Fourier transformation of the Wavefunction in QM

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Homework Help Overview

The discussion revolves around the Fourier transformation of a wavefunction in quantum mechanics, specifically focusing on a piecewise-defined wavefunction denoted as A_0. Participants are exploring how to perform the Fourier transformation given the constraints of the problem.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are attempting to understand the implications of the piecewise definition of the wavefunction and how it affects the Fourier transformation. Questions arise regarding the integration process and the interpretation of the resulting function.

Discussion Status

Some participants have provided hints and attempted to solve the integral, while others are questioning the correctness of the results and the interpretation of variables involved in the transformation. There is an ongoing exploration of the mathematical steps required to complete the task.

Contextual Notes

There is a mention of the wavefunction being defined piecewise, which may impose constraints on the integration process. Additionally, the discussion highlights potential confusion regarding the relationship between the variables in the Fourier transformation.

B4cklfip
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Homework Statement
Given is the function phi(x) = A_0 for -L≤x≤L and phi(x) = 0 otherwise.
The task is to first sketch phi(x) as function of x. Then to calculate the fourier-transformation and sketch phi(k) as function of kL. Also I have to compare accessible Broads.
Relevant Equations
phi(k)=1/sqrt(2*pi) integral_-inf_inf (dx exp(i*k*x)*phi(x))
Hello Physics Forum,

I am not sure what to to in this task, because the wavefunction is only given as A_0. Maybe someone can explain it to me.

Thanks in Advance,
B4ckflip
 
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It says in your problem statement that <br /> \phi(x) = \begin{cases} 0 &amp; x &lt; -L \\<br /> A_0 &amp; -L \leq x \leq L \\<br /> 0 &amp; x &gt; L\end{cases}. So what is <br /> \frac{1}{\sqrt{2\pi}}\int_{-\infty}^\infty e^{ikx} \phi(x)\,dx?
 
\phi(k) = \frac{1}{\sqrt{2\pi}}\int_{-\infty}^\infty e^{ikx} \phi(x)\,dx

is the Fouriertransformation of \phi(x). It changes the dependence of the wavefunction from position x to momentum p.
 
And how would you do the integral, given that \phi(x) is defined piecewise?
 
Thanks for the hint, I now tried to solve it and got following result:

$$\tilde{\phi}(x) = \begin{cases} 0 & x < -L \\ \frac{A_0}{\sqrt{2pi}k} \cdot 2sin(kL)\ & -L \leq x \leq L \\ 0 & x > L\end{cases}$$

I have integrated from -L to L for the second interval. Is it correct ?
And how can I sketch specially phi(x) ?
 
B4cklfip said:
Thanks for the hint, I now tried to solve it and got following result:

$$\tilde{\phi}(x) = \begin{cases} 0 & x < -L \\ \frac{A_0}{\sqrt{2pi}k} \cdot 2sin(kL)\ & -L \leq x \leq L \\ 0 & x > L\end{cases}$$

I have integrated from -L to L for the second interval. Is it correct?
No, it's not correct. Note that you integrated with respect to ##x##, so ##x## doesn't appear in the final result once you plug the limits in. ##\tilde{\phi}## is not a function of ##x## but of ##k##.
 

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