Converting missed `Zeros` to `Residues`
"\\end{equation}\n",
"This admittance matches the target response if $R = \\frac{1}{d_i}$ and $C = e_i$.\n",
"\n",
- "### Real Poles and Zeros\n",
+ "### Real Poles and Residues\n",
"The individual terms $\\frac{c_{k,i}}{\\mathrm{\\underline{s}} - p_{k,i}}$ of the fit with a real pole $p_{k,i}$ and a real residue $c_{k,i}$ can be represented in an electrical circuit by equivalent impedances $\\underline{Z}_\\mathrm{RC}(\\mathrm{\\underline{s}})$ or equivalent admittances $\\underline{Y}_\\mathrm{RL}(\\mathrm{\\underline{s}})$ build out of a parallel RC or series RL circuits.\n",
"\n",
"Target response of the real pole-residue term:\n",
"\\end{equation}\n",
"This admittance matches the target response if $L = \\frac{1}{c_{k,i}}$ and $R = \\frac{-p_{k,i}}{c_{k,i}}$.\n",
"\n",
- "### Complex Conjugate Poles and Zeros\n",
+ "### Complex Conjugate Poles and Residues\n",
"In Vector Fitting, complex poles $\\underline{p}_k = p'_k + \\mathrm{j} p''_k$ and residues $\\underline{c}_k = c'_k + \\mathrm{j} c''_k$ always come in complex conjugate pairs $(\\underline{p}_k, \\underline{p}_k^*)$ and $(\\underline{c}_k, \\underline{c}_k^*)$. The target response for an equivalent electrical circuit of such a complex conjugate pair is therefore:\n",
"\n",
"\\begin{equation}\n",
