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2. IR observations

The sources were observed with the MkIII infrared photometer (Glass 1985) on the SAAO 1.9-m telescope. A chopping secondary mirror defines two effective apertures: on-source (star) and off-source (background). Square apertures of 9'' or 12'' were used, depending on the seeing. A single observation module consisted of a 40 s integration, with the star placed alternately in the two apertures by nodding the telescope. These individual 40 s observations were then repeated, typically 2-4 times per filter, until a sufficient precision (standard error tex2html_wrap_inline8450.01 magnitudes) was achieved. The observations were obtained in the SAAO JHK system (1.25, 1.65 & 2.2 microns; Carter 1990) in photometric conditions, transformations being affected from regular observations of IR standards.

The observations were carried out during the period December 1993 - November 1995 at approximately quarterly intervals. The result from the observation of each source taken on a good photometric night, and a measure of its variability are presented in Table 1 (click here).

 

 
Source RA (2000) Dec (2000) Obs. date J H K N F
Name hr mn sc tex2html_wrap_inline865
RX J0051.8-7231 00 51 53.4 -72 31 56.5 02 Oct. 1996 13.95tex2html_wrap_inline8690.11 14.06tex2html_wrap_inline8690.19 14.55tex2html_wrap_inline8690.42 1 -
1E0050.1-7247
RX J0059.2-7138 00 59 12.7 -71 38 44.8 02 Oct. 1996 13.95tex2html_wrap_inline8690.09 14.12tex2html_wrap_inline8690.23 13.74tex2html_wrap_inline8690.24 1 -
SMC X-3 00 52 07.7 -72 25 43.7 17 Nov. 1995 14.67tex2html_wrap_inline8690.14 14.78tex2html_wrap_inline8690.45 14.63tex2html_wrap_inline8690.46 6 0.17
SMC X-2 00 54 34.7 -73 40 43.2 02 Oct. 1993 14.80tex2html_wrap_inline8690.10 15.0tex2html_wrap_inline8690.30 14.5tex2html_wrap_inline8690.20 3 0.09
RX J005354-722600 53 52.8 -72 26 34.4 14 Nov. 1995 13.18tex2html_wrap_inline8690.05 12.93tex2html_wrap_inline8690.05 12.84tex2html_wrap_inline8690.06 2 0.25
1E0052.1-7242
RX J0101.0-7206 01 01 03.2 -72 06 57 02 Oct. 1996 14.69tex2html_wrap_inline8690.32 14.15tex2html_wrap_inline8690.43 14.03tex2html_wrap_inline8690.09 1 -
RX J0103-722 01 03 13.9 -72 09 14.1 30 Jun. 1994 14.85tex2html_wrap_inline8690.34 1 -
SMC X-1 01 16 41.9 -73 26 12.4 14 Nov. 1995 13.47tex2html_wrap_inline8690.04 13.55tex2html_wrap_inline8690.06 13.43tex2html_wrap_inline8690.15 7 0.030
Sk160
RX J0501.6-7034 05 01 24.5 -70 33 30 02 Oct. 1996 13.74tex2html_wrap_inline8690.19 12.85tex2html_wrap_inline8690.03 12.85tex2html_wrap_inline8690.05 1 -
CAL 9
RX J0502.9-6626 05 02 52.5 -66 26 26 02 Oct. 1996 14.24tex2html_wrap_inline8690.02 14.65tex2html_wrap_inline8690.09 14.33tex2html_wrap_inline8690.11 1 -
CAL E
EXO 0531.1-6609 05 31 12.0 -66 07 08 02 Oct. 1996 13.99tex2html_wrap_inline8690.06 13.92tex2html_wrap_inline8690.08 13.57tex2html_wrap_inline8690.08 1 -
RX J0532.5-6551 05 32 32.6 -65 51 40.8 03 Oct. 1996 13.50tex2html_wrap_inline8690.06 13.45tex2html_wrap_inline8690.02 13.60tex2html_wrap_inline8690.14 1 -
Sk -65 66
LMC X-4 05 32 49.2 -66 22 14.4 5 Mar. 1993 14.58tex2html_wrap_inline8690.10 14.80tex2html_wrap_inline8690.20 14.90tex2html_wrap_inline8690.30 5 0.046
