Klein-Gordon Finite Well

In summary, the problem is to solve the Klein-Gordon equation for a finite well with a constant potential, under the condition that V > E + mc^2. The solutions for the wave function in the different regions of the well are identified as 1, 2, and 3, but further explanation and derivation is needed. The concept of bound energy states is mentioned, but not fully explained, and it is unclear how this relates to the problem. Additionally, the possibility of solving for the coefficients in the wave function outside the well is raised, but without explanation or reasoning. Lastly, the concept of transmission and reflection coefficients is mentioned, but it is not clear how this relates to the problem or the solutions provided.
  • #1
Pengwuino
Gold Member
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Homework Statement



The problem is basically solving the Klein-Gordon equation for a finite well for a constant potential under the condition [tex]V > E + mc^2[/tex]

Homework Equations



[tex] V = 0 -a<x<a[/tex]
[tex] V = V_o [/tex] elsewhere

KG Equation: [tex][\nabla^2 + \left({{V-E} \over {\hbar c}}\right)^2 - k_c^2]\phi(x) = 0[/tex]

The Attempt at a Solution



So we're looking at the situation where the potential is high enough so that [tex]V > KE + 2mc^2[/tex]

We have solutions of the form [tex]\psi(x) = Ae^{ikx}+Be^{-ikx}[/tex] where
[tex]k = \sqrt{\left({{V-E}\over{\hbar c}}\right)^2 - k_c^2}[/tex]
[tex]k_c = {{m} \over {\hbar c}}[/tex]

For this case, the group velocities are such that the solutions in the left, center, and right regions, which i'll denote as 1, 2, and 3, are as follows:

[tex]\phi_1(x) = Ae^{ik_1x}[/tex]
[tex]\phi_{2}(x) = Ccos(k_{2}x) + Dsin(k_{2}x)[/tex]
[tex]\phi_{3}(x) = Ge^{-ik_{3}x}[/tex]

where
[tex]k_{1/3} = \sqrt{\left({{V-E}\over{\hbar c}}\right)^2 - k_c^2}[/tex]
[tex]k_{2} = \sqrt{\left({{E}\over{\hbar c}}\right)^2 - k_c^2}[/tex]

The problem is I have no idea how far this problem can be taken. I assume you can figure out the bound energy states for the particle. However, considering the wave function outside the well are sinusoidal, are the coefficients solvable? In scattering problems you can define a transmission and reflection coefficient but does it make sense to talk about "incoming" particles if the potential is so high?
 
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  • #2


I would like to offer some feedback on your solution attempt. First, it is important to clearly state the problem and the given conditions. In this case, the problem is to solve the Klein-Gordon equation for a finite well with a constant potential, under the condition that V > E + mc^2.

Next, you have correctly identified the solutions to the Klein-Gordon equation in the different regions of the well, denoted as 1, 2, and 3. However, you have not explained how you arrived at these solutions or how they are related to the given conditions. It would be helpful to provide some explanation or derivation for these solutions.

Furthermore, you mention the concept of bound energy states, but do not explain what these are or how they relate to the problem. It would be important to clarify this for a better understanding of the solution. Additionally, you ask if it is possible to solve for the coefficients in the wave function outside the well. This is a valid question, but again, it would be helpful to provide some explanation or reasoning behind it.

In terms of the scattering problem, it is possible to define transmission and reflection coefficients for particles with high potential barriers, as long as the particles have enough energy to overcome the barrier. However, it is not clear how this relates to the given problem or the solutions you have provided.

Overall, your solution attempt shows some understanding of the problem, but it would benefit from further explanation and clarification. it is important to clearly state the problem, provide a thorough explanation of the solution, and clearly connect the solution to the given conditions. I hope this feedback is helpful in your understanding of the problem and in improving your solution attempt.
 

1. What is the Klein-Gordon Finite Well?

The Klein-Gordon Finite Well is a mathematical model used in quantum mechanics to describe the behavior of particles within a finite potential well. It combines the concepts of both the Klein-Gordon equation and the finite potential well to provide a more accurate representation of particle behavior in confined spaces.

2. How is the Klein-Gordon Finite Well different from the Schrödinger equation?

Unlike the Schrödinger equation, which is a non-relativistic equation, the Klein-Gordon equation is a relativistic equation that takes into account the effects of special relativity on particle behavior. The Klein-Gordon Finite Well incorporates both the relativistic effects and the finite potential well to provide a more comprehensive model.

3. What are the applications of the Klein-Gordon Finite Well?

The Klein-Gordon Finite Well has various applications in the field of quantum mechanics, such as in the study of particle interactions and in the development of quantum computing algorithms. It is also used in other fields, such as solid-state physics, to study the behavior of electrons in confined spaces.

4. How is the Klein-Gordon Finite Well solved?

The Klein-Gordon Finite Well is solved using mathematical techniques, such as perturbation theory and numerical methods. The solution involves finding the eigenvalues and eigenfunctions of the Klein-Gordon equation within the finite potential well, which can be used to describe the energy levels and wave functions of particles within the well.

5. What are the limitations of the Klein-Gordon Finite Well?

One of the limitations of the Klein-Gordon Finite Well is that it does not take into account the effects of external forces on particles, such as electromagnetic fields. It also does not consider the spin of particles, which can be important in certain scenarios. Additionally, the model assumes a one-dimensional system and does not account for three-dimensional effects.

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