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Table 1

X-ray observations of IGR J05414-6858.

Observation ObsID Date Time Instrument Modea Offaxb Net Exp Net Ctsc R sc d
(UT) [′] [ks] [′′]

XMM 2001 0094410101 2001-10-19 17:49–20:30 EPIC-pn ff-medium 8.2 8.2  <26 30
17:09–20:29 EPIC-MOS1 ff-medium 7.2 11.7  <5 30
17:09–20:29 EPIC-MOS2 ff-medium 6.9 11.7  <14 30

XMM 2011 0679380101 2011-08-13 07:45–14:07 EPIC-pn ff-thin 1.1 7.2 2018 21
07:22–14:07 EPIC-MOS1 ff-medium 1.2 9.4 863 29
07:22–14:07 EPIC-MOS2 ff-medium 1.2 9.4 954 31

Swift 2010a 00031745001 2010-06-25 05:35–09:10 XRT pc 5.3 3.9 221 40
Swift 2010b 00031745002 2010-06-30 01:14–23:59 XRT pc 2.0 5.2 497 50

Swift 2011a 00045428001 2011-08-05 15:28–22:26 XRT pc 10.5 3.3 40 40
Swift 2011b 00031745003 2011-08-09 23:53–04:55 XRT pc 1.8 3.7 120 40
Swift 2011c 00031745004 2011-08-12 00:03–22:53 XRT pc 2.4 4.1 100 40
Swift 2011d 00031745005 2011-08-20 00:25–16:53 XRT pc 3.1 2.1  <6 40
Swift 2011e 00031745006 2011-08-24 02:44–04:29 XRT pc 2.5 1.2  <5 40

Notes. 

(a)

Observation setup: full-frame mode (ff) and photon-counting mode (pc). For XMM-Newton, the filter is given as well.

(b)

Off-axis angle under which the source was observed.

(c)

Net counts as used for spectral analysis in the (0.2−10.0) keV band for XMM-Newton and in the (0.3−6.0) keV band for Swift.

(d)

Radius of the circular source extraction region.

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