How Do You Evaluate Complex Contour Integrals with Sinusoidal Functions?

riemannian
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greetings , we have the following integral :

I(x)=\lim_{T\rightarrow \infty}\frac{1}{2\pi i}\int_{\gamma-iT}^{\gamma+iT}\sin(n\pi s)\frac{x^{s}}{s}ds

n is an integer . and \gamma >1

if x>1 we can close the contour to the left . namely, consider the contour :

C_{a}=C_{1}\cup C_{2}\cup C_{3}\cup C_{4}

where :

C_{1}=\left [ \gamma-iT,\gamma+iT \right ]

C_{2}=\left [ \gamma+iT,-U+iT \right ]

C_{3}=\left [ -U+iT ,-U-iT \right ]

C_{4}=\left [ -U-iT ,\gamma-iT \right ]

and U>>\gamma
then by couchy's theorem :

I(x)=I_{1}+I_{2}+I_{3}+I_{4}=0

if x<1, we can close the contour to the right via the following contour :

C_{b}=C_{1}\cup C_{2}\cup C_{3}\cup C_{4}

C_{1}=\left [ \gamma-iT,\gamma+iT \right ]

C_{2}=\left [ \gamma+iT,U+iT \right ]

C_{3}=\left [ U+iT ,U-iT \right ]

C_{4}=\left [ U-iT ,\gamma-iT \right ]

then also by couchy's theorem :

I(x)=0

the plan is to give an estimate of the integrals along the segments of the rectangular contour, and calculate I_{1} in both cases via the result obtained by cauchy's theorem . however, i don't have the first clue on how to do that, hence the quest !
 
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riemannian said:
then by couchy's theorem :
I(x)=I_{1}+I_{2}+I_{3}+I_{4}=0
I don't think you mean that. Yes, by Cauchy, I_{1}+I_{2}+I_{3}+I_{4}=0, but the challenge is to show that three of these tend to 0 as T tends to infinity, and therefore the fourth (the one that tends to I(x)) does too.
I got stuck trying to put some bound on sin(s). When s = c+id has a large imaginary component, id, this grows like exp(d). I tried pairing up the negative imaginary points with the positive ones, e.g. doing C3 as the integral from -U to -U+iT of {f(s) - f(complex conjugate of s)}.dt, hoping to get some cancellation. No luck.
 
haruspex said:
I don't think you mean that. Yes, by Cauchy, I_{1}+I_{2}+I_{3}+I_{4}=0, but the challenge is to show that three of these tend to 0 as T tends to infinity, and therefore the fourth (the one that tends to I(x)) does too.
I got stuck trying to put some bound on sin(s). When s = c+id has a large imaginary component, id, this grows like exp(d). I tried pairing up the negative imaginary points with the positive ones, e.g. doing C3 as the integral from -U to -U+iT of {f(s) - f(complex conjugate of s)}.dt, hoping to get some cancellation. No luck.

yes, sorry .. it was a typo . and i was trying to do exactly the same , no luck :cry:

remark : the integral of question bears resemblance to the perron's integral, and could be thought of as a laplace inverse of \frac{\sin(n\pi s)}{s}, with \ln x as the variable in the 'time' domain.
 
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