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Home All issues Volume 494 / No 3 (February II 2009) A&A, 494 3 (2009) 987-1003 Full HTML
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Table 2:

JHK, Spitzer-GLIMPSE and MIPS magnitudes of discussed stars.
Star $\alpha_{2000}$ $\delta_{2000}$ J H $K_{\rm {S}}$ [3.6] [4.5] [5.8] [8.0] [24]
Objects discussed around RCW 82

4		 13$^{\rm h}$59$^{\rm m}$34.76$^{\rm s}$ -61 $\hbox{$^\circ$ }$19 $\hbox{$^\prime$ }$22.10 $\hbox{$^{\prime\prime}$ }$ 17.586: 15.055 12.408 10.127 8.999 8.771 8.258 5.04
9 14$^{\rm h}$00$^{\rm m}$01.65$^{\rm s}$ -61 $\hbox{$^\circ$ }$21 $\hbox{$^\prime$ }$54.76 $\hbox{$^{\prime\prime}$ }$ 15.892: 15.058 12.693 9.703 8.897 8.136 7.419 4.15
21 13$^{\rm h}$59$^{\rm m}$01.26$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$59.87 $\hbox{$^{\prime\prime}$ }$ 16.652 14.821 13.304 11.178 10.534 10.020 9.544 ...
22 13$^{\rm h}$59$^{\rm m}$06.76$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$55.77 $\hbox{$^{\prime\prime}$ }$       13.305 12.791 11.198 9.539 ...
23 13$^{\rm h}$59$^{\rm m}$17.56$^{\rm s}$ -61 $\hbox{$^\circ$ }$25 $\hbox{$^\prime$ }$49.26 $\hbox{$^{\prime\prime}$ }$ 17.067: 15.109 13.574 12.150 11.611 10.902 10.043 7.48
27 14$^{\rm h}$00$^{\rm m}$12.63$^{\rm s}$ -61 $\hbox{$^\circ$ }$20 $\hbox{$^\prime$ }$13.23 $\hbox{$^{\prime\prime}$ }$ 17.188: 12.422 9.390 7.040 6.611 5.932 5.205 1.85
35 13$^{\rm h}$59$^{\rm m}$50.89$^{\rm s}$ -61 $\hbox{$^\circ$ }$25 $\hbox{$^\prime$ }$22.23 $\hbox{$^{\prime\prime}$ }$ 13.723 12.207 10.780 8.622 7.837 7.074 6.110 2.58
47 13$^{\rm h}$58$^{\rm m}$57.77$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$25.58 $\hbox{$^{\prime\prime}$ }$ 16.613 14.451 12.407 10.201 9.583 9.143 8.687 ...
81 13$^{\rm h}$59$^{\rm m}$31.91$^{\rm s}$ -61 $\hbox{$^\circ$ }$20 $\hbox{$^\prime$ }$37.43 $\hbox{$^{\prime\prime}$ }$ 17.605 15.261 13.145 11.306 11.065 10.543 9.635 ...
98 13$^{\rm h}$59$^{\rm m}$36.76$^{\rm s}$ -61 $\hbox{$^\circ$ }$20 $\hbox{$^\prime$ }$48.25 $\hbox{$^{\prime\prime}$ }$ 16.267: 15.305 13.566 10.088 9.238 8.472 ... 4.01
106 13$^{\rm h}$59$^{\rm m}$05.86$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$26.50 $\hbox{$^{\prime\prime}$ }$ ... ...   10.867 8.570 6.382 4.485 ...
