$\newcommand{\bbx}[1]{\,\bbox[8px,border:1px groove navy]{\displaystyle{#1}}\,}
\newcommand{\braces}[1]{\left\lbrace\,{#1}\,\right\rbrace}
\newcommand{\bracks}[1]{\left\lbrack\,{#1}\,\right\rbrack}
\newcommand{\dd}{\mathrm{d}}
\newcommand{\ds}[1]{\displaystyle{#1}}
\newcommand{\expo}[1]{\,\mathrm{e}^{#1}\,}
\newcommand{\ic}{\mathrm{i}}
\newcommand{\mc}[1]{\mathcal{#1}}
\newcommand{\mrm}[1]{\mathrm{#1}}
\newcommand{\pars}[1]{\left(\,{#1}\,\right)}
\newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}}
\newcommand{\root}[2][]{\,\sqrt[#1]{\,{#2}\,}\,}
\newcommand{\totald}[3][]{\frac{\mathrm{d}^{#1} #2}{\mathrm{d} #3^{#1}}}
\newcommand{\verts}[1]{\left\vert\,{#1}\,\right\vert}$
Note that
$\ds{\int_{b}^{c}\delta\pars{x - a}\dd x} =
\ds{\bracks{b < a < c} - \bracks{c < a < b}}$ where $\ds{\bracks{\cdots}}$ is an Iverson Bracket.
\begin{align}
&\int_{0}^{t}\dd s\int_{0}^{t'}\dd s'\,\delta\pars{s - s'} =
\int_{0}^{t}\int_{0}^{t'}\delta\pars{s' - s}\dd s'\,\dd s
\\[5mm] = &\
\int_{0}^{t}\bracks{0 < s < t'}\dd s - \int_{0}^{t}\bracks{t' < s < 0}\dd s =
\int_{0}^{t}\bracks{0 < s < t'}\dd s + \int_{t}^{0}\bracks{t' < s < 0}\dd s
\\[1cm] = &\
\bracks{t > 0}\bracks{t' > 0}\braces{\vphantom{\Large A}%
\bracks{t' < t}t' + \bracks{t' > t}t}
\\[5mm] + &\
\bracks{t < 0}\bracks{t' < 0}\braces{\vphantom{\Large A}%
\bracks{t' < t}\pars{-t} + \bracks{t' > t}\pars{-t'}}
\\[1cm] = &\
\bracks{t > 0}\bracks{t' > 0}\min\braces{t,t'} -
\bracks{t < 0}\bracks{t' < 0}\max\braces{t,t'}
\\[5mm] = &\
\bracks{t > 0}\bracks{t' > 0}\min\braces{t,t'} +
\bracks{t < 0}\bracks{t' < 0}\min\braces{-t,-t'}
\\[5mm] = &\
\braces{\vphantom{\Large A}%
\bracks{t > 0}\bracks{t' > 0} + \bracks{t < 0}\bracks{t' < 0}}
\min\braces{\verts{t},\verts{t'}}
\\[5mm] = &\
\bbox[#ffe,20px,border:2px dotted navy]{%
\ds{\bracks{tt' > 0}\min\braces{\verts{t},\verts{t'}}}}
\end{align}