January
2018
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2018ApJ...853...70U
Authors
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Udalski, A.
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Han, C.
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Bozza, V.
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Gould, A.
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Bond, