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\begin{align}&\totald{}{\alpha}\int_{0}^{1}
\ln\pars{\Gamma\pars{x + \alpha}}\,\dd x
=\int_{0}^{1}\partiald{\ln\pars{\Gamma\pars{x + \alpha}}}{\alpha}\,\dd x
=\int_{0}^{1}\partiald{\ln\pars{\Gamma\pars{x + \alpha}}}{x}\,\dd x
\\[3mm]&=\ln\pars{\Gamma\pars{1 + \alpha} \over \Gamma\pars{\alpha}}
=\ln\pars{\alpha}
\end{align}
\begin{align}&\int_{0}^{1}\ln\pars{\Gamma\pars{x + \alpha}}\,\dd x
=\alpha\ln\pars{\alpha} - \alpha + \int_{0}^{1}\ln\pars{\Gamma\pars{x}}\,\dd x
\end{align}
\begin{align}&\int_{0}^{1}\ln\pars{\Gamma\pars{x}}\,\dd x
=\int_{0}^{1}\ln\pars{\Gamma\pars{1 - x}}\,\dd x
=\int_{0}^{1}\ln\pars{\pi \over \Gamma\pars{x}\sin\pars{\pi x}}\,\dd x
\\[3mm]&=\ln\pars{\pi} - \int_{0}^{1}\ln\pars{\sin\pars{\pi x}}\,\dd x
-\int_{0}^{1}\ln\pars{\Gamma\pars{x}}\,\dd x
\end{align}
\begin{align}&\int_{0}^{1}\ln\pars{\Gamma\pars{x}}\,\dd x
=\half\,\ln\pars{\pi}
-{1 \over 2\pi}\
\underbrace{\int_{0}^{\pi}\ln\pars{\sin\pars{x}}\,\dd x}_{\ds{-\pi\ln\pars{2}}}
=\half\,\ln\pars{2\pi}
\end{align}
La anterior $\ds{\ul{\ln\pars{\sin\pars{\cdots}}\!\mbox{-integral}}}$ es un resultado conocido y aparece con frecuencia en M. SE.
$$\color{#66f}{\large%
\int_{0}^{1}\ln\pars{\Gamma\pars{x + \alpha}}\,\dd x
={\ln\pars{2\pi} \over 2} + \alpha\ln\pars{\alpha} - \alpha}
$$