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Home All issues Volume 520 (September-October 2010) A&A, 520 (2010) A74 Full HTML
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This article has an erratum: [https://doi.org/10.1051/0004-6361/200810284e]

 

 

Table 12:

Wilson-Devinney analysis, as obtained on the basis of both photometry and spectroscopy.

Object 		Model $T_{{\rm eff}}^{{\rm S}} / T_{{\rm eff}}^{{\rm P}}$ $\Omega_{\rm P}$ $\Omega_{\rm S}$ $(L_{\rm S}/L_{\rm P})_{B}$ $(L_{\rm S}/L_{\rm P})_{V}$ $(L_{\rm S}/L_{\rm P})_{I}$ $(L_{\rm S}/L_{\rm P})_B^{{\rm sp}}$
          $\ell_{3,B}$ $\ell_{3,V}$ $\ell_{3,I}$  
4 110409 sd $0.654 \pm0.007$ $5.732\pm0.092$ 2.922 (fixed) $1.292\pm0.023$ $1.353\pm0.024$ $1.367\pm0.024$ $1.392\pm0.036$
4 113853 sd $0.737 \pm0.015$ $3.868\pm0.090$ 3.209 (fixed) $0.680\pm0.010$ $0.713\pm0.009$ $0.753\pm0.009$ $0.681\pm0.058$
4 117831 d $0.981 \pm0.023$ 4.855 (fixed) $4.479\pm0.108$ $1.175\pm0.052$ $1.177\pm0.050$ $1.180\pm0.049$ $1.009\pm0.103$
4 121084 d $0.940 \pm0.007$ 3.770 (fixed) $3.817\pm0.043$ $0.707\pm0.061$ $0.713\pm0.010$ $0.720\pm0.010$ $0.704\pm0.061$
4 121110 d $0.894 \pm0.007$ $3.820\pm0.035$ $4.184\pm0.059$ $0.424\pm0.005$ $0.433\pm0.005$ $0.442\pm0.005$ $0.415\pm0.047$
4 121461 d $0.949 \pm0.023$ $6.980\pm0.133$ $6.822\pm0.099$ $0.907\pm0.030$ $0.914\pm0.029$ $0.923\pm0.029$ $0.954\pm0.063$
4 159928 sd $0.723 \pm0.010$ $3.138\pm0.024$ 2.983 (fixed) $0.357\pm0.003$ $0.376\pm0.003$ $0.397\pm0.004$ $0.453\pm0.029$
4 160094 d $0.854 \pm0.018$ 5.517 (fixed) $5.545\pm0.100$ $0.476\pm0.050$ $0.489\pm0.007$ $0.502\pm0.007$ $0.428\pm0.101$
4 163552 d $0.997 \pm0.004$ $3.983\pm0.026$ $4.214\pm0.044$ $0.798\pm0.024$ $0.799\pm0.016$ $0.800\pm0.014$ $0.926\pm0.171$
          $0.142\pm0.014$ $0.112\pm0.012$ $0.119\pm0.006$  
4 175149 sd $0.849 \pm0.006$ $4.411\pm0.056$ 3.171 (fixed) $1.176\pm0.025$ $1.200\pm0.023$ $1.229\pm0.023$ $1.415\pm0.132$
4 175333 d $0.879 \pm0.022$ $5.054\pm0.151$ $5.010\pm0.196$ $0.582\pm0.034$ $0.595\pm0.035$ $0.609\pm0.036$ $0.562\pm0.103$
5 016658 d $1.007 \pm0.009$ 4.086 (fixed) $4.590\pm0.068$ $0.609\pm0.074$ $0.612\pm0.008$ $0.614\pm0.008$ $0.604\pm0.074$
5 026631 sd $0.734 \pm0.007$ $3.507\pm0.030$ 3.226 (fixed) $0.495\pm0.003$ $0.519\pm0.003$ $0.547\pm0.003$ $0.736\pm0.049$
5 032412 d $0.880 \pm0.008$ 7.284 (fixed) $6.949\pm0.073$ $0.578\pm0.050$ $0.584\pm0.007$ $0.583\pm0.007$ $0.546\pm0.005$
5 038089 d $1.012 \pm0.009$ $4.606\pm0.047$ $5.065\pm0.067$ $0.693\pm0.019$ $0.692\pm0.018$ $0.691\pm0.018$ $0.678\pm0.032$
5 095337 d $0.936 \pm0.007$ $3.685\pm0.022$ $3.835\pm0.040$ $0.676\pm0.008$ $0.684\pm0.008$ $0.691\pm0.008$ $0.659\pm0.085$