107 $^{\footnotesize b}$ 13$^{\rm h}$59$^{\rm m}$03.57$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$15.80 $\hbox{$^{\prime\prime}$ }$ 10.870 8.074 6.320 ... ... ... ... 1.47
Cluster, NTT field 1
51 13$^{\rm h}$59$^{\rm m}$57.61$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$36.85 $\hbox{$^{\prime\prime}$ }$ 17.811 $^{\footnotesize a}$ 13.795 $^{\footnotesize a}$ 11.127 $^{\footnotesize a}$ 8.192 7.538 6.157 4.724  
68 13$^{\rm h}$59$^{\rm m}$57.48$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$29.38 $\hbox{$^{\prime\prime}$ }$ 14.968 $^{\footnotesize a}$ 12.731 $^{\footnotesize a}$ 11.294 $^{\footnotesize a}$ 9.671 9.304 9.123 8.116  
53 13$^{\rm h}$59$^{\rm m}$59.94$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$22.14 $\hbox{$^{\prime\prime}$ }$ 19.762 $^{\footnotesize a}$ 16.419 $^{\footnotesize a}$ 14.088 $^{\footnotesize a}$ 11.921 11.290 10.692 10.059  
36 13$^{\rm h}$59$^{\rm m}$58.14$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$10.27 $\hbox{$^{\prime\prime}$ }$ 17.695 $^{\footnotesize a}$ 14.973 $^{\footnotesize a}$ 13.354 $^{\footnotesize a}$ 11.353 10.819 10.245 9.626 5.64
43 13$^{\rm h}$59$^{\rm m}$59.16$^{\rm s}$ -61 $\hbox{$^\circ$ }$23 $\hbox{$^\prime$ }$43.467 $\hbox{$^{\prime\prime}$ }$ 19.191 $^{\footnotesize a}$ 16.308 $^{\footnotesize a}$ 14.772 $^{\footnotesize a}$ 13.162 12.693 12.123 11.275  
102 $^{\footnotesize b}$ 13$^{\rm h}$59$^{\rm m}$48.40$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$20.23 $\hbox{$^{\prime\prime}$ }$ 15.287 $^{\footnotesize a}$ 11.323 $^{\footnotesize a}$ 9.341 $^{\footnotesize a}$ 7.791 7.715 7.249 7.087 5.80
A2 13$^{\rm h}$59$^{\rm m}$57.40$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$37.2 $\hbox{$^{\prime\prime}$ }$ ... 16.962 $^{\footnotesize a}$ 14.216 $^{\footnotesize a}$ ... ... ... ... ...
C2 13$^{\rm h}$59$^{\rm m}$57.12$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$34.4 $\hbox{$^{\prime\prime}$ }$ 19.359 $^{\footnotesize a}$ 17.381 $^{\footnotesize a}$ 15.951 $^{\footnotesize a}$ ... ... ... ... ...
E2 13$^{\rm h}$59$^{\rm m}$56.43$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$29.2 $\hbox{$^{\prime\prime}$ }$ 17.865 $^{\footnotesize a}$ 15.721 $^{\footnotesize a}$ 14.826 $^{\footnotesize a}$ ... ... ... ... ...
F2 13$^{\rm h}$59$^{\rm m}$56.88$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$41.2 $\hbox{$^{\prime\prime}$ }$ ... 15.594 $^{\footnotesize a}$ 13.889 $^{\footnotesize a}$ ... ... ... ... ...
L2 13$^{\rm h}$59$^{\rm m}$57.89$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$25.46 $\hbox{$^{\prime\prime}$ }$ 18.226 $^{\footnotesize a}$ 15.828 $^{\footnotesize a}$ 14.303 $^{\footnotesize a}$ 12.128 11.857 11.514 ... ...
M2 13$^{\rm h}$59$^{\rm m}$58.13$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$27.07 $\hbox{$^{\prime\prime}$ }$ ... 18.989 $^{\footnotesize a}$ 16.201 $^{\footnotesize a}$ 13.663 12.917 ... ... ...
P2 14$^{\rm h}$00$^{\rm m}$01.70$^{\rm s}$ -61 $\hbox{$^\circ$ }$24 $\hbox{$^\prime$ }$51.40 $\hbox{$^{\prime\prime}$ }$ 12.126 11.7096 11.504 11.270 11.162 ... ... ...
