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Table 1

X-ray observations of 1ES 0229+200 showing the results for the annual binning of XMM-Newton, Swift, and RXTE, as well as historical observations from Einstein (Elvis et al. 1992), ROSAT (Brinkmann et al. 1995) and BeppoSAX (Donato et al. 2005).

Instrument Time Obs. ID Energy range Photon index F2 − 10   keV,deabs(ergcm-2s-1)

XMM-Newton 21., 23. August 2009 604 210 201, 604 210 301 0.1–15 keV 1.84 ± 0.02 (9.0 ± 0.1) × 10-12
Swift/XRT 5., 7., 8. August 2008 31 249 001–31 249 003 0.2–10 keV 1.87 ± 0.05 (1.03 ± 0.04) × 10-11
Swift/XRT 19. Oct.–23. Nov. 2009 31 249 004–31 249 019 0.2–10 keV 1.73 ± 0.03 (1.47 ± 0.04) × 10-11
RXTE/PCA 1. Jan.–13. Oct. 2010 95 387 3–60 keV 1.92 ± 0.05 (1.23 ± 0.04) × 10-11
BeppoSAX 16. July 2001 51 472 001 0.1–50 keV 1.99 ± 0.05 1.5 × 10-11
ROSAT 0.1–2.4 keV (4.5 ± 0.6) × 10-12 at 1 keV
Einstein 0.4–4.0 keV (7.6 ± 2.2) × 10-12 at 1 keV

Notes. The measured fluxes are given for the energy range between 2 and 10 keV. For the ROSAT and Einstein observations, the fluxes are determined at an energy of 1 keV. The absorption derived from the high precision XMM-Newton spectra of NH = 1.1 × 1021cm2 was used for the XMM-Newton, Swift, and RXTE spectra to determine the unabsorbed flux. The absorption detected in the BeppoSAX spectrum was NH = 1.0 × 1021cm2 (Donato et al. 2005).

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