\begin{table}%t2 \caption{\label{tab:fitparam}Best fit parameters.} \small%\centerline { \begin{tabular}{lccc} \hline \hline Parameter$^a$ & Model A & Model B & Model C \\ & pure gas & gas \& dust & pure gas \\ & curv. corr. & curv. corr & no curv. corr \\ \hline %&&& \\[-8pt] $\chi^2$ & 2341 & 2327 & 2366 \\ d.o.f. & 1316 & 1315 & 1316 \\ $f(5)^{b}$ & $1.056\pm 0.009$ & $1.055\pm 0.009$ & $1.035\pm 0.009$ \\ $f(40)^{b}$ & $0.746\pm 0.016$ & $0.762\pm 0.016$ & $0.854\pm 0.019$ \\ \hline \multicolumn{4}{l}{column densities$^{c}$:}\\ \hline %&&& \\[-8pt] \ion{H}{i}$^{d,e}$ & $31~750\pm 220$ & $ 9700 \pm 1700 $ & $31~280\pm 220$ \\ \ion{H}{i}$^{d,f}$ & $-$ & $22~300 \pm 1800 $ & $-$ \\ \ion{H}{i}$^{d,g}$ & $31~750\pm 220$ & $32~060\pm 220 $ & $31~280\pm 220$ \\ \ion{H}{ii}$^h$ &$1752\pm 4$& $1752\pm 4$ & $1752\pm 4$\\ \ion{N}{i} & $ 2.67\pm 0.24$ & $ 2.72\pm 0.24$ & $ 2.48\pm 0.25$ \\ \ion{O}{i} & $19.28\pm 0.18$ & $19.83\pm 0.22$ & $19.23\pm 0.18$ \\ \ion{O}{ii} & $ 0.23\pm 0.14$ & $ 0.25\pm 0.15$ & $ 0.20\pm 0.14$ \\ \ion{Ne}{i} & $ 4.69\pm 0.21$ & $ 4.66\pm 0.21$ & $ 4.74\pm 0.21$ \\ \ion{Ne}{ii} & $ 0.46\pm 0.25$ & $ 0.52\pm 0.24$ & $ 0.64\pm 0.25$ \\ \ion{Mg}{i} & $ 1.14\pm 0.28$ & $ 1.20\pm 0.28$ & $ 1.13\pm 0.28$ \\ \ion{Mg}{ii} & $ 0.00\pm 0.09$ & $ 0.00\pm 0.10$ & $ 0.00\pm 0.09$ \\ \ion{Fe}{i} & $ 0.65\pm 0.05$ & $ 0.77\pm 0.04$ & $ 0.65\pm 0.05$ \\ \ion{Fe}{ii} & $ 0.23\pm 0.06$ & $ 0.14\pm 0.04$ & $ 0.26\pm 0.07$ \\ \hline \end{tabular}} \medskip $^a$ Error bars are all $1\sigma$ for one interesting parameter.\\ $^b$ $f(5)$ and $f(40)$ are the values of the effective area scale factor $f(\lambda)$, Eq.~(\ref{eqn:aeff_cor}), at~5 and 40~\AA.\\ $^c$ Ionic column densities are given in units of $10^{21}$~m$^{-2}$. The column densities of all metals include all phases (dust and gas).\\ $^d$ \ion{H}{i} includes in the cross section contributions from neutral~He, C, Si, S, Ar, Ca and Ni assuming proto-solar abundances for these elements.\\ $^e$ For the pure gaseous phase only.\\ $^f$ For the gas \& dust mixture with proto-solar abundances added to the pure gaseous phase above.\\ $^g$ Total column: sum of contributions listed as $b$ and $c$.\\ $^h$ For \ion{H}{ii} the column is derived from the pulsar dispersion measure assuming that all free electrons originate from hydrogen (see text). \end{table}