A0538-66 05 35 40.27 -66 51 52.9 14 Nov. 1995 14.99tex2html_wrap_inline8690.25 15.08tex2html_wrap_inline8690.36 15.8tex2html_wrap_inline8691.3 1 -
H0544-665 05 44 15.4 -66 33 50.2 17 Nov. 1995 13.73tex2html_wrap_inline8690.09 12.72tex2html_wrap_inline8690.07 12.74tex2html_wrap_inline8690.08 3 0.11
Source no:22
1H0739-529 07 47 23.5 -53 19 58.3 14 Nov. 1995 7.46tex2html_wrap_inline8690.01 7.42tex2html_wrap_inline8690.01 7.41tex2html_wrap_inline8690.01 6 0.006
HD63666
1H0749-600 07 56 15.8 -61 05 59.4 14 Nov. 1995 6.60tex2html_wrap_inline8690.01 6.56tex2html_wrap_inline8690.01 6.55tex2html_wrap_inline8690.01 6 0.008
HD65663
GRO J1008-57.110 09 46.9 -58 17 35.5 14 Nov. 1995 11.57tex2html_wrap_inline8690.03 10.91tex2html_wrap_inline8690.01 10.49tex2html_wrap_inline8690.01 5 0.066
1E1024.0-5732 10 25 56.5 -57 48 41.1 14 Nov. 1995 8.88tex2html_wrap_inline8690.01 8.23tex2html_wrap_inline8690.01 7.87tex2html_wrap_inline8690.01 5 0.018
Wack2134
A1118-615 11 20 52.9 -61 54 52.2 14 Nov. 1995 9.66tex2html_wrap_inline8690.01 9.09tex2html_wrap_inline8690.01 8.64tex2html_wrap_inline8690.01 8 0.009
He3-640/Wray763
2U1119-603 11 21 15.2 -60 37 24.2 14 Nov. 1995 11.33tex2html_wrap_inline8690.03 10.86tex2html_wrap_inline8690.01 10.57tex2html_wrap_inline8690.01 4 0.103
Cen X-3/V779Cen
1E1145.1-6141 11 47 28.5 -61 57 13.5 21 Feb. 1995 9.71tex2html_wrap_inline8690.01 9.17tex2html_wrap_inline8690.02 8.90tex2html_wrap_inline8690.02 7 0.009
V830Cen
2S1145-619 11 48 00.1 -62 12 24.5 21 Feb. 1995 8.66tex2html_wrap_inline8690.01 8.44tex2html_wrap_inline8690.02 8.19tex2html_wrap_inline8690.02 8 0.089
V801Cen/HD102567
3U1223-624 12 26 37.6 -62 46 13.2 23 Feb. 1995 6.83tex2html_wrap_inline8690.01 6.11tex2html_wrap_inline8690.01 5.72tex2html_wrap_inline8690.01 7 0.010
GX301-2/WRA 977
1H1253-761 12 39 14.9 -75 22 11.8 22 Feb. 1995 6.18tex2html_wrap_inline8690.01 6.15tex2html_wrap_inline8690.01 6.11tex2html_wrap_inline8690.01 4 0.050
HD109857
GX304-1 13 01 16.4 -61 36 14.4 23 Feb. 1995 9.86tex2html_wrap_inline8690.01 9.28tex2html_wrap_inline8690.01 9.02tex2html_wrap_inline8690.01 8 0.012
V850Cen
SS 2883 13 02 47.6 -63 51 19.9.2 23 Feb. 1995 8.08tex2html_wrap_inline8690.01 7.71tex2html_wrap_inline8690.02 7.27tex2html_wrap_inline8690.02 7 0.013
PSR 1259-63
4U1538-52 15 42 23.2 -52 23 09.9 22 Feb. 1995 10.56tex2html_wrap_inline8690.01 10.35tex2html_wrap_inline8690.01 10.14tex2html_wrap_inline8690.01 4 0.033
QVNor/Nor X-2
1H1555-552 15 54 21.9 -55 19 43.6 22 Feb. 1995 7.14tex2html_wrap_inline8690.01 6.84tex2html_wrap_inline8690.01 6.51tex2html_wrap_inline8690.01 5 0.018
HD141926
2S1728-247 17 32 01.6 -24 43 50.7 30 Jun. 1993 10.20tex2html_wrap_inline8690.20 8.72tex2html_wrap_inline8690.03 8.13tex2html_wrap_inline8690.02 7 0.029
AX1845.0-0433 18 45 01.5 -04 33 55.0 03 Oct. 1996 10.17tex2html_wrap_inline8690.02 10.61tex2html_wrap_inline8690.02 11.55tex2html_wrap_inline8690.04 8 0.07
Table 1: List of sources observed in this programme. N is the number of observations and F is the fluctuation factor (the range of J magnitudes observed divided by the number of observations)


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