Table 2: Best fit model parameters and inferred physical system parameters. Here CF is the partial covering coefficient, F3-100 the observed X-ray flux in the 3-100 keV band, F0.1-100 the unabsorbed X-ray flux in the 0.1-100 keV band, both in 10-11 erg cm-2 s-1 units. The distances for V405 Aur, V709 Cas, PQ Gem and V2400 Oph are assumed.
Name $M_{\rm wd}$, CF $N_{\rm H}$, F3-100 F0.1- 100 $\dot M$ $L_{\rm x}$, 1033 d $\chi^2$ (d.o.f.)
  $M_{\odot}$   1022 cm-2     1016 g s-1 erg s-1 pc  
V1223 Sgr $0.95\pm0.05$ 1.0a $3.7\pm1$ 4.2 7.3 12.6 24.3 5271 105.4(63)
    $0.57\pm0.05$ $28\pm3$            
FO Aqr $0.60\pm 0.05$ $0.9\pm0.1$ $36\pm4$ 1.5 4.9 10.2 9.4 4002 62.1(65)
EX Hya $0.50 \pm 0.05$ 1.0 $0.6\pm1.0$ 1.5 3.4 0.25 0.17 64.53 85.3(65)
AO Psc $0.65\pm0.05$ $0.95\pm0.1$ $10\pm5$ 1.3 2.5 4.7 4.9 4204 55.8(65)
TVCol $0.84\pm0.06$ $0.81\pm0.3$ $21\pm5$ 1.7 3.5 3.4 5.7 3685 63.4(65)
GK Per $0.59\pm0.05$ 1.0a $20\pm2$ 12.5 88.6 81.5 156 3406 110.5(63)
    $0.75\pm0.05$ $125\pm10$            
V709 Cas $0.90\pm0.10$ $0.5\pm 0.1$ $29\pm5$ 2.3 3.7 5.76 11.1 (500) 56.3(65)
PQ Gem $0.65\pm 0.2$ 1.0 $5\pm1$ 0.80 1.3 3.7 3.9 (500) 38.7(65)
V2400 Oph $0.59\pm0.05$ $0.4\pm0.1$ $29\pm10$ 2.43 5.6 18.7 16.75 (500) 78.5(65)
BG CMi $0.85\pm0.12$ $0.70\pm0.05$ $25\pm6$ 0.77 1.54 5.3 9.0 7007 57.4(65)
V405 Aur $0.90\pm0.10$ $0.6\pm0.1$ $39\pm3$ 0.9 1.7 2.65 5.09 (500) 51.6(65)
V1062 Tau $1.00\pm0.20$ $0.6\pm0.1$ $21\pm7$ 1.1 1.8 2.2 5.4 5008 45.6(65)
DO Dra $0.75\pm0.05$ $0.4\pm0.1$ $20\pm5$ 7.8 14.4 3.1 4.1 1559 69.7(65)
TX Col $0.70\pm0.30$ <0.4 <60 0.32 0.58 1.8 2.1 55010 52.6(65)
a - For the systems V1223 Sgr and GK Per which have very high mass accretion rates we used two absorbers.

References to distance estimates: 1. Beuermann et al. (2004); 2. McHardy et al. (1987); 3. Beuermann et al. (2003); 4. Hellier et al. (1991); 5. McArthur et al. (2001); 6. Warner (1987); 7. Berriman (1987); 8. Szkody & Silber (1996); 9. Mateo et al. (1991); 10. Buckley & Tuohy (1989).


Source LaTeX | All tables | In the text