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Table 3:

Spectral information from X-ray observations of H 2356-309.

Instrument
MJD Model $\Gamma_1$ $E_{\rm break}$ $
\Gamma_2$ $F_{0.1-2.0~\rm keV}$ $F_{2-10~\rm keV}$ $\chi^2_{\rm r}$, NDFa
        [keV]   [10-12 erg cm-2 s-1]b  

BeppoSAX
51 350-51 BPL $\rm0.78^{+0.06}_{-0.07}$ $1.8 \pm 0.4$ $1.10 \pm 0.04$ - 25 -
RXTE 53 320 PL $2.43 \pm 0.25$ - - - $\rm 9.70^{+0.3}_
{-1.3}$ -

XMM-Newtonc
53 534 PL $2.23 \pm 0.01$ - - 25.9 8.05 1.41, 541
    BPL $2.08 \pm 0.03$ $1.00 \pm 0.08$ $2.32 \pm 0.02$ 23.2 7.46 0.95, 539

XMM-Newtonc
53 536 PL $2.16 \pm 0.01$ - - 25.9 9.54 1.52, 541
    BPL $1.89 \pm 0.10$ $0.66 \pm 0.14$ $2.20 \pm 0.02$ 22.3 9.15 1.21, 539

Notes. aThe reduced $\chi^2_{\rm r}$ and degrees of freedom (NDF) correspond to fits of either a power-law (PL) function or broken power-law (BPL) function to the XMM-Newton X-ray data. bThe integrated fluxes have the effects of Galactic absorption removed. cAll errors from the XMM-Newton fits are quoted at the 90% confidence level.


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