$$\int\frac{\ln(1+xy)}{1+x^2} dx$$
Give me some idea how to solve to solve this. Is it possible to use some complex analysis to solve this. Or some nice substitution will work?
$$\int\frac{\ln(1+xy)}{1+x^2} dx$$
Give me some idea how to solve to solve this. Is it possible to use some complex analysis to solve this. Or some nice substitution will work?
As is, the integral is pretty hard. We can work with its derivative with respect to $y$, however. If the integral is $f(y)$, then, assuming the integration interval is $x \in [0,\infty)$:
$$f'(y) = \int_0^{\infty} dx \frac{x}{(1+x y)(1+x^2)}$$
We can evaluate this integral using residue theory, with a keyhole contour $C$ about the positive real axis, for the following integral:
$$\oint_C dz \frac{z \log{z}}{(1+z y)(1+z^2)}$$
This integral consists of four pieces:
$$\int_{\epsilon}^R dx \frac{x \log{x}}{(1+x y)(1+x^2)}+ i R \int_0^{2 \pi} d\phi \, e^{i \phi} \frac{R e^{i \phi} (\log{R} + i \phi)}{(1+R y e^{i \phi})(1+R^2 e^{i 2 \phi})} + \\ \int_R^{\epsilon} dx \frac{x (\log{x} + i 2 \pi)}{(1+x y)(1+x^2)}+i \epsilon \int_{2 \pi}^0 d\phi \, e^{i \phi} \frac{\epsilon e^{i \phi} (\log{\epsilon} + i \phi)}{(1+ \epsilon y e^{i \phi})(1+\epsilon^2 e^{i 2 \pi})} $$
As $R \to \infty$ and $\epsilon \to 0$, the second integral vanishes as $\log{R}/R$ and the fourth integral vanishes as $\epsilon^2 \log{\epsilon}$. The contour integral is then
$$-i 2 \pi \int_0^{\infty} dx \frac{x}{(1+x y)(1+x^2)}$$
The contour integral is also equal to $i 2 \pi$ times the sum of the residues of three poles $z=\pm i$ and $z=-1/y$ of the integrand. Use the fact that, for a function $g(z)=p(z)/q(z)$, the residue of $g$ at a pole $z_0$ is $p(z_0)/q'(z_0)$ and compute the sum of the residues. Note that the factor of $i 2 \pi$ in front of the integral we seek cancels out the $i 2 \pi$ in front of the sum of the residues. Thus, the integral we seek is the negative of the sum of the residues. Thus
$$\begin{align}\int_0^{\infty} dx \frac{x}{(1+x y)(1+x^2)} &= -\underbrace{\frac{i \cdot (i \pi/2)}{(1+i y)(2 i)}}_{\text{Residue at }z=i}-\underbrace{\frac{-i \cdot (i 3 \pi/2)}{(1-i y)(-2 i)}}_{\text{Residue at }z=-i}-\underbrace{\frac{1}{y} \frac{(-1/y) (-\log{y}+i \pi)}{1+1/y^2}}_{\text{Residue at }z=-1/y}\\ &= -\frac{\log{y}}{1+y^2} + \frac{i \pi}{1+y^2} - \frac{i \pi}{4} \left [\frac{1}{1+i y}+\frac{3}{1-i y} \right ] \\ &= \frac{(\pi/2)y - \log{y}}{1+y^2}\end{align}$$
Thus
$$f'(y) = \frac{(\pi/2)y - \log{y}}{1+y^2}$$ $$f(0) = 0$$
The sought-after integral is then
$$f(y) = \int_0^{\infty} dx \frac{\log{(1+x y)}}{1+x^2} = \frac{\pi}{4} \log{(1+y^2)} + \tanh{y}\, \log{y} - \frac{y}{4} \Phi(y^2,2,1/2)$$
where $\Phi$ is the Lerch phi transcendant
$$\Phi(z,s,a) = \sum_{k=0}^{\infty} \frac{z^k}{(k+a)^s}$$