$\newcommand{\braces}[1]{\left\lbrace\,{#1}\,\right\rbrace}
\newcommand{\bracks}[1]{\left\lbrack\,{#1}\,\right\rbrack}
\newcommand{\dd}{\mathrm{d}}
\newcommand{\ds}[1]{\displaystyle{#1}}
\newcommand{\expo}[1]{\,\mathrm{e}^{#1}\,}
\newcommand{\ic}{\mathrm{i}}
\newcommand{\mc}[1]{\mathcal{#1}}
\newcommand{\mrm}[1]{\mathrm{#1}}
\newcommand{\pars}[1]{\left(\,{#1}\,\right)}
\newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}}
\newcommand{\root}[2][]{\,\sqrt[#1]{\,{#2}\,}\,}
\newcommand{\totald}[3][]{\frac{\mathrm{d}^{#1} #2}{\mathrm{d} #3^{#1}}}
\newcommand{\verts}[1]{\left\vert\,{#1}\,\right\vert}$
We can easily see that
$$
\bbox[0.5em,#efe,border:0.1em groove navy]{\
r_{1} \equiv -0.78891677373356634396694435041559932834090342558\
}
$$
is a 'good approximation' to the real root of
$\ds{z^{5} + \root{2}z^{3} + 1 = 0}$.
Then, a 'fine approximation' is given by:
\begin{align}
z^{5} + \root{2}z^{3} + 1 & =
\pars{z - r_{1}}\pars{z^{4} + bz^{3} + cz^{2} + dz - {1 \over r_{1}}}
\\[5mm] & =
z^{5} + \pars{b - r_{1}}z^{4}+ \pars{c - br_{1}}z^{3}+ \pars{d - cr_{1}}z^{2}+ \pars{dr_{1} - {1 \over r_{1}}}z + 1
\end{align}
Now, we have an equation which can be solved analytically. Namely,
$$
z^{4} + r_{1}z^{3} + \pars{r_{1}^{2} + \root{2}}z^{2} + r_{1}\pars{r_{1}^{2} + \root{2}}z - {1 \over r_{1}} = 0
$$