Integration of abs(k)e^(ikx)dk

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The discussion centers on the integration of the expression abs(k)e^(ikx)dk, where participants explore splitting the integral to simplify calculations. There is uncertainty regarding the application of boundary conditions, particularly the decision to integrate from 0 to a instead of -a to a to eliminate the absolute value. A suggestion is made to redefine the variable for better clarity in the integration limits. The conversation highlights the importance of recognizing the evenness of the function versus the integrand, emphasizing that doubling the integral may not be valid due to the integrand's properties. Overall, the integration process and boundary conditions remain key points of contention.
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Homework Statement
This is for a quantum free particle problem, doing the Fourrier transform and I just want to make sure I've got the integral correct.
Relevant Equations
$$\frac{1}{\sqrt{2\pi}}\int^{\infty}_{-\infty} \phi (k) e^{ikx}dk$$


Where ##\phi## is:
$$

f\left(k\right) = \left\{

\begin{array}{lr}

A(a-|k|) & : |k| \le a\\

0 & : |k| > a

\end{array}

\right.\\

$$
Split the integral
$$\frac{Aa}{\sqrt{2\pi}}\int^{\infty}_{-\infty}e^{ikx}dk - \frac{A}{\sqrt{2\pi}}\int^{\infty}_{-\infty}|k|e^{ikx}dk$$

Apply the boundary conditions, this is where my biggest source of uncertainty comes from I doubled the integral and integrated from 0 to a instead of from -a to +a to get rid of that absolute value. I plotted the |k|e^k function and it appears to have even parity.

$$\frac{Aa}{\sqrt{2\pi}}\int^{a}_{-a}e^{ikx}dk - \frac{2A}{\sqrt{2\pi}}\int^{a}_{0}|k|e^{ikx}dk$$

$$\frac{Aa}{\sqrt{2\pi}ix}(e^{iax} - e^{-iax}) + \frac{2Ai}{\sqrt{2\pi}x}[ke^{ikx}-\frac{1}{ix}e^{ikx}]^a_0$$

$$\frac{Aa}{\sqrt{2\pi}ix}(e^{iax} - e^{-iax}) - \frac{2A}{\sqrt{2\pi}ix}(ae^{iax}-0 - \frac{1}{ix}(e^{iax}-1))$$

$$\frac{Aa}{\sqrt{2\pi}ix}(e^{iax}-e^{-iax}-2e^{iax}) - \frac{2A}{\sqrt{2\pi}(ix)^2}(e^{iax}-1)$$

Clean up and use Euler
$$\frac{2iAa}{\sqrt{2\pi}x}cos(ax) + \frac{2A}{\sqrt{2\pi}x^2}(e^{iax}-1)$$
 
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Hi,

rmiller70015 said:
Apply the boundary conditions, this is where my biggest source of uncertainty comes from I doubled the integral and integrated from 0 to a instead of from -a to +a to get rid of that absolute value
If you have to split anyway, why not write ##\phi = a+k ## from -a to 0 and ##\phi = a-k ## from 0 to a ?

Are you somewhat familiar with the FT ? Since your ##\phi## is a convolution of a boxcar in time (6) with itself, I would expect (14) something like a ##\displaystyle {\ {sin^2 x\over x^2}}\ ## for ##\psi ##.

##\ ##
 
Mathematica yields a simpler result (this one's wrong):
$$\frac{2A}{\sqrt{2\pi}} \frac{1-e^{iax}+iax}{x^2}.$$ On the other hand, if I evaluate the integral using the InverseFourierTransform function, I get a result like @BvU's expectation.

You can't double the integral from 0 to ##a## because while ##f(k)## is even, the integrand as a whole isn't.
 
Last edited:
First, I tried to show that ##f_n## converges uniformly on ##[0,2\pi]##, which is true since ##f_n \rightarrow 0## for ##n \rightarrow \infty## and ##\sigma_n=\mathrm{sup}\left| \frac{\sin\left(\frac{n^2}{n+\frac 15}x\right)}{n^{x^2-3x+3}} \right| \leq \frac{1}{|n^{x^2-3x+3}|} \leq \frac{1}{n^{\frac 34}}\rightarrow 0##. I can't use neither Leibnitz's test nor Abel's test. For Dirichlet's test I would need to show, that ##\sin\left(\frac{n^2}{n+\frac 15}x \right)## has partialy bounded sums...