Table 2:

Herschel observing geometries for our seven targets, including properties derived from ground-based visible observations and the obtained radiometric solutions.
Target r [AU] $\Delta$ [AU] $\alpha$ $[^\circ]$ HV [mag] $\Delta_{\rm mag}$ P [h] Ref. $D^{\rm TPM}_{\rm eff}$ $p^{\rm TPM}_V$ $\Gamma$ $\eta $
2003 AZ84 45.376 44.889 1.11 3.83 $\pm$ 0.04 0.14 $\pm$ 0.03 6.79 h 1, 2, 3 850-970 0.05-0.09 2-10 1.31
2001 YH140 36.576 36.169 1.44 5.8 $\pm$ 0.2 0.13 $\pm$ 0.05 13.2 h 4 300-390 0.06-0.10 0-10 1.2$^{\star}$
1997 CS29 43.509 43.241 1.27 5.65 $\pm$ 0.09 <0.08, <0.22 -- 5, 6, 7, 8 250-420 0.06-0.14 0-25 1.2$^{\star}$
2000 YW134 44.125 43.833 1.25 4.88 $\pm$ 0.05 <0.10 -- 9, 10 <500 >0.08 0-25 --
Typhon 17.943 18.376 2.84 7.68 $\pm$ 0.04 0.07 $\pm$ 0.01 9.67 h 4, 11, 12 134-154 0.065-0.085 1-10 0.96
2006 SX368 11.972 12.271 4.48 9.5 -- -- MPC 70-80 0.05-0.06 0-40 1.2$^{\star}$
2005 TB190 46.377 46.683 1.17 4.58 $\pm$ 0.22 0.12 $\pm$ 0.02 12.68 h 13 335-410 0.15-0.24 0-25 1.2$^{\star}$

Notes. r: Sun-target distance, $\Delta$: Herschel-target distance, $\alpha$: phase angle; HV magnitudes, lightcurve  $\Delta_{\rm mag}$, and the rotation period P; references for the preceeding three columns, derived effective diameter  $D^{\rm TPM}_{\rm eff}$ in [km] and geometric albedo  $p^{\rm TPM}_V$ values from the TPM analysis, the corresponding possible thermal inertias $\Gamma$ [J m-2 s-0.5 K-1], and the fitted NEATM $\eta $ value ($^{\star}$: for a fixed value).

References. (1) Fornasier et al. (2004); (2) DeMeo et al. (2009); (3) Perna et al. (2010); (4) Thirouin et al. (2010); (5) Sheppard & Jewitt (2002); (6) Romanishin & Tegler (1999); (7) Davies et al. (2000); (8) Boehnhardt et al. (2001); (9) Sheppard & Jewitt (2003); (10) Doressoundiram et al. (2005); (11) Rabinowitz et al. (2007); (12) Tegler et al. (2003); (13) Thirouin et al., in prep.; MPC: http://www.cfa.harvard.edu/iau/lists/Centaurs.html


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