Scott W. Fleming, Jian Ge, Rory Barnes, Thomas G. Beatty, Justin R. Crepp, Nathan De Lee, Massimiliano Esposito, Bruno Femenia, Leticia Ferreira, Bruce Gary, B. Scott Gaudi, Luan Ghezzi, Jonay I. González Hernández, Leslie Hebb, Peng Jiang, Brian Lee, Ben Nelson, Gustavo F. Porto de Mello, Benjamin J. Shappee, Keivan Stassun, Todd A. Thompson, Benjamin M. Tofflemire, John P. Wisniewski, W. Michael Wood-Vasey, Eric Agol, Carlos Allende Prieto, Dmitry Bizyaev, Howard Brewington, Phillip A. Cargile, Louis Coban, Korena S. Costello, Luis N. da Costa, Melanie L. Good, Nelson Hua, Stephen R. Kane, Gary R. Lander, Jian Liu, Bo Ma, Suvrath Mahadevan, Marcio A. G. Maia, Elena Malanushenko, Viktor Malanushenko, Demitri Muna, Duy Cuong Nguyen, Daniel Oravetz, Martin Paegert, Kaike Pan, Joshua Pepper, Rafael Rebolo, Eric J. Roebuck, Basilio X. Santiago, Donald P. Schneider, Alaina Shelden, Audrey Simmons, Thirupathi Sivarani, Stephanie Snedden, Chelsea L. M. Vincent, Xiaoke Wan, Ji Wang, Benjamin A. Weaver, Gwendolyn M. Weaver, Bo Zhao
We report the discovery via radial velocity of a short-period (P = 2.430420 \pm 0.000006 days) companion to the F-type main sequence star TYC 2930-00872-1. A long-term trend in the radial velocities indicates the presence of a tertiary stellar companion with $P > 2000$ days. High-resolution spectroscopy of the host star yields T_eff = 6427 +/- 33 K, log(g) = 4.52 +/- 0.14, and [Fe/H]=-0.04 +/- 0.05. These parameters, combined with the broad-band spectral energy distribution and parallax, allow us to infer a mass and radius of the host star of M_1=1.21 +/- 0.08 M_\odot and R_1=1.09_{-0.13}^{+0.15} R_\odot. We are able to exclude transits of the inner companion with high confidence. The host star's spectrum exhibits clear Ca H and K core emission indicating stellar activity, but a lack of photometric variability and small v*sin(I) suggest the primary's spin axis is oriented in a pole-on configuration. The rotational period of the primary from an activity-rotation relation matches the orbital period of the inner companion to within 1.5 \sigma, suggesting they are tidally locked. If the inner companion's orbital angular momentum vector is aligned with the stellar spin axis, as expected through tidal evolution, then it has a stellar mass of M_2 ~ 0.3-0.4 M_\odot. Direct imaging limits the existence of stellar companions to projected separations < 30 AU. No set of spectral lines and no significant flux contribution to the spectral energy distribution from either companion are detected, which places individual upper mass limits of M < 1.0 M_\odot, provided they are not stellar remnants. If the tertiary is not a stellar remnant, then it likely has a mass of ~0.5-0.6 M_\odot, and its orbit is likely significantly inclined from that of the secondary, suggesting that the Kozai-Lidov mechanism may have driven the dynamical evolution of this system.
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http://arxiv.org/abs/1206.5514
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