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Table 2.

W2 unabsorbed fluxes and luminosities (0.3–10 keV) for each observation.

Obs. ID (a) Funabs LX
(10−14 erg cm−2 s−1) (1032 erg s−1)
78* 6 ± 2 1.5 ± 0.5
953 1.4 0.3 + 0.5 $ ^{+0.5}_{-0.3} $ 0.34 0.07 + 0.12 $ ^{+0.12}_{-0.07} $
955 6.2 0.7 + 0.8 $ ^{+0.8}_{-0.7} $ 1.5 ± 0.2
956* 6.5 2.2 + 2.0 $ ^{+2.0}_{-2.2} $ 1.6 ± 0.5
2735 6.4 0.4 + 0.5 $ ^{+0.5}_{-0.4} $ 1.5 0.09 + 0.12 $ ^{+0.12}_{-0.09} $
3384* 8 ± 2 2.0 ± 0.5
2736 5.8 ± 0.4 1.42 ± 0.09
3385* 9 ± 2 2.2 ± 0.5
2737 7.1 0.2 + 0.3 $ ^{+0.3}_{-0.2} $ 1.73 0.05 + 0.07 $ ^{+0.07}_{-0.05} $
3386* 2 ± 1 0.5 ± 0.2
2738 8.4 ± 0.6 2.0 ± 0.1
3387* 2.6 0.9 + 1.1 $ ^{+1.1}_{-0.9} $ 0.6 0.2 + 0.3 $ ^{+0.3}_{-0.2} $
16527 3.9 0.4 + 0.6 $ ^{+0.6}_{-0.4} $ 0.95 0.09 + 0.14 $ ^{+0.14}_{-0.09} $
15747 5.7 ± 0.6 1.4 ± 0.1
16529 4.8 ± 0.7 1.2 ± 0.2
17420 4 ± 1 1.0 ± 0.2
15748 5 ± 1 1.2 ± 0.2
26229 2 ± 1 0.5 ± 0.2
26286 ≤2.8 (b) ≤0.7 (b)

Notes. Fluxes and luminosities have been obtained for the thermal Bremsstrahlung model, having N H 47 Tuc + local $ N_{\mathrm{H}}^{\mathrm{47\,Tuc + local}} $ and kT fixed at 1.1 × 1021 cm−2 and 10 keV, respectively.

(a)

Observations with exposure times shorter than the orbital period are marked with an asterisk.

(b)

Upper limit at 90% c.l.

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