Table 1: Best-fit parameters for the absorbed power-law model of the HETGS spectra of IGR J00291+5934 and for the absorbed power-law plus thermal component of the HETGS, PCA, and Chandra zeroth-order spectra. $N_{{\rm H}}$ is the column density in units of 1021 cm$^{\rm -2}$; $kT_{\rm in}$ is the inner temperature of the thermal (DISKBB) component; d.o.f. = degrees of freedom (the decrease in d.o.f. in the combined HEG/MEG and PCA spectrum is due to the heavy rebinning we performed in the HETGS data, see text); in all the fits we fixed HEG, MEG and zeroth-order normalisation factors to 1. The indicated errors are at 1$\sigma $.
  HEG / MEG HEG / MEG / PCA
$N_{{\rm H}}$ 4.3 $\pm$ 0.4 $4.3 {+0.7 \atop -0.5}$
$\Gamma$ 2.06 $\pm$ 0.07 $1.7\pm0.08$
$kT_{\rm in}$   $0.42 {+0.07 \atop -0.06}$ keV
PCA norm   1.13
reduced $\chi^2_{\nu}$ 0.79 (431 d.o.f.) 0.9 (161 d.o.f.)
  HEG / MEG  
  PCA / 0th order  
$N_{{\rm H}}$ $3.9{+0.5 \atop -0.4}$  
$\Gamma$ 1.7 $\pm$ 0.04  
$kT_{\rm in}$ 0.40 $\pm$ 0.06 keV  
PCA norm 1.13  
reduced $\chi^2_{\nu}$ 1.15 (293 d.o.f.)  


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