Regarding double well potential

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SUMMARY

The discussion centers on the eigenvalue conditions for a particle in a double-well potential defined by the piecewise function V(x) with E<0. The conditions for even and odd solutions are expressed as tan(q(a-b))=qα(1+tanh(αb)/(q² -α²tanh(αb)) and tan(q(a-b))=qα(1+coth(αb)/(q² -α²coth(αb)), respectively. The participant initially defined the wave function for odd solutions using Ψ(x)=Ae-αx for x>a and Bsin(q(x-b)) for b PREREQUISITES

  • Understanding of quantum mechanics, specifically wave functions and potential wells.
  • Familiarity with eigenvalue problems in quantum systems.
  • Knowledge of boundary conditions and continuity in wave functions.
  • Proficiency in mathematical techniques involving trigonometric functions and hyperbolic functions.
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  • Study the derivation of eigenvalue equations in quantum mechanics, focusing on double-well potentials.
  • Learn about the properties of wave functions in quantum systems, particularly odd and even solutions.
  • Explore the mathematical implications of continuity conditions for wave functions at boundaries.
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Students and professionals in quantum mechanics, physicists working with potential wells, and anyone interested in solving eigenvalue problems in quantum systems.

peripatein
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A particle is in the following double-well potential with E<0:
V(x)=0 for x<-a, x>a; -V0 for -a<x<-b, b<x<a; 0 for -b<x<b
I am asked to show that the eigenvalues conditions may be written in the form:
tan(q(a-b))=qα(1+tanh(αb)/(q22tanh(αb))$$
and
tan(q(a-b))=qα(1+coth(αb)/(q22coth(αb))$$
for the even and odd solutions, where -E=ħ2α2/2m and E+V02q2/2m.

I first tried to define the wave function in the various regions, focusing on the positive x-axis only and demanding odd solutions:
Ψ(x)=Ae-αx for x>a; Bsin(q(x-b)) for b<x<a; Ce-αx + Deαx for 0<x<b

Is that correct thus far?
 
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Looks good so far.
 
Alright, but as I impose continuity of wave function and its derivatives I obtain the four following equations, from which I am unable to derive the desired expression:
(1) Ae-αa = Bsin(q(a-b))
(2) -αAe-αa = Bqcos(q(a-b))
(3) 0 = Ce-αb + Deαb
(4) Bq = -αCe-αb + Dαeαb

What am I doing wrong?
 
You could explain what you did. Where does equation 3 come from?
Where is the odd/even condition?
 
Well, equation 3 stems from the demand for continuity at x=b. I have decided to focus on the odd solutions first, hence the use of sine. Is that wrong?
 
Ah, I see the issue.
The way you defined the wave function in the well, you get a mixture of odd and even functions (the sine would have some non-zero value at x=0). If you want odd functions, you need something like sin(qx).
 
So which function ought I to choose for Ψ(x) in the well? Ought it to be a combination of sine and cosine at once (like harmonic oscillator)?
 
In other words, should I then simply choose sin(qx) for the odd and cos(qx) for the even, within the well?
 
peripatein said:
So which function ought I to choose for Ψ(x) in the well? Ought it to be a combination of sine and cosine at once (like harmonic oscillator)?
You can do that, if you choose them without that offset it is easier to split them into odd and even contributions.
peripatein said:
In other words, should I then simply choose sin(qx) for the odd and cos(qx) for the even, within the well?
That is the easierst approach I think.
 
  • #10
Yet please note the expressions I am expected to arrive at. It seems I am indeed expected to use forms as sin(q(x-b)). Wouldn't you agree?
 
  • #11
I don't see how you get that impression. Yes there is an q(a-b), but that can appear in other ways, too.
 

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