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Table 1

Spitzer light curves used in this work.

Program AOR Start IRAC band N p Baseline BLISS BLISS β w β r
ID ID date (μm) model N x N y

542 39218176 2010 Apr. 26 3.6 101 0 0 0.92 1.06
542 39217920 2010 Apr. 27 4.5 103 p([xy2 + l2) 0 0 0.85 1.20
70148 40216832 2010 Oct. 16 3.6 110 0 0 0.93 1.56
70148 40217088 2010 Oct. 17 4.5 109 0 0 0.85 1.33
70148 40217344 2010 Oct. 25 3.6 109 0 0 0.66 1.15
70148 40217600 2010 Oct. 27 4.5 109 0 0 1.04 1.05
70148 40217856 2010 Oct. 28 3.6 110 p([xy2 + l2) 0 0 0.93 1.00
70148 40211882 2010 Oct. 31 4.5 109 0 0 0.96 1.59
70049 42045952 2011 Apr. 29 4.5 666 10 11 0.93 1.17
70049 42046208 2011 Apr. 30 4.5 667 11 10 0.99 1.20
70049 42046464 2011 May 1 4.5 597 9 9 0.98 1.37
70049 42046720 2011 May 2 4.5 663 9 10 0.99 1.15
70049 42046976 2011 May 3 4.5 667 10 9 0.96 1.40
70049 42047232 2011 May 4 4.5 610 10 9 0.94 1.19
70049 42047488 2011 May 5 4.5 665 9 10 0.92 1.17
70049 42047744 2011 May 6 4.5 667 9 9 0.87 1.07
70049 42048000 2011 May 7 4.5 472 8 8 0.93 1.74
70049 42048256 2011 May 8 4.5 667 p([xy2) 10 9 0.94 1.03
70049 42048512 2011 May 9 4.5 666 10 9 0.98 1.21
70049 42048768 2011 May 10 4.5 667 10 10 0.98 1.81
70049 42049280 2011 May 11 4.5 666 9 9 0.89 1.18
70049 42049536 2010 May 12 4.5 112 0 0 0.91 1.16
70049 42050048 2011 May 14 4.5 655 10 9 0.98 1.77
70049 42050304 2011 May 15 4.5 667 10 10 0.95 1.16
70049 42050560 2011 May 16 4.5 583 10 9 0.83 1.27
70049 42050816 2011 May 17 4.5 667 11 10 0.90 1.45
70049 42051072 2011 May 18 4.5 667 10 10 0.89 1.12
70049 42051328 2011 May 19 4.5 639 10 9 0.89 1.67
70049 44591872 2011 Nov. 6 3.6 660 11 10 0.89 1.54
70049 44592128 2011 Nov. 7 3.6 443 7 8 0.82 1.29

Notes. Each light curve corresponds to a specific Spitzer observing block (AOR). For each of them, the table gives the ID of the Spitzer program and of the AOR, the start date, the IRAC channel used, the number of measurements, the baseline function selected for our global modeling (see Sect. 3), the number of divisions in the x- and y-directions used for the BLISS pixel mapping (see Sect. 3), and the βw and βr error rescaling factors (see Sect. 3). For the baseline function, p(ϵN) denotes, respectively, a N-order polynomial function of the logarithm of time (ϵ = l), of the PSF x- and y-positions (ϵ =  [xy]), and widths (ϵ = wx & wy).

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