A system of two spin- \( 1 / 2 \mathrm{~s} A \) and \( B \) is in the state
\[
\left|\psi_{A+B}\right\rangle=\alpha_{++}|++\rangle+\alpha_{+-}|+-\rangle+\alpha_{-+}|-+\rangle+\alpha_{--}|--\rangle .
\]
Show that
\[
\begin{aligned}
\hat{\rho}^{(\mathrm{A})}= & \left(\left|\alpha_{++}\right|^{2}+\left|\alpha_{+-}\right|^{2}\right)|+\rangle\langle+|+\left(\left|\alpha_{--}\right|^{2}+\left|\alpha_{-+}\right|^{2}\right)|-\rangle\langle-| \\
& +\left(\alpha_{++} \alpha_{-+}^{*}+\alpha_{+-} \alpha_{--}^{*}\right)|+\rangle\langle-|+\left(\alpha_{--} \alpha_{+-}^{*}+\alpha_{-+} \alpha_{++}^{*}\right)|-\rangle\langle+| .
\end{aligned}
\]
and
\[
\begin{aligned}
\hat{\rho}^{(\mathrm{B})}= & \left(\left|\alpha_{++}\right|^{2}+\left|\alpha_{-+}\right|^{2}\right)|+\rangle\langle+|+\left(\left|\alpha_{--}\right|^{2}+\left|\alpha_{+-}\right|^{2}\right)|-\rangle\langle-| \\
& +\left(\alpha_{++} \alpha_{+-}^{*}+\alpha_{-+} \alpha_{--}^{*}\right)|+\rangle\langle-|+\left(\alpha_{--} \alpha_{-+}^{*}+\alpha_{+-} \alpha_{++}^{*}\right)|-\rangle\langle+| .
\end{aligned}
\]