Evaluación de $\int_0^1 \frac{\log(1+x)}{1+x}\log\left(\log\left(\frac{1}{x}\right)\right) \, dx$

Question

Necesito algunos consejos, pistas para conseguir la forma cerrada de

$$\int_0^1 \frac{\log(1+x)}{1+x}\log\left(\log\left(\frac{1}{x}\right)\right) \, dx$$

Answer 1

$\newcommand{\+}{^{\daga}} \newcommand{\ángulos}[1]{\left\langle\, nº 1 \,\right\rangle} \newcommand{\llaves}[1]{\left\lbrace\, nº 1 \,\right\rbrace} \newcommand{\bracks}[1]{\left\lbrack\, nº 1 \,\right\rbrack} \newcommand{\ceil}[1]{\,\left\lceil\, nº 1 \,\right\rceil\,} \newcommand{\dd}{{\rm d}} \newcommand{\down}{\downarrow} \newcommand{\ds}[1]{\displaystyle{#1}} \newcommand{\expo}[1]{\,{\rm e}^{#1}\,} \newcommand{\fermi}{\,{\rm f}} \newcommand{\piso}[1]{\,\left\lfloor #1 \right\rfloor\,} \newcommand{\mitad}{{1 \over 2}} \newcommand{\ic}{{\rm i}} \newcommand{\iff}{\Longleftrightarrow} \newcommand{\imp}{\Longrightarrow} \newcommand{\isdiv}{\,\left.\a la derecha\vert\,} \newcommand{\cy}[1]{\left\vert #1\right\rangle} \newcommand{\ol}[1]{\overline{#1}} \newcommand{\pars}[1]{\left (\, nº 1 \,\right)} \newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\parcial #3^{#1}}} \newcommand{\pp}{{\cal P}} \newcommand{\raíz}[2][]{\,\sqrt[#1]{\vphantom{\large Un}\,#2\,}\,} \newcommand{\sech}{\,{\rm sech}} \newcommand{\sgn}{\,{\rm sgn}} \newcommand{\totald}[3][]{\frac{{\rm d}^{#1} #2}{{\rm d} #3^{#1}}} \newcommand{\ul}[1]{\underline{#1}} \newcommand{\verts}[1]{\left\vert\, nº 1 \,\right\vert} \newcommand{\wt}[1]{\widetilde{#1}}$ $\ds{\int_{0}^{1}{\ln\pars{1 + x} \over 1 + x}\ln\pars{\ln\pars{1 \over x}} \,\dd x:\ {\large ?}}$

\begin{align}&\overbrace{\color{#c00000}{% \int_{0}^{1}{\ln\pars{1 + x} \over 1 + x}\ln\pars{\ln\pars{1 \over x}}\,\dd x}} ^{\ds{\mbox{Set}\ x \equiv \expo{-t}\ \imp\ t = \ln\pars{x}}}\ =\ \int_{\infty}^{0}{\ln\pars{1 + \expo{-t}} \over 1 + \expo{-t}}\,\ln\pars{t}\, \pars{-\expo{-t}\,\dd t} \\[3 mm]&=\lim_{\mu \-1}\partiald{}{\mu}\color{#00f}{\int_{0}^{\infty}\ln\pars{t}\expo{-t} \pars{1 + \expo{-t}}^{\mu}\,\dd t} \end{align}

\begin{align}&\color{#00f}{\int_{0}^{\infty}\ln\pars{t}\expo{-t} \pars{1 + \expo{-t}}^{\mu}\,\dd t} =\sum_{n = 0}^{\infty}{\mu \elegir n}\int_{0}^{\infty} \ln\pars{t}\expo{-\pars{n + 1}t}\,\dd t \\[3 mm]&=\sum_{n = 0}^{\infty}{-\mu + n - 1 \elegir n}\pars{-1}^{n}\lim_{\epsilon \to 0}\partiald{}{\epsilon}\int_{0}^{\infty}t^{\epsilon}\expo{-\pars{n + 1}t} \,\dd t \\[3 mm]&=\sum_{n = 0}^{\infty}{-\mu + n - 1 \elegir n}\pars{-1}^{n}\lim_{\epsilon \to 0}\partiald{}{\epsilon} \bracks{{1 \over \pars{n + 1}^{\epsilon + 1}} \int_{0}^{\infty}t^{\epsilon}\expo{-t}\,\dd t} \\[3 mm]&=\sum_{n = 0}^{\infty}{-\mu + n - 1 \elegir n}\pars{-1}^{n}\lim_{\epsilon \to 0}\partiald{}{\epsilon} \bracks{{\Gamma\pars{\epsilon + 1} \\pars{n + 1}^{\epsilon + 1}}} \\[3 mm]&=-\sum_{n = 0}^{\infty}{-\mu + n - 1 \elegir n}\pars{-1}^{n}\, {\ln\pars{n + 1} + \gamma \más de n + 1} \end{align}

