Error of the WKB approximation

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Discussion Overview

The discussion centers on the error analysis of the WKB approximation in the context of the Schrödinger equation with a quadratic potential, specifically ##V(x) = x^2##. Participants explore methods to quantify the error between approximate and exact wavefunctions, considering both energy and wavefunction differences.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant seeks guidance on calculating the error of the WKB approximation compared to the exact solution, proposing the use of the formula ##e = |y_{exact} - y_{approx}|##.
  • Another participant suggests calculating the relative error on eigenenergy and the L2 norm of the difference in wavefunctions, but expresses concern about the influence of complex phases on the results.
  • There is a proposal to calculate the difference in probability distributions as an alternative measure of error.
  • A participant questions the validity of using the probability difference integral as a measure of "distance of states," noting that it is influenced by normalization conditions.
  • Suggestions are made to consider integrating the absolute value of the differences in probability distributions for a more accurate measure.
  • One participant reflects on the need for a measure of the difference in local probability distribution, proposing the maximum difference at any point as a potential approach.

Areas of Agreement / Disagreement

Participants express differing views on the best methods to quantify the error of the WKB approximation, with no consensus reached on a definitive approach. Some methods are challenged or refined, indicating ongoing debate.

Contextual Notes

The discussion highlights limitations in the proposed measures, particularly regarding normalization and the influence of complex phases, but does not resolve these issues.

phyQu
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TL;DR
How to calculate the error made using the WKB approximation?
hello everyone

I tell you a little about my situation.
I already found the approximate wavefunctions for the Schrödinger equation with the potential ##V(x) = x^2##, likewise, energy, etc.
I have the approximate WKB solution and also the exact numeric solution.

What I need to do is to calculate the error of the approximate solution with respect to the exact solution,
but I need help to start, because I am lost with this topic.

Will it be possible to make an error analysis?
Will it be possible apply that is defined as ##e = |y_{exact} - y_{approx}|##?

Do you know if someone has already worked out the error for the WKB approximation?
Do you know of any recent article dealing with this?
I've searched the internet and I can't find anything that tells me specifically about the error of this method, please, can someone help me.

Thanks in advance
 
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I am not aware of any previous results concerning the error of the WKB approximation. Since the quality of the approximation depends on the variation of the potential with respect to the oscillation (wave number) of the wave function, I would be surprised if there was a general answer to this.

I would calculate the relative error on the eigenenergy as well as the L2 norm of the difference in wave functions,
$$
\int_{-\infty}^\infty \left| \psi_\textrm{exact}(x) - \psi_\textrm{approx}(x) \right|^2 \, dx
$$
However, this might be too much influenced by the complex phase, which is not physically relevant, so I would also calculate the difference in probability
$$
\int_{-\infty}^\infty \left| \psi_\textrm{exact}(x)\right|^2 - \left|\psi_\textrm{approx}(x) \right|^2 \, dx
$$
 
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Thank you very much, by the way, do you know a book that has this topic you are talking about? I would help me to reference my work.
 
The latter integral is not a good measure for the "distance of states", because the overall factor is just determined by the normalization condition, i.e., that integral should be 0 when normalizing both wave functions properly.
 
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DrClaude said:
However, this might be too much influenced by the complex phase, which is not physically relevant, so I would also calculate the difference in probability
$$
\int_{-\infty}^\infty \left| \psi_\textrm{exact}(x)\right|^2 - \left|\psi_\textrm{approx}(x) \right|^2 \, dx
$$
vanhees71 said:
The latter integral is not a good measure for the "distance of states", because the overall factor is just determined by the normalization condition, i.e., that integral should be 0 when normalizing both wave functions properly.
Well, you could integrate over the absolute value of the differences:
$$
\int_{-\infty}^\infty \left|\left| \psi_\textrm{exact}(x)\right|^2 - \left|\psi_\textrm{approx}(x) \right|^2\right| \, dx
$$
 
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vanhees71 said:
The latter integral is not a good measure for the "distance of states", because the overall factor is just determined by the normalization condition, i.e., that integral should be 0 when normalizing both wave functions properly.
Obviously :confused:. I should've thought a bit more about it. I was after a measure of the difference in local probability distribution. Maybe something like
$$
\max_x \left( \left| \psi_\textrm{exact}(x)\right|^2 - \left|\psi_\textrm{approx}(x) \right|^2 \right)
$$
 
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