Understanding Energy Corrections in a Perturbed Square Well Potential

In summary, the conversation discusses the introduction of a small potential perturbation in an infinite one-dimensional square well potential. The first-order energy correction for the ground state is found to be 100 times lower than that of the first excited state. This is due to the fact that the ground state wave function has a maximum in the middle, while the first excited state has a node, making the ground state more stable and less affected by the perturbation. The calculations and interpretations of the results are also discussed.
  • #1
JohanL
158
0
we have a particle in an infinite one-dimensional square well potential

[V(x)=0 for 0<x<L and V(x) is infinite otherwise]

and introduce a small potential (perturbation) in the middle of the
square well potential. Then the first order energy correction
for the ground state is 100 times lower than the first order correction
to the first excited state. I don't understand why...

The wave function without the small potential step in the middle
is zero in the middle for the first excited state and maximum in the middle
for the ground state. Has the diffrence in energy corrections something
to do with this?
 
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  • #2
Welcome JohanL !

I don't know exactly the parameters, so it is difficult to answer. Maybe the reason is that the lower energy state is especially stable, whereas excited states already have dynamics included.

I hope better answers will come.
 
  • #3
Thank you!

Im just a beginner in perturbation theory...
The wavefunctions are just the usual standing waves in
[V(x)=0 for 0<x<L and V(x) is infinite otherwise]

and then a small step of width a=L/10 and height h is introduced in the
middle of the square well potential, i.e.
V(x)=h for 0.5(L-a)<x<0.5(L+a)

Then with perturbation theory I calculate the first orde energy corrections
to the unperturbed eigenvalues and I get that the corrections
is 100 times larger for the first excited state than for the ground state.
and i don't understand why...
 
  • #4
OK, now all the parameters are here.

I don't know if my interpretation is correct. If I figure out something better, I'll let you know. The calculations barely tell you any deep reason. Do they ?
 
  • #5
JohanL said:
Thank you!

Im just a beginner in perturbation theory...
The wavefunctions are just the usual standing waves in
[V(x)=0 for 0<x<L and V(x) is infinite otherwise]

and then a small step of width a=L/10 and height h is introduced in the
middle of the square well potential, i.e.
V(x)=h for 0.5(L-a)<x<0.5(L+a)

Do you mean <psi|V|psi> where V is your potential and psi the unperturbed state (sin(pi nx/L) ?

So I guess you calculate something like Integral( h sin^2(pi n x/L) dx) between x = 0.5(L-a) and 0.5(L+a) with appropriate normalisations I don't know by heart ?

cheers,
Patrick.
 
  • #6
Yes, that's exactly what i have done.
and when i have calculated the integral i set n=1 for
the energy correction for the ground state and then n=2
for the correction for the first excited states.
and the corrections i get is
E(n=1)=0.0016 h
E(n=2)=0.19 h

and then i need a qualitative interpretation for why they differ
so much...
 
  • #7
JohanL said:
Yes, that's exactly what i have done.
and when i have calculated the integral i set n=1 for
the energy correction for the ground state and then n=2
for the correction for the first excited states.
and the corrections i get is
E(n=1)=0.0016 h
E(n=2)=0.19 h

I get something else.

psi_n(x) = sqrt(2/L) Sin[ n Pi x/L ]

I then find (using Mathematica) that the integral of psi_n(x)^2 from (L-a)/2 to (L+a)/2 equals:

a/L - Cos[n Pi] Sin[ a n Pi/L] / (n Pi)

this gives for the first energy correction:

a/L + Sin[a Pi/L]

for the second:

a/L - Sin[2 a Pi/L] / (2 Pi)

...

(all this times h of course).
Filling in L -> 1, a -> 1/10, I find numerically:
{0.198363, 0.00645107, 0.185839, 0.0243173, 0.163662, 0.0495449}

for n = 1, 2, 3, 4, 5 and 6.

Now maybe I'm wrong ! I can send you the (simple) mathematica sheet if you want.

cheers,
Patrick.
 
  • #8
JohanL said:
Yes, that's exactly what i have done.
and when i have calculated the integral i set n=1 for
the energy correction for the ground state and then n=2
for the correction for the first excited states.
and the corrections i get is
E(n=1)=0.0016 h
E(n=2)=0.19 h

and then i need a qualitative interpretation for why they differ
so much...

Hi there.

I can tell without doing the calculation that your results can't be right.

Your perturbation is in the center of the well. Around that point, the ground state probability density has a maximum whereas the second excited state has a node. Therefore, the ground state will be much more affected by the perturbation than the first excited state.

Pat
 
  • #9
Thank you Patrick and Pat!
Now I understand!
 

1. What is Simple Perturbation Theory?

Simple Perturbation Theory is a mathematical technique used in physics and engineering to approximate solutions to complex problems by breaking them down into simpler, more manageable parts. It is based on the idea that small changes in input parameters can lead to small changes in output values.

2. How is Simple Perturbation Theory different from regular perturbation theory?

Simple Perturbation Theory is a special case of regular perturbation theory where the perturbation parameter is small and the unperturbed system can be solved analytically. This allows for more precise and accurate solutions to be obtained.

3. What are some applications of Simple Perturbation Theory?

Simple Perturbation Theory has a wide range of applications in different fields such as quantum mechanics, fluid dynamics, and celestial mechanics. It is used to study the behavior of systems with small perturbations, such as the stability of orbits in the solar system or the behavior of electrons in an atom.

4. What are the limitations of Simple Perturbation Theory?

Simple Perturbation Theory is only applicable when the perturbation is small and the unperturbed system can be solved analytically. If the perturbation is large, the resulting solutions may not accurately represent the actual behavior of the system. Additionally, it may not be applicable to systems with nonlinear dynamics.

5. How can Simple Perturbation Theory be used in experimental science?

Simple Perturbation Theory can be used to analyze experimental data and make predictions about the behavior of a system. By measuring small changes in input parameters and using the perturbation theory equations, scientists can make accurate predictions about the behavior of the system under different conditions. This can help in designing experiments and understanding complex systems.

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