\begin{table}%T7
\caption{Spectral-fit parameters for Ph~III \igr, \xmm, \pca\ and
  RXTE-HEXTE fits (see Sect.~\ref{sec:rxsphaseres}).  
%exact used N_H is 1.4675 \times 10^22
}
\small%\centerline
{
\begin{tabular}{lc}
\hline
\hline
\multicolumn{2}{c}{{\xmm+\pca+HEXTE+}}\\
\multicolumn{2}{c}{{\igr\ 0.5--270~keV}}\\
$kT$                   & $0.23 \pm 0.02$\\
$F_{0~kT}$             & $(2.82 \pm 0.64) \times  10^{-5}$\\
$\Gamma_{\rm{I}}\ (0.5 {\rm~keV} - E_{\rm{break}}) $&${\bf -}0.55 \pm 0.14$\\
$E_{\rm{break}}$        &  $4.92 \pm 0.11$\\
$\Gamma_{\rm{II}}\ (E_{\rm{break}} - 270 {\rm~keV}) $  & $1.77 \pm 0.09$\\
$F_{0~}$               & $(2.05 \pm 0.52) \times  10^{-5}$\\
$\Gamma_{\rm{III}}\ (0.5 - 270 {\rm~keV}) $     & $0.02 \pm 0.50$\\
$F_{20-150~\rm{keV}}$   &$(0.86 \pm 0.22) \times 10^{-11}$ \\
\chir~ (d.o.f.)          & 0.90 (29)\\
$F_{0.5-2~\rm{keV}}$ (\ecs) & $(0.19 \pm 0.07) \times  10^{-11}$\\
$F_{2-10~\rm{keV}}$ (\ecs)  & $(0.23 \pm 0.07) \times  10^{-11}$\\
$F_{20-150~\rm{keV}}$ (\ecs) &$(1.54 \pm 0.18) \times 10^{-11}$ \\
$F_{20-270~\rm{keV}}$ (\ecs) &$(3.74 \pm 0.65) \times  10^{-11}$ \\
\multicolumn{2}{c}{{\igr\ 20$-$270~keV}}\\
$\Gamma_{\rm{\igr}}$ & $1.09 \pm 0.16$\\
$F_{20-150~\rm{keV}}$ (\ecs) &$(1.53 \pm 0.12) \times 10^{-11}$ \\ 
\chir~ (d.o.f.)       &  1.15 (5)\\
$F_{20-270~\rm{keV}}$ (\ecs) &$(2.81 \pm 0.42) \times  10^{-11}$ \\
\hline
\end{tabular}}
\smallskip
 The $N_{\rm H}$ is fixed to $1.47 \times 10^{22}$~cm$^{-2}$. $kT$ and $E_{{\rm break}}$ are in units~keV. $F_{0}$~is the
normalization at 1~keV in units \pcsk. The integrated fluxed are in
units~\ecs.
\label{tab:rxsph3}
\end{table}