Solve Double Potential Well: Write Equations & Find Wavenumbers

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Homework Help Overview

The discussion revolves around a quantum mechanics problem involving a double potential well defined by piecewise potential functions. The original poster seeks to set up the relevant equations for different regions defined by the potential and to demonstrate that the wavenumbers of the wave functions satisfy a transcendental equation.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the setup of Schrödinger equations for various regions of the potential and express confusion about boundary conditions, particularly in infinite potential regions. There is an exploration of how to handle different energy conditions (E > V0, E = V0, E < V0) and the implications for the wave functions.

Discussion Status

Some participants have offered guidance on the nature of reflections in infinite potential regions and the continuity of wavefunctions at boundaries. The conversation indicates that multiple interpretations of the problem are being explored, particularly regarding the treatment of boundary conditions and energy levels.

Contextual Notes

Participants note constraints such as the requirement to find energies that work without solving for specific energy conditions, leading to uncertainty about the implications of the infinite potential regions on the wavefunctions.

MobiusPrime
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Homework Statement



V(x) = [tex]\left\{\infty \textrm{ for } x<0[/tex]
[tex]\left\{0 \textrm{ for } 0<x<a[/tex]
[tex]\left\{V_0 \textrm{ for } a<x<a+2b[/tex]
[tex]\left\{0 \textrm{ for } a+2bx<2a+2b[/tex]
[tex]\left\{\infty \textrm{ for } 2a+2b<x[/tex]

Set up the relevant equations in each region, write down the appropriate solution and then show that the wavenumber of the wave functions inside and outside the barrier satisfy a transcendental equation.

Homework Equations





The Attempt at a Solution



I have basically used Schrödinger equations for the energy for regions 1 2 and 3. but this is where i get stuck. I have to show the energies that work (hope that makes sense). I'm not suppose to solve for [tex]E>V_0, E=V_0 or E<V_0[/tex] but find the energies that work. I am a bit confused about the boundary conditions also. I set them up the same as a finite potential barrier, but do i need boundary conditions for x<0 and x>2a+2b? as these sections are infinite, we should just get 100% reflection?
I am also confused about the barrier in the middle. When solving for [tex]E>V_0, E=V_0 or E<V_0[/tex] we have different Schrödinger equations and different boundary conditions. How do i do it for any value of E?

I guess you all know by now i am pretty stuck lol.
Hope someone can help =)
and hope my LaTeX and writing is easy to understand =P
 
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MobiusPrime said:

Homework Statement



V(x) = [tex]\left\{\infty \textrm{ for } x<0[/tex]
[tex]\left\{0 \textrm{ for } 0<x<a[/tex]
[tex]\left\{V_0 \textrm{ for } a<x<a+2b[/tex]
[tex]\left\{0 \textrm{ for } a+2bx<2a+2b[/tex]
[tex]\left\{\infty \textrm{ for } 2a+2b<x[/tex]

Set up the relevant equations in each region, write down the appropriate solution and then show that the wavenumber of the wave functions inside and outside the barrier satisfy a transcendental equation.

Homework Equations





The Attempt at a Solution



I have basically used Schrödinger equations for the energy for regions 1 2 and 3. but this is where i get stuck. I have to show the energies that work (hope that makes sense). I'm not suppose to solve for [tex]E>V_0, E=V_0 or E<V_0[/tex] but find the energies that work.
I'm not exactly sure what that means, but I'd try considering each case separately even if you're not going to have them in your final solution, just so you can develop an intuition for the problem and its solutions.
I am a bit confused about the boundary conditions also. I set them up the same as a finite potential barrier, but do i need boundary conditions for x<0 and x>2a+2b? as these sections are infinite, we should just get 100% reflection?
Yes, you'll get 100% reflection and no penetration into those regions. You know that the wavefunction vanishes when x<0 or x>2a+2b because the potential is infinite in those regions. You still need continuity of the wavefunction at the boundaries, but because you're dealing with an infinite potential, the derivative doesn't need to be continuous.
I am also confused about the barrier in the middle. When solving for [tex]E>V_0, E=V_0 or E<V_0[/tex] we have different Schrödinger equations and different boundary conditions. How do i do it for any value of E?

I guess you all know by now i am pretty stuck lol.
Hope someone can help =)
and hope my LaTeX and writing is easy to understand =P
 
[tex] V(x)= \left\{ \begin{array}{ccccc}<br /> \infty & \textrm{ for } x<0 \\<br /> 0 & \textrm{ for } 0 < x < a \\<br /> Vo & \textrm{ for } a < x < a+2b \\<br /> 0 & \textrm{ for } a+2bx<2a+2b \\<br /> \infty & \textrm{ for } 2a+2b<br /> <br /> \end{array} \right <br /> [/tex]
 
Last edited:
vorcil said:
[tex] \Psi(x,0) = \left\{ \begin{array}{ccc}<br /> \infty & \textrm{ for } x<0 \\<br /> 0 & \textrm{ for } 0 < x < a \\<br /> \{V_0 & \textrm{ for } a < x < a+2b \\<br /> 0 & \textrm{ for } a+2bx<2a+2b \\<br /> \infty & \textrm{ for } 2a+2b<br /> <br /> \end{array} \right <br /> [/tex]

you can not have the wavefunction and the potential infinity for the same region! .. please try to solve the question step by step..
 
whoops I just copyed some latex, forgot to replace Psi with v(x)
my bad
 

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