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Table 1

Herschel observations and monochromatic flux densities of six unpublished and two reanalysed targets.

Target 1st OBSIDs Dur. Mid-time r Δ α Flux densities [mJy]
of visit 1/2 (min) (AU) (AU) (°) 70 μm 100 μm 160 μm
1995 SM55 1342190925/...0994 73.1 2010-Feb-22 11:58 38.62 38.99 1.37 <1.7 <1.7 <2.7
2005 RR43 1342190957/...1033 73.1 2010-Feb-23 00:16 38.73 38.88 1.45 2.6 ± 1.8 4.6 ± 2.4 <2.8
2003 UZ117 1342190961/...1037 109.3 2010-Feb-23 01:07 39.27 39.50 1.41 2.0 ± 1.6 <2.2 <2.3
2003 OP32 1342197669/...7721 75.7 2010-Jun-03 20:31 41.53 41.31 1.39 1.7 ± 1.5 <2.1 <4.1
2002 TX300 1342212764/...2802 188.5 2011-Jan-17 03:46 41.68 41.76 1.36 1.2 ± 1.1 <2.8 <4.1
1996 TO66 1342222430/...2481 188.5 2011-Jun-10 11:25 46.92 47.34 1.14 <1.2 <1.3 <2.9

1999 CD158 1342206024/...6060 150.9 2010-Oct-08 05:01 47.40 47.83 1.09 <1.3 <1.6 <2.1
1999 KR16 1342212814/...3071 188.5 2011-Jan-18 06:14 35.76 36.06 1.51 4.2 ± 1.1a 6.9 ± 2.2a <4.5

Notes. Targets 2002 TX300 (Lellouch et al. 2013)and 1999 KR16 (Santos-Sanz et al. 2012) have been reanalysed and their flux densities updated in this work. OBSIDs are observation identifiers in the Herschel Science Archive. The first OBSID of the consecutive OBSIDs/visit are given. Duration is the total duration of the two visits (70 and 100 μm filters were used for half of the duration each), mid-time is the mean UT time, r is the heliocentric distance at mid-time, Δ is the Herschel-target distance at mid-time, and α is the Sun-target-Herschel phase angle at mid-time (JPL Horizons Ephemeris System; Giorgini et al. 1996). Flux densities are colour-corrected and the 1σ uncertainties include the absolute calibration uncertainty of 5% in all bands. Targets above the horizontal line are confirmed Haumea family members while those below the line are probable dynamical interlopers. (a) Differential fluxes from visit 1 only. During visit 2 a background source was near the target location. This background source is close to the edge of the images from visit 1 and could not be properly compensated by the positive and negative images.

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