No. | Source ID | C1a | C2a | X1a | X2a | X3a |
(cnts/ks) | (cnts/ks) | (cnts/ks) | (cnts/ks) | (cnts/ks) | ||
1 | IRS 2 |
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2 | Source 5 | n.d. | n.d. | n.d. | n.d. | n.d. |
3 |
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n.d. | n.d. | n.d. | |
4 | IRS 5 |
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5 | n.d. | n.d. | n.d. | n.d. | n.d. | |
6 | IRS 6 |
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7 | IRS 1 |
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8 | IRS 9 |
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9 | R CrA |
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10 | n.d. | n.d. | n.d. | n.d. | n.d. | |
11 | Source 9 | n.d. | n.d. | n.d. | n.d. | n.d. |
12 | IRS 7W |
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13 | n.d. | n.d. | n.d. | n.d. | n.d. | |
14 | IRS 7E |
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15 | n.d. | n.d. | n.d. | n.d. | n.d. |
a Background-subtracted count rates (0.5-10 keV) from X-ray datasets as listed in Table 2, Chandra and XMM-Newton count rates are not directly comparable. Additionally, different filters were used in the XMM-Newton observations: "thin'' for X1 and "medium'' for X2/X3. b Flare. c Source partly covered by chip gap, loss estimated to be ![]() d Contamination from neighbouring source. |