$\newcommand{\angles}[1]{\left\langle\, #1 \,\right\rangle}
\newcommand{\braces}[1]{\left\lbrace\, #1 \,\right\rbrace}
\newcommand{\bracks}[1]{\left\lbrack\, #1 \,\right\rbrack}
\newcommand{\dd}{{\rm d}}
\newcommand{\ds}[1]{\displaystyle{#1}}
\newcommand{\dsc}[1]{\displaystyle{\color{red}{#1}}}
\newcommand{\expo}[1]{\,{\rm e}^{#1}\,}
\newcommand{\half}{{1 \over 2}}
\newcommand{\ic}{{\rm i}}
\newcommand{\imp}{\Longrightarrow}
\newcommand{\Li}[1]{\,{\rm Li}_{#1}}
\newcommand{\pars}[1]{\left(\, #1 \,\right)}
\newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}}
\newcommand{\root}[2][]{\,\sqrt[#1]{\vphantom{\large A}\,#2\,}\,}
\newcommand{\totald}[3][]{\frac{{\rm d}^{#1} #2}{{\rm d} #3^{#1}}}
\newcommand{\verts}[1]{\left\vert\, #1 \,\right\vert}$
$\ds{}$
\begin{align}&\overbrace{\color{#66f}{\int_{0}^{\pi/2}\expo{-\sin\pars{x}}\,\dd x}}
^{\ds{\dsc{\sin\pars{x}}=\dsc{t}\ \imp\ \dsc{x}=\dsc{\arcsin\pars{t}}}}\ =\
\int_{0}^{1}\frac{\expo{-t}}{\root{1 - t^{2}}}\,\dd t
=\color{#66f}{\large -\,\frac{\pi}{2}\,{\rm M}_{0}\pars{1}}
\approx{\tt 0.8731}\tag{1}
\end{align}
$\ds{\,{\rm M}_{\nu}\pars{z}}$ is a
Modified Struve Function.
The result
$\ds{\pars{~\mbox{given in expression}\ \pars{1}~}}$ corresponds to $11.5.4$ in
this link.