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Table 2

Properties of the X-ray/NIR flares observed so far.

References Date Instruments NIR filtera LX/Lquiesb FNIRc d Id.
          [mJy] [mJy]  

[1] ............... 2009 Apr. 1 XMM/VLT 3.8 μm (L′)  < 7 19 ... A
[1] ............... 2009 Apr. 3 XMM/VLT 3.8 μm (L′) 10 8 ... B
[2, 3] ............ 2007 Apr. 4 XMM/VLT 3.8 μm (L′) 103 26 ... C
[2, 4] ............ 2007 Apr. 4 XMM/HST 1.7 μm 26 7 16 D
[2, 4] ............ 2007 Apr. 4 XMM/HST 1.7 μm 37 4 9 E
[2, 4] ............ 2007 Apr. 2 XMM/HST 1.7 μm 14 10 22 F
[5, 6] ............ 2004 Aug. 31 XMM/HST 1.6 μm  < 40 10 24 G
[7] ............... 2005 Jul. 31 Chandra/Keck 3.8 μm (L′)  < 1.2 15 ... H
[7] ............... 2006 Jul. 17 Chandra/Keck 3.8 μm (L′) 20  > 5 ... I
[8] ............... 2005 Jun. 30 Chandra/VLT 2.1 μm (Ks) 3 14 4 J
[9] ............... 2005 Jul. 7 Chandra/VLT 2.1 μm (Ks) 15 11 3 K
[10] .............. 2003 Jun. 19 Chandra/VLT 2.1 μm (Ks) 3  > 7  > 2 L

Notes. 

(a)

The HST 1.6 and 1.7 μm pass-bands correspond to the NICMOS filters F160W and F170M, respectively.

(b)

Peak X-ray luminosity (2–10 keV) in units of the quiescent level (~2 × 1033 erg s-1, Baganoff et al. 2003). “ > ” and “ < ” signs were added when the peak flux was missed or not simultaneous with the NIR peak.

(c)

Background-subtracted peak NIR-fluxes in the bands indicated in the fourth column, dereddened assuming A1.6   μm = 4.5 mag, A1.7   μm = 5.03 mag, A2.1   μm = 2.8 mag, and A3.8   μm = 1.8 mag.

(d)

Equivalent NIR flux in the L′-band extrapolated assuming a power-law spectral index α =  −1 (see Sect. 4).

References. [1] This work, [2] Porquet et al. (2008), [3] Dodds-Eden et al. (2009), [4] Yusef-Zadeh et al. (2009), [5] Bélanger et al. (2005), [6] Yusef-Zadeh et al. (2006a), [7] Hornstein et al. (2007), [8] Eckart et al. (2008a), [9] Eckart et al. (2006a), [10] Eckart et al. (2004).

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