Free Access
 

 

Table 3:

X-ray spectral properties of the 23 sources showing a detection in at least one of the two energy bands, S and H.
ID CR0.5-2 CR2-10 HR Flux2-10 $N_{\rm H}$ log( $L_{\rm X,obs}$) log($L_{\rm X}$) log( $\lambda L_{5.8}$/L2-10) Analysis
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10)
1 $19.4 \pm3.4$ $6.1 \pm2.5$ - $0.52\pm0.19$ $\rm 10.2_{-4.0}^{+3.8}$ $\rm 1.1_{-0.7}^{+1.4}$ 43.68 43.72 1.4 1 SP
4 $1.7 \pm0.8$ $2.2 \pm0.9$ $0.13\pm0.31$ $\rm 8.5_{-4.2}^{+5.9}$ $\rm 19.9_{-14.4}^{+37.8}$ 43.90 44.31 1.31 SP
5 $2.7 \pm1.3$ $1.8 \pm1.2$ - $0.25\pm0.53$ $\rm 2.2_{-0.6}^{+2.8}$ <14.3 42.93 43.03 2.1 SP
6 $21.1 \pm2.5$ $63.7\pm4.3$ $0.49\pm0.07$ $\rm 113.1_{-30.0}^{+17.0}$ $\rm 10.8_{-3.8}^{+3.6}$ 44.49 44.71 0.95 SP
7 $4.0 \pm2.8$ $7.4 \pm3.9$ $0.30\pm0.44$ $\rm 14.2_{-3.0}^{+3.0}$ $\rm 25.0_{-23.0}^{+35.0}$ 44.40 44.48 1.43 HR
8 <6.9 $4.8 \pm4.1$ >-0.53 $\rm 3.4_{-1.6}^{+1.6}$ >0.1 43.13 >43.13a 1.29 HR
9 $1.8 \pm1.6$ $2.8 \pm1.9$ $0.21\pm0.54$ $\rm 5.3_{-1.9}^{+1.9}$ $\rm 25.0_{-24.0}^{+60.0}$ 44.08 44.15 1.47 HR
10 $1.0 \pm0.9$ <1.5 <0.25 < $\rm 2.3_{-1.4}^{+1.4}$ <6.0 42.82 42.87 1.76 HR
11 $5.0 \pm2.3$ $3.5 \pm2.4$ - $0.18\pm0.39$ $\rm 5.8_{-2.7}^{+2.6}$ $\rm 4.9_{-4.0}^{+9.9}$ 43.40 43.57 1.73 SP
12 $1.9 \pm1.6$ $5.7 \pm2.5$ $0.50\pm0.44$ $\rm 27.1_{-3.9}^{+4.8}$ $\rm 267.9_{-144.8}^{+274.7}$ 43.40 45.16 0.34 SP
19 $2.2 \pm1.3$ $8.6 \pm4.4$ $0.60\pm0.62$ $\rm 12.6_{-7.9}^{+7.9}$ $\rm 25.0_{-17.0}^{+75.0}$ 44.10 44.92 1.76 HR
21 $13.0 \pm5.3$ $10.6 \pm4.9$ - $0.10\pm0.31$ $\rm 24.8_{-6.4}^{+6.4}$ $\rm 4.0_{-3.5}^{+8.0}$ 44.19 44.21 1.05 HR
22 $5.9 \pm3.0$ $6.7 \pm3.7$ $0.06\pm0.37$ $\rm 11.3_{-4.2}^{+4.2}$ $\rm 13.0_{-11.0}^{+35.0}$ 44.35 44.39 1.56 HR
25 $10.9 \pm3.7$ $4.5 \pm5.0$ - $0.42\pm0.43$ $\rm 18.6_{-3.8}^{+3.8}$ <45.0 45.26 45.30 1.33 HR
31 <2.2 $0.9 \pm0.4$ >-0.15 $\rm 1.7_{-0.7}^{+0.7}$ >0.1 43.24 >43.24a 1.70 HR
32 $0.7 \pm0.3$ $1.8 \pm0.5$ $0.49\pm0.31$ $\rm 3.1_{-0.5}^{+0.5}$ $\rm 75.0_{-40.0}^{+75.0}$ 44.10 44.53 2.23 HR
33 $0.7 \pm0.3$ $1.9 \pm0.6$ $0.48\pm0.28$ $\rm 3.8_{-0.6}^{+0.6}$ $\rm 60.0_{-30.0}^{+45.0}$ 44.10 44.59 1.82 HR
36 $3.7 \pm2.5$ $9.4 \pm3.8$ $0.43\pm0.40$ $\rm 4.3_{-1.2}^{+6.6}$ <28.0 43.01 43.06 1.21 SP
39 $11.2 \pm2.8$ $25.9 \pm3.9$ $0.40\pm0.14$ $\rm 29.9_{-13.4}^{+7.4}$ $\rm 6.7_{-2.4}^{+3.5}$ 43.65 43.85 1.03 SP
40 $23.2 \pm3.5$ $6.9 \pm2.3$ - $0.53\pm0.16$ $\rm 9.3_{-1.3}^{+2.1}$ <1.5 43.88 43.90 1.34 SP
41 $4.6 \pm1.9$ $17.5\pm2.8$ $0.58\pm0.18$ $\rm 23.7_{-8.1}^{+6.9}$ $\rm 11.9_{-5.0}^{+8.7}$ 43.88 44.05 0.46 SP
43 $40.7 \pm5.8$ $3.3 \pm3.0$ - $0.81\pm0.18$ $\rm 12.0_{-2.7}^{+6.6}$ <0.3 44.44 44.45 1.04 SP
44 $31.2 \pm4.1$ $18.4\pm3.6$ - $0.26\pm0.11$ $\rm 19.5_{-7.5}^{+6.9}$ $\rm 1.7_{-0.8}^{+1.1}$ 43.94 44.01 1.24 SP
Column: (1) ID number; (2) count rate in the S band in units of 10-4 count/s; (3) count rate in the H band in units of 10-4 count/s; (4) Hardness Ratio between the H band and the S band computed with the formula H-S/${\rm H+S}$; (5) H band flux in units of 10-15 erg s-1 cm-2; (6) rest-frame column density $N_{\rm H}$ in units of 1022 cm-2; (7) logarithm of the observed luminosity in the H band (erg s-1); (8) logarithm of the absorption-corrected luminosity in the H band (erg s-1); (9) logarithm of the $\lambda $ $L_{5.8~\mu {\rm m}}$L2-10 ratio; (10) analysis method: SP for spectral fitting, HR for hardness ratio. For Chandra data the 2-10 keV count rate and flux was extrapolated from the 2-8 keV value assuming $\Gamma=1.9$.
a For these sources we computed the absorption-corrected luminosity using the lower limit on the $N_{\rm H}$ value. Accordingly, the intrinsic luminosity shown here is also a lower limit.

Source LaTeX | All tables | In the text

Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.

Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.

Initial download of the metrics may take a while.