite square well potential, where the total energy E exceeds the potential V. Inside the well, the eigenfunction is represented as Asin(k_0x), while outside the well, it takes the form Bsin(k_1x + φ), with k_0 and k_1 being wave numbers that indicate different frequencies. Participants debate whether the amplitude of the eigenfunction should be higher inside the well due to increased energy, but some argue that it actually decreases, suggesting a lower probability of finding the particle in that region. The conversation emphasizes the importance of mathematical analysis over intuition in understanding wave behavior. Ultimately, the consensus leans towards calculating amplitudes to clarify these concepts.
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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 Schrodinger Equation we see that:

The Attempt at a Solution



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

Outside well: Solution is of from Bsin(k_1x + \phi) where k_1 = \sqrt{2m(E-V)/\hbar^2} where \phi 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.
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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