Undergrad Integral of e^(ikx^3): Write as Line Integral from 0 to $\infty$

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Show that $$\int_0^\infty dx\exp(ikx^3) , k>0$$ may be written as integral from 0 to ##\infty## along the line ##arg(z) = \frac{\pi}{6}##.

I'd appreciate it if you can help me how to approach this problem. My initial impression was to expand the integrand out
$$\sum^{\infty}_{n=0}\frac{(ikx^3)^n}{n!}$$
but did not how to obtain the ##arg(z)## condition. I plugged the integral in wolframalpha and gave me an expression with a Gamma function, which the lecture has covered but I'm not sure how to apply here.

Thanks
 
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spacetimedude said:
Show that $$\int_0^\infty dx\exp(ikx^3) , k>0$$ may be written as integral from 0 to ##\infty## along the line ##arg(z) = \frac{\pi}{6}##.

I'd appreciate it if you can help me how to approach this problem. My initial impression was to expand the integrand out
$$\sum^{\infty}_{n=0}\frac{(ikx^3)^n}{n!}$$
but did not how to obtain the ##arg(z)## condition. I plugged the integral in wolframalpha and gave me an expression with a Gamma function, which the lecture has covered but I'm not sure how to apply here.

Thanks
Which expression in terms of the gamma-function do you get from the substitution ##t = -ikx^3\,##?
 
fresh_42 said:
Which expression in terms of the gamma-function do you get from the substitution ##t = -ikx^3\,##?

Wolfram says $$\frac{\Gamma(\frac{4}{3})}{\sqrt[3]{-ik}}.$$
I have been told that using ##i=\exp(i\frac{\pi}{2})## helps but I can only get as far as writing the integrand as ##\exp(\exp(i\frac{\pi}{2})kx^3))## and not sure what to do after.
 
spacetimedude said:
Wolfram says $$\frac{\Gamma(\frac{4}{3})}{\sqrt[3]{-ik}}.$$
I have been told that using ##i=\exp(i\frac{\pi}{2})## helps but I can only get as far as writing the integrand as ##\exp(\exp(i\frac{\pi}{2})kx^3))## and not sure what to do after.
That wasn't my question. I've asked what do you get, not WolframAlpha. The substitution of ##i## might help to properly calculate the powers of ##i## but I'd rather write ##k=ic## to begin. In any case one has to be cautious with the handling of the purely imaginary constants.

The substitution ##t \mapsto -ikx^3## allows to write ##x## as power of ##t## as well as the integral in terms of the gamma function.
 
I think the exercise asks not to compute the value of the integral but to express it as a contour integral with the contour being the line ##arg(z)=\frac{\pi}{6}##.
 
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Delta² said:
I think the exercise asks not to compute the value of the integral but to express it as a contour integral with the contour being the line ##arg(z)=\frac{\pi}{6}##.
Yes, the expression is what I am looking for.
I am solving one of the past exam papers for my university and it is the first part of the question.
 

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fresh_42 said:
That wasn't my question. I've asked what do you get, not WolframAlpha. The substitution of ##i## might help to properly calculate the powers of ##i## but I'd rather write ##k=ic## to begin. In any case one has to be cautious with the handling of the purely imaginary constants.

The substitution ##t \mapsto -ikx^3## allows to write ##x## as power of ##t## as well as the integral in terms of the gamma function.
Okay, so I am looking for the expression of the contour integral as Delta said. I allowed ##i=\exp(i\frac{\pi}{2})## and extend the integral to z space. Then let ##z=r\exp(i\theta)##, yielding
$$ \int _C dz e^{{kr^2e^{i(\pi/2+3\theta)}}}.$$

Do you think this is correct so far? Maybe ##z=r\exp(i\theta)## is unnecessary.
 
Last edited:
What I have now is:
Choose ##z=re^{i\pi/6}## so ##dz=e^{i\pi/6}dr##. Plug in the integral ->
$$e^{i\pi/6}\int^\infty_{-\infty} e^{ikr^3e^{i\pi/2}}$$ and note ##e^{i\pi/2}=i##
Finally, the integral becomes $$e^{i\pi/6}\int^\infty_{-\infty} e^{-kr^3}.$$
Does this seem right?
 
The limits of integration should be from 0 to ##+\infty## (the contour is the positive part of the line ##z=re^{i\pi/6}##.

However in order to be rigorous and clear you have to provide a function ##f:\mathbb{C}->\mathbb{C}## such that
##\int_0^{\infty}f(z(r))z'(r)dr=\int_0^{\infty}e^{ikr^3}dr##
 

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