discov_num |
notes |
refcode |
YSC 133 |
A first orbit for this system was reported recently in Tokovinin et |
Tok2015c |
|
al. (2015), but those authors assumed a quadrant flip of one data |
|
|
point taken by Horch et al. (2008). That was not an unreasonable |
Hor2008 |
|
assumption based on the relatively small magnitude difference, but the |
|
|
points presented here give support to an "alternate" orbit where no |
|
|
quadrant flips are needed and the period is about half of that derived |
|
|
in the earlier calculation. Given the revised Hipparcos parallax of |
|
|
13.55 +/- 0.43 mas, the new orbit gives a mass sum of 3.5 +/- 1.0Msun, |
|
|
which is somewhat high for a system of composite spectral type F7, but |
|
|
with substantial uncertainty at this stage. In contrast, the Tokovinin |
|
|
orbit gives a mass sum of about 1 Msun, which would seem to be too low |
|
|
by roughly the same amount. |
Hor2015b |
refcode |
metd |
author |
reference |
Hor2008 |
S j |
Horch, E.P., van Altena, W.F., Cyr, W.M., Jr., Kinsman-Smith, L., Srivastava, A., |
2008AJ....136..312H |
Hor2008 |
+orb |
& Zhou, J. |
|
Hor2008 |
|
AJ 136, 312, 2008 |
|
Hor2015b |
S j |
Horch, E.P., van Belle, G.T., Davidson, J.W., Jr., Ciastko, L.A., Everett, M.E., & |
2015AJ....150..151H |
Hor2015b |
|
Bjorkman, K.S. |
|
Hor2015b |
|
AJ 150, 151, 2015 |
|
Hor2021b |
S |
Horch, E.P., Broderick, K.G., Casetti-Dinescu, D.I., Henry, T.J., Fekel, F.C., |
2021AJ....161..295H |
Hor2021b |
|
Mutterspaugh, M.W., Willmarth, D.W., Winters, J.G., van Belle, G.T., Clark, C.A. & |
|
Hor2021b |
|
Everett, M.E. |
|
Hor2021b |
|
AJ 161, 295, 2021 |
|
Tok2015c |
orb+j |
Tokovinin, A., Mason, B.D., Hartkopf, W.I., Mendez, R.A., & Horch, E.P. |
2015AJ....150...50T |
Tok2015c |
+St |
AJ 150, 50, 2015 (some measures corrected in Tok2017b) |
2017AJ....154..110T |