Integral evaluation - analytical vs. numerical

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Discussion Overview

The discussion revolves around the evaluation of the integral \(\int_{-\infty}^{\infty}\cosh(x)^{-n}dx\) for different values of \(n\), specifically contrasting integer values with non-integer values. Participants explore the analytical versus numerical evaluation of this integral, particularly in the context of its application in Quantum Mechanics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants suggest that the residue theorem from complex analysis allows for an exact expression when \(n\) is an integer, while this method may not apply for non-integer values.
  • One participant provides an expression for the integral when \(n\) is complex, noting that the result is multiplied by 2.
  • There is a discussion about discrepancies in factors, particularly the "1/2" factor, with participants questioning whether the integration was performed over the entire domain or only half.
  • Another participant explains that the gamma function is expressible in terms of elementary functions for whole and half integers, but requires numerical methods for arbitrary values.
  • Some participants mention that both beta and gamma functions are tabulated for certain ranges, implying that the integral can be solved analytically under specific conditions.
  • There is a contention regarding the usefulness of distinguishing between analytical solutions based on the naming of special functions.

Areas of Agreement / Disagreement

Participants express differing views on the nature of analytical versus numerical solutions, with no consensus reached on the implications of these distinctions. The discussion remains unresolved regarding the broader significance of these findings.

Contextual Notes

Limitations include the dependence on the definitions of special functions and the conditions under which the integral can be evaluated. Some assumptions about the convergence and domains of integration are also noted but not fully resolved.

broegger
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Hi,

Does anyone know a reason why [tex]\int_{-\infty}^{\infty}\cosh(x)^{-n}dx[/tex] (n>0) can be evaluated analytically when n = 1,2,3,..., but only numerically when n is non-integer. I don't know if there is a "reason", but I'm using this result in a Quantum Mechanics project and it would be cool if I could give some kind of intuitive reason why this is so.
 
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My best guess:
You may use the residue theorem from complex analysis to gain an exact expression in the case of integer values, whereas this won't work if you have a non-integer.
I might be wrong, though..
 
I've attached the antiderivative and here's your integral

[tex]\int_{-\infty}^{+\infty} \frac{dx}{\cosh^{n} x}=\frac{\sqrt{\pi}}{2}\frac{\Gamma \left(\frac{n}{2}\right)}{\Gamma \left(\frac{n+1}{2}\right)}[/tex]

"n" can be complex,even.

Daniel.

EDIT:The correct result is multiplied by 2.See posts #4 & #7.
 

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Last edited:
O.K, in Mathematica I go that if [itex]\Re (n) > 0[/itex] then:

[tex]\int_{-\infty}^{+\infty} \cosh^{-n} (x) dx = \frac{ \sqrt{\pi} \, \Gamma\left( \frac{n}{2} \right)}{ \Gamma\left( \frac{n + 1}{2} \right)}[/tex]
 
How do you explain the "1/2" factor discrepancy...?

Daniel.

EDIT:See post #7 for details.
 
Last edited:
dextercioby said:
How do you explain the "1/2" factor discrepancy...?

Danie.
Well if I left n=1 and integrate in mathematica I get [itex]\pi[/itex] and:

[tex]\Gamma \left( \frac{1}{2} \right) = \sqrt{\pi}[/tex]

Are you sure you did not integrate between 0 and Infinity?
 
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I got it,i plugged only for half a domain

Using [1]

[tex]\int_{0}^{+\infty} \frac{\sinh^{\mu}x}{\cosh^{\nu}x} \ dx =\frac{1}{2}B\left(\frac{\mu +1}{2},\frac{\nu-\mu}{2}\right)[/tex] (1)

,provided that

[tex]\mbox{Re} \left(\mu\right) >-1 \ ; \ \mbox{Re} \left(\mu-\nu\right) <0[/tex] (2)

Making [itex]\mu=0[/itex] (3) in (1) (admissible according to (2) and implying the condition [itex]\mbox{Re} (\nu) >0[/itex] (4) ),one gets

[tex]\int_{0}^{\infty} \frac{dx}{\cosh^{\nu} x} \ dx =\frac{1}{2} B\left(\frac{1}{2},\frac{\nu}{2}\right)=\frac{1}{2}\frac{\Gamma \left(\frac{1}{2}\right)\Gamma \left(\frac{\nu}{2}\right)}{\Gamma\left(\frac{\nu+1}{2}\right)}[/tex] (5)

Using

[tex]\Gamma\left(\frac{1}{2}\right)=\sqrt{\pi}[/tex] (6)

and

[tex]\int_{\mathbb{R}} \frac{dx}{\cosh^{\nu} x} \ dx =2 \int_{0}^{\infty} \frac{dx}{\cosh^{\nu} x} \ dx[/tex] (7)

,one gets exactly the formula posted by Zurtex.

Daniel.

--------------------------------------------------
[1]G & R,5-th edition,Academic Press,CD version,1996,page 388,formula 3.512-2.
 
Zurtex said:
Well if I left n=1 and integrate in mathematica I get [itex]\pi[/itex] and:

[tex]\Gamma \left( \frac{1}{2} \right) = \sqrt{\pi}[/tex]

Are you sure you did not integrate between 0 and Infinity?

Yes,i used an online integrator and indeed integrated only half of the domain.

I'll edit and make a reference to your post & mine just above.

Daniel.
 
So just in case anyone is at all unclear about how this relates to the original observation that :
Does anyone know a reason why [tex]\int_{-\infty}^{\infty}\cosh(x)^{-n}dx[/tex] (n>0) can be evaluated analytically when n = 1,2,3,..., but only numerically when n is non-integer.

It's because [tex]\Gamma(x)[/tex] is easily expressable in terms of elementary functions and constants for whole and half integers but generally needs other forms of numerical calulation for arbitrary values of "x".
 
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  • #10
Incidentally,both beta & gamma-Euler are tabulated for a certain range of values of their arguments.

So the integral is solvable analytically.Expressing its values in terms of analytical special functions means just that.

Daniel.
 
  • #11
dextercioby said:
So the integral is solvable analytically.Expressing its values in terms of analytical special functions means just that.
That means that whether an integral has an analytical solution or not is based on convention (how many special functions are named). I don't find such a distinction very useful. I would echo uart's comment.
 
  • #12
Thanks y'all. I've included a bit about the gamma function, interesting stuff...
 

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