Stieltjes integral I

In this post we would like to illustrate the calculation of an integral using perturbation techniques. We would like to calculate the following Stieltjes integral:

\displaystyle I = \int_{0}^{\infty} \frac{e^{-t}}{1+t}dt

This integral can be evaluated exactly (I = 0.5963), but we’ll use perturbation techniques to compare the results obtained using these approximation techniques with the exactly calculated value. In order to do so, we will insert the parameter \epsilon as follows:

\displaystyle I(\epsilon) = \int_{0}^{\infty} \frac{e^{-t}}{1+\epsilon^2t}dt

For \epsilon = 0 we have I(\epsilon) = 1. This is the solution to the unperturbed problem. We observe that:

\displaystyle \frac{1}{1-x} = 1 + x + x^2 + ...
\displaystyle = 1 + x + x^2 + ... + x^n + x^{n+1}(1 + x + x^2 + ...)
\displaystyle =  1 + x + x^2 + ... + x^n + \frac{x^{n+1}}{1-x}

Defining x := -\epsilon^2 t and using \int_{0}^{\infty} e^{-t} t^n dt = n! in the formula above we obtain:

\displaystyle \frac{1}{1 +\epsilon^2t} =  1 -\epsilon^2 t   + \epsilon^4 t^2 + ... + (-1)^n \epsilon^{2n} t^{n} + \frac{(-1)^{n+1} \epsilon^{2n+2} t^{n+1}}{1+\epsilon^2 t}
\displaystyle I(\epsilon) = \int_{0}^{\infty} e^{-t}(1 -\epsilon^2 t + \epsilon^4 t^2 + ... + (-1)^n \epsilon^{2n} t^{n} + \frac{(-1)^{n+1} \epsilon^{2n+2} t^{n+1}}{1 + \epsilon^2 t}) dt
\displaystyle = \int_{0}^{\infty} (e^{-t} -\epsilon^2 e^{-t} t + \epsilon^4 e^{-t} t^2 + ... + (-1)^n \epsilon^{2n} e^{-t} t^{n} + \frac{(-1)^{n+1} \epsilon^{2n+2} e^{-t} t^{n+1}}{1 + \epsilon^2 t}) dt
\displaystyle = 1 - \epsilon^2 + \epsilon^4 2! + ... + (-1)^{n}\epsilon^{2n} n! + (-1)^{n+1} \epsilon^{2n+2} I_{n+1}(\epsilon)

where I_{n+1}(\epsilon) := \int_{0}^{\infty} \frac{e^{-t} t^{n+1}}{1 + \epsilon^2 t} dt. Finally we have:

\displaystyle I(\epsilon) = \sum_{k=0}^{n} (-1)^{k} \epsilon^{2k} k! + (-1)^{n+1} \epsilon^{2n+2} I_{n+1}(\epsilon)

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