How do I solve this integration problem in quantum mechanics?

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Discussion Overview

The discussion revolves around solving a specific integration problem in quantum mechanics related to normalization conditions. Participants explore methods to evaluate the integral involved in the problem and discuss the relevance of different mathematical techniques.

Discussion Character

  • Homework-related
  • Mathematical reasoning

Main Points Raised

  • One participant presents a normalization condition involving an integral and expresses uncertainty about how to solve it, questioning whether Fourier Transform is necessary.
  • Another participant suggests using the Poisson integral to simplify the problem, providing the integral's result as a potential solution.
  • A later reply indicates surprise at the simplicity introduced by the Poisson integral, implying a shift in understanding.
  • There is a challenge posed regarding the expected mathematical background necessary for solving the integral, referencing the complexity of calculus in quantum mechanics.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the best approach to solve the problem, as there are differing opinions on the methods required and the level of mathematical knowledge expected.

Contextual Notes

Some assumptions about the mathematical techniques and their applicability to the problem remain unresolved, particularly regarding the necessity of Fourier Transform versus the Poisson integral.

Hyperreality
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I've recently posted a thread asking for help in the Homework forum in solving this problem, but till now I still can't figure out how do find the solution to this equation.

Here is the problem.

Show that [tex]A=(\frac{m\omega}{\hbar\pi})^{1/4}.[/tex]

From the normalisation condition

[tex]|A|^2\int_{-\infty}^{\infty} e^{-2ax^{2}}=1[/tex]

Where [tex]a =\frac{\sqrt{km}}{2\hbar}[/tex]

I'm really have no idea on how do solve this problem. Does this solving this problem require the use of Fourier Transform?
 
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Hyperreality said:
I've recently posted a thread asking for help in the Homework forum in solving this problem, but till now I still can't figure out how do find the solution to this equation.

Here is the problem.

Show that [tex]A=(\frac{m\omega}{\hbar\pi})^{1/4}.[/tex]

From the normalisation condition

[tex]|A|^2\int_{-\infty}^{\infty} e^{-2ax^{2}}=1[/tex]

Where [tex]a =\frac{\sqrt{km}}{2\hbar}[/tex]

I'm really have no idea on how do solve this problem. Does this solving this problem require the use of Fourier Transform?

No,just the Poisson integral:
[tex]I_{1}(a)=:\int_{-\infty}^{+\infty} e^{-ax^{2}} dx =\sqrt{\frac{\pi}{a}}[/tex]

Daniel.

PS.In physics,this integral is widely used...
 
Ohhhhh...

Never heard of it That made things whole a lot simpler.
 
Hyperreality said:
Ohhhhh...

Never heard of it That made things whole a lot simpler.

Then how the heck were u supposed to do that integral??I'm sure it's about HLO in QM...You should know a lotta calculus for QM...

Daniel.
 

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