$\newcommand{\+}{^{\dagger}}
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\newcommand{\braces}[1]{\left\lbrace\, #1 \,\right\rbrace}
\newcommand{\bracks}[1]{\left\lbrack\, #1 \,\right\rbrack}
\newcommand{\ceil}[1]{\,\left\lceil\, #1 \,\right\rceil\,}
\newcommand{\dd}{{\rm d}}
\newcommand{\down}{\downarrow}
\newcommand{\ds}[1]{\displaystyle{#1}}
\newcommand{\expo}[1]{\,{\rm e}^{#1}\,}
\newcommand{\fermi}{\,{\rm f}}
\newcommand{\floor}[1]{\,\left\lfloor #1 \right\rfloor\,}
\newcommand{\half}{{1 \over 2}}
\newcommand{\ic}{{\rm i}}
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\newcommand{\imp}{\Longrightarrow}
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\newcommand{\ol}[1]{\overline{#1}}
\newcommand{\pars}[1]{\left(\, #1 \,\right)}
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\newcommand{\root}[2][]{\,\sqrt[#1]{\vphantom{\large A}\,#2\,}\,}
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\newcommand{\wt}[1]{\widetilde{#1}}$
Lets $\ds{\fermi\pars{x}\equiv
\left\{\begin{array}{lcrcl}
{\sin\pars{2x} \over x} & \mbox{if} & x & \not= & 0
\\[1mm]
2 & \mbox{if} & x & = & 0
\end{array}\right.}$
Note that $\ds{\fermi}$ is an even function of $\ds{x}$:
$\ds{\fermi\pars{-x}=\fermi\pars{x}\,,\ \forall\ x\in{\mathbb R}}$.
We'll use the
$\large\mbox{Abel-Plana Formula}$:
\begin{align}
&\color{#66f}{\large\sum_{n = 1}^{\infty}\pars{-1}^{n}\,{\sin\pars{2n} \over n}}
=-2 + \sum_{n = 0}^{\infty}\pars{-1}^{n}\fermi\pars{n}
\\[5mm]&=-2 + \bracks{\half\,\fermi\pars{0} + \ic\
\underbrace{\int_{0}^{\infty}%
{\fermi\pars{\ic t} - \fermi\pars{-\ic t} \over 2\sinh\pars{\pi t}}\,\dd t}
_{\ds{=\ \color{#c00000}{\large 0}}}}
\\[5mm]&=-2 + \bracks{\half\times 2 + \ic\times 0} = \color{#66f}{\Large -1}
\end{align}