También, $$ \lim_{\mu \a - 1}\partiald{}{\mu}{-\mu + n - 1 \elegir n} =-\Psi\pars{n + 1} - \gamma $$

tal que \begin{align}&\color{#c00000}{% \int_{0}^{1}{\ln\pars{1 + x} \over 1 + x}\ln\pars{\ln\pars{1 \over x}}\,\dd x} =-\sum_{n = 1}^{\infty}\pars{-1}^{n}\, {\bracks{\gamma + \Psi\pars{n}}\bracks{\gamma + \ln\pars{n}} \over n} \\[3 mm]&=-\gamma^{2} \sum_{n = 1}^{\infty}{\pars{-1}^{n} \over n} -\gamma\sum_{n = 1}^{\infty}\pars{-1}^{n}\,{\ln\pars{n} \over n} -\gamma\sum_{n = 1}^{\infty}\pars{-1}^{n}\,{\Psi\pars{n} \over n} -\sum_{n = 1}^{\infty}\pars{-1}^{n}\,{\Psi\pars{n}\ln\pars{n} \over n} \end{align}

Con \begin{align} \sum_{n = 1}^{\infty}{\pars{-1}^{n} \over n} & = -\ln\pars{2} \\ \sum_{n = 1}^{\infty}\pars{-1}^{n}\,{\ln\pars{n} \over n}&= \gamma\ln\pars{2} - \media\,\ln^{2}\pars{2} \\[3 mm] \sum_{n = 1}^{\infty}\pars{-1}^{n}\,{\Psi\pars{n} \over n}&= \gamma\ln\pars{2} + \media\,\ln^{2}\pars{2} \end{align}

vamos a tener \begin{align}&\color{#66f}{\large% \int_{0}^{1}{\ln\pars{1 + x} \over 1 + x}\ln\pars{\ln\pars{1 \over x}}\,\dd x} \\[3 mm]&=\color{#66f}{\large-\gamma^{2}\ln\pars{2} -\sum_{n = 1}^{\infty}\pars{-1}^{n}\,{\Psi\pars{n}\ln\pars{n} \over n}} \aprox -0.2408 \end{align}

$\ds{\tt% \mbox{hasta el momento, yo no era capaz de evaluar la última suma. Todavía estoy tratando de}\ldots}$.

Parece relacionados de alguna manera a un Euler Suma.

Answer 2

Sustituto $x\mapsto e^{-x}$ y $x\mapsto x/n$: $$ \begin{align}\hspace{-1cm} \int_0^1\frac{\log(1+x)}{1+x}\log(\log(1/x))\,\mathrm{d}x &=\int_0^\infty\frac{\log(1+e^{-x})}{1+e^{-x}}\log(x)\,e^{-x}\,\mathrm{d}x\\ &=\sum_{n=2}^\infty\int_0^\infty(-1)^nH_{n-1}e^{-nx}\log(x)\,\mathrm{d}x\\ &=\sum_{n=2}^\infty\int_0^\infty(-1)^n\frac{H_{n-1}}ne^{-x}(\log(x)-\log(n))\,\mathrm{d}x\\ &=\sum_{n=2}^\infty(-1)^n\frac{H_{n-1}}n(-\gamma\log(n))\etiqueta{1} \end{align} $$ El uso de $(3)$ de esta respuesta, obtenemos $$ \begin{align} \sum_{n=2}^\infty(-1)^n\frac{H_{n-1}}n &=\frac{\zeta(2)}{2}-\sum_{n=1}^\infty(-1)^{n-1}\frac{H_n}n\\ &=\frac12\log(2)^2\etiqueta{2} \end{align} $$ Por lo tanto, obtenemos que $(1)$ es $$ -\frac\gamma2\log(2)^2-\sum_{n=2}^\infty(-1)^n\frac{H_{n-1}}n\log(n)\etiqueta{3} $$

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Comparación con Felix Marin Respuesta

Usando $(8)$ de esta respuesta, obtenemos $$ \begin{align} \sum_{n=2}^\infty(-1)^n\frac{H_{n-1}}n\log(n) &=\sum_{n=2}^\infty(-1)^n\frac{\psi(n)+\gamma}n\log(n)\\ &=\sum_{n=2}^\infty(-1)^n\frac{\psi(n)}n\log(n)+\gamma^2\log(2)-\gamma\frac{\log(2)^2}{2}\la etiqueta{4} \end{align} $$ Por lo tanto, el taponamiento de $(4)$ en $(3)$, vemos que $(1)$ es $$ -\gamma^2\log(2)-\sum_{n=2}^\infty(-1)^n\frac{\psi(n)}n\log(n)\etiqueta{5} $$ que es el mismo que Félix Marín consigue.

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Más Investigación

Quizás el siguiente paso es considerar la derivada de $$ \sum_{n=2}^\infty(-1)^n\frac{H_{n-1}}{n^x}\etiqueta{6} $$