Evaluate $\int_0^\infty{\frac{\ln x \sin x}{x}dx}$ Evaluate$$\int_0^\infty{\frac{\ln x \sin x}{x}dx}$$
I don't know where to start with this integral. Mathematica shows that $-\frac{\gamma\pi}2$ is the answer, so I don't think that it is easy to be solved.
 A: 
I thought it might be instructive to present another approach that uses real analysis only, which complement my answer using contour integration (SEE THIS ANSWER).  We shall make use of Frullani's integral.  To that end we proceed.


Note that from Frullani's Integral we have
$$\log(x)=\int_0^\infty \frac{e^{-t}-e^{-xt}}{t}\,dt\tag1$$

Using $(1)$, we can write the integral of interest as
$$\begin{align}
\int_0^\infty \frac{\log(x)\sin(x)}{x}\,dx&=\int_0^\infty\left(\int_0^\infty \frac{e^{-t}-e^{-xt}}{t}\,dt\right) \frac{\sin(x)}{x}\,dx\\\\
&=\int_0^\infty \frac1t \color{blue}{\int_0^\infty \frac{\sin(x)}{x}(e^{-t}-e^{-xt})\,dx} \,dt\\\\
&=\int_0^\infty \frac1t\color{blue}{\left(\frac\pi2e^{-t}-\pi/2+\arctan(t)\right)}\,dt\tag2
\end{align}$$

Integrating by parts the integral on the right-hand side of $(2)$ with $u=\frac\pi2e^{-t}-\pi/2+\arctan(t)$ and $v=\frac1t$ reveal
$$\begin{align}
\int_0^\infty \frac1t\color{blue}{\left(\frac\pi2e^{-t}-\pi/2+\arctan(t)\right)}\,dt&=-\int_0^\infty \log(t)\color{blue}{\left(-\frac\pi2 e^{-t}+\frac1{t^2+1}\right)}\,dt\\\\
&=-\frac\pi2\gamma
\end{align}$$
since $$\int_0^\infty \frac{\log(t)}{t^2+1}\,dt\overbrace{=}^{t\mapsto1/t}\int_0^\infty \frac{\log(1/t)}{t^2+1}\,dt\implies \int_0^\infty \frac{\log(t)}{t^2+1}\,dt=0$$
A: It is pretty straightforward: the Laplace transform of $\sin(x)$ is $\frac{1}{s^2+1}$ and the inverse Laplace transform of $\frac{\log x}{x}$ is $-\gamma-\log(s)$, hence
$$ \int_{0}^{+\infty}\frac{\log(x)\sin(x)}{x}\,dx = \int_{0}^{+\infty}\frac{-\gamma-\log(s)}{1+s^2}\,ds = -\frac{\gamma\pi}{2} $$
since $\int_{0}^{+\infty}\frac{\log s}{1+s^2}\,ds$ vanishes by symmetry ($s\mapsto \frac{1}{s}$).
A: 
I wanted to present a way forward using contour integration that is complementary to the real analysis solution I presented earlier HERE.  To the end, we proceed.


Using the principal value of the complex logarithm, Cauchy's Integral Theorem Guarantees that for $0<\epsilon<R$
$$\begin{align}
0&=\int_\epsilon^R \frac{e^{ix}\log(x)}{x}\,dx+\int_0^{\pi/2}\frac{e^{iRe^{i\phi}}\log(Re^{i\phi})}{Re^{i\phi}}\,iRe^{i\phi}\,d\phi\\\\
&+\int_R^\epsilon \frac{e^{-x}\log(ix)}{ix}\,i\,dx+\int_{\pi/2}^0\frac{e^{i\epsilon e^{i\phi}}\log(\epsilon e^{i\phi})}{\epsilon e^{i\phi}}\,i\epsilon e^{i\phi}\,d\phi\tag 1
\end{align}$$

For the second integral on the right-and side of $(1)$, we find that 
$$\begin{align}
\left|\int_0^{\pi/2}\frac{e^{iRe^{i\phi}}\log(Re^{i\phi})}{Re^{i\phi}}\,iRe^{i\phi}\,d\phi\right|&\le \int_0^{\pi/2}|\log(R)+i\phi|e^{-R\sin(\phi)}\,d\phi\\\\
&\le (\log(R)+\pi/2) \int_0^{\pi/2}e^{-2R\phi/\pi}\,d\phi\\\\
&=(\log(R)+\pi/2) \left(\frac{1-e^{-R}}{2R/\pi}\right)\tag2
\end{align}$$
which clearly vanishes in the limit as $R\to\infty$.

For the fourth integral on the right-and side of $(1)$, we find that 
$$\begin{align}
\text{Im}\left(\int_{\pi/2}^0\frac{e^{i\epsilon e^{i\phi}}\log(\epsilon e^{i\phi})}{\epsilon e^{i\phi}}\,i\epsilon e^{i\phi}\,d\phi\right)&=-\frac\pi2\log(\epsilon)+O(\epsilon\log(\epsilon))\tag3
\end{align}$$

Hence, taking the imaginary part of $(1)$ and letting $R\to \infty$ and $\epsilon\to 0$ and using $(2)$ and $(3)$ reveals
$$\begin{align}
\int_0^\infty \frac{\log(x)\sin(x)}{x}\,dx= \frac\pi2 \lim_{\epsilon\to 0}\left(\int_\epsilon^\infty \frac{e^{-x}}{x}\,dx +\log(\epsilon)\right)\tag4
\end{align}$$
Finally, integrating by parts the integral on the right-hand side of $(4)$ with $u=e^{-x}$ and $v=\log(x)$ yields
$$\begin{align}
\int_0^\infty \frac{\log(x)\sin(x)}{x}\,dx&=\frac\pi2\lim_{\epsilon\to 0}\left(-e^{-\epsilon}\log(\epsilon)+\int_\epsilon^\infty \log(x)e^{-x}\,dx+\log(\epsilon)\right)\\\\
&=\frac\pi2 \int_0^\infty \log(x)e^{-x}\,dx\\\\
&=-\frac\pi2\gamma
\end{align}$$
as was to be shown!
A: Not exactly a full answer, but if you treat this integral as the Mellin transform (from $x$ to $s$) of $\log(x)\sin(x)$, Mathematica gives the result, 
$$
\mathcal{M}_{x\to s}[\log(x) \sin(x)] = \frac{\pi}{2}\cos\left(\frac{\pi s}{2}\right)\Gamma(s) + \Gamma(s) \psi_0(s)\sin\left(\frac{\pi s}{2}\right)
$$
this can be found on page 318 (pdf page 330), under entry (13), of this book. When $s=0$, we reclaim the integral you had, but this result diverges. If we take the limit $s \to 0$, we get $-\frac{\gamma \pi}{2}$.