NTT field 2
A3 13$^{\rm h}$59$^{\rm m}$44.34$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$43.77 $\hbox{$^{\prime\prime}$ }$ 14.099 $^{\footnotesize a}$ 13.048 $^{\footnotesize a}$ 12.630 $^{\footnotesize a}$ 12.377 12.603 ... ... ...
B3 13$^{\rm h}$59$^{\rm m}$44.85$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$44.4 $\hbox{$^{\prime\prime}$ }$ 12.488 $^{\footnotesize a}$ 12.147 $^{\footnotesize a}$ 11.960 $^{\footnotesize a}$ ... ... ... ... ...
C3 13$^{\rm h}$59$^{\rm m}$44.71$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$51.1 $\hbox{$^{\prime\prime}$ }$ ... 15.172 $^{\footnotesize a}$ 13.683 $^{\footnotesize a}$ ... ... ... ... ...
D3 13$^{\rm h}$59$^{\rm m}$45.11$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$46.1 $\hbox{$^{\prime\prime}$ }$ 15.578 $^{\footnotesize a}$ 14.249 $^{\footnotesize a}$ 13.459 $^{\footnotesize a}$ ... ... ... ... ...
7 13$^{\rm h}$59$^{\rm m}$47.34$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$01.69 $\hbox{$^{\prime\prime}$ }$ 18.766 $^{\footnotesize a}$ 15.847 $^{\footnotesize a}$ 14.028 $^{\footnotesize a}$ 11.284 10.235 9.111 8.167 ...
J3 13$^{\rm h}$59$^{\rm m}$46.87$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$09.26 $\hbox{$^{\prime\prime}$ }$ 15.914 $^{\footnotesize a}$ 14.573 $^{\footnotesize a}$ 13.484 $^{\footnotesize a}$ 11.882 11.445 11.381 ... ...
N3 13$^{\rm h}$59$^{\rm m}$48.89$^{\rm s}$ -61 $\hbox{$^\circ$ }$23 $\hbox{$^\prime$ }$03.4 $\hbox{$^{\prime\prime}$ }$ 17.606 $^{\footnotesize a}$ 16.076 $^{\footnotesize a}$ 14.861 $^{\footnotesize a}$ ... ... ... ... ...
O3 13$^{\rm h}$59$^{\rm m}$49.38$^{\rm s}$ -61 $\hbox{$^\circ$ }$23 $\hbox{$^\prime$ }$04.01 $\hbox{$^{\prime\prime}$ }$ ... ... 15.035 $^{\footnotesize a}$ 12.276 11.453 10.599 ... ...
Candidate exciting stars
e1 13$^{\rm h}$59$^{\rm m}$29.93$^{\rm s}$ -61 $\hbox{$^\circ$ }$23 $\hbox{$^\prime$ }$07.78 $\hbox{$^{\prime\prime}$ }$ 10.090 9.549 9.093 8.439 8.275 8.000 7.656 ...
e2 13$^{\rm h}$59$^{\rm m}$29.17$^{\rm s}$ -61 $\hbox{$^\circ$ }$23 $\hbox{$^\prime$ }$03.02 $\hbox{$^{\prime\prime}$ }$ 9.934 9.587 9.403 9.211 9.218 9.225 9.098 ...
e3 13$^{\rm h}$59$^{\rm m}$ 28.11$^{\rm s}$ -61 $\hbox{$^\circ$ }$22 $\hbox{$^\prime$ }$59.12 $\hbox{$^{\prime\prime}$ }$ 9.741 9.409 9.188 8.972 9.020 9.114 9.149 ...
e4 13$^{\rm h}$59$^{\rm m}$ 27.39$^{\rm s}$ -61 $\hbox{$^\circ$ }$23 $\hbox{$^\prime$ }$19.34 $\hbox{$^{\prime\prime}$ }$ 12.792 10.438 9.352 8.623 8.826 8.505 8.472 ...
$^{\footnotesize a}$ NTT magnitude; $^{\footnotesize b}$ giant stars.

Source LaTeX | All tables | In the text

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