5 095557 d $0.908 \pm0.013$ $5.991\pm0.107$ $6.602\pm0.165$ $0.523\pm0.015$ $0.532\pm0.015$ $0.541\pm0.015$ $0.625\pm0.190$
5 100485 d $1.008 \pm0.007$ $5.193\pm0.076$ $5.216\pm0.080$ $0.966\pm0.034$ $0.965\pm0.034$ $0.963\pm0.034$ $0.930\pm0.052$
5 100731 c $0.828 \pm0.035$ $3.851\pm0.058$ 3.351 (fixed) $0.517\pm0.014$ $0.533\pm0.013$ $0.552\pm0.012$ $0.438\pm0.041$
5 106039 sd $0.638 \pm0.006$ $5.178\pm0.057$ 2.928 (fixed) $1.007 \pm0.009$ $1.076\pm0.009$ $1.168\pm0.009$ $1.062\pm0.063$
5 111649 d $1.025 \pm0.011$ 4.600 (fixed) $4.736\pm0.067$ $0.889\pm0.056$ $0.886\pm0.015$ $0.882\pm0.014$ $0.880\pm0.052$
5 123390 d $1.017 \pm0.020$ 5.077 (fixed) $5.631\pm0.106$ $0.587\pm0.060$ $0.587\pm0.011$ $0.585\pm0.010$ $0.584\pm0.061$
5 180185 d $1.036 \pm0.029$ $7.724\pm0.169$ $8.571\pm0.249$ $0.707\pm0.042$ $0.705\pm0.025$ $0.700\pm0.024$ $0.611\pm0.042$
5 180576 d $0.813 \pm0.027$ $4.918\pm0.170$ $5.071\pm0.207$ $0.450\pm0.027$ $0.465\pm0.028$ $0.483\pm0.029$ $0.45 \pm0.07 $
5 185408 d $0.944 \pm0.018$ 5.052 (fixed) $4.957\pm0.094$ $0.757\pm0.047$ $0.764\pm0.017$ $0.772\pm0.016$ $0.619\pm0.045$
5 196565 d $0.867 \pm0.016$ 5.956 (fixed) $6.639\pm0.120$ $0.43 \pm0.04$a b $0.453\pm0.009$ $0.413\pm0.040$
5 261267 sd $0.728 \pm0.004$ $3.353\pm0.013$ 2.923 (fixed) $0.439\pm0.002$ $0.461\pm0.003$ $0.487\pm0.001$ $0.451\pm0.039$
5 265970 d $0.901 \pm0.012$ 4.157 (fixed) $5.370\pm0.056$ $0.219\pm0.024$ $0.264\pm0.001$ $0.227\pm0.001$ $0.233\pm0.024$
5 266015 sd $0.757 \pm0.005$ $3.512\pm0.026$ 2.759 (fixed) $0.494\pm0.002$ $0.515\pm0.002$ $0.539\pm0.002$ $0.617\pm0.045$
5 266131 d $0.936 \pm0.007$ 4.510 (fixed) $4.727\pm0.065$ $0.647\pm0.060$ $0.655\pm0.008$ $0.661\pm0.007$ $0.644\pm0.060$
5 266513 d $0.959 \pm0.018$ 4.390 (fixed) $4.530\pm0.084$ $0.692\pm0.070$ $0.697\pm0.016$ $0.703\pm0.015$ $0.733\pm0.076$
5 277080 sd $0.685 \pm0.004$ $3.932\pm0.047$ 2.884 (fixed) $0.567\pm0.015$ $0.600\pm0.008$ $0.641\pm0.008$ $0.690\pm0.022$
5 283079 d $0.997 \pm0.010$ 5.162 (fixed) $5.184\pm0.074$ $0.987\pm0.086$ $0.987\pm0.015$ $0.988\pm0.015$ $0.936\pm0.088$

Notes. Listed parameters: system type (detached, semi-detached or contact), temperature ratio, normalized surface potentials and passband luminosity ratios. Third light contribution is given for the system 4 163552 (normalized to total flux at phase 0.25). The given potentials and the luminosity ratios are those obtained including the spectroscopic constraints (final WD/PHOEBE analysis).
(a) B data missing, ratio given by the WD code on the basis of the I data, via the atmosphere models; (b) V data missing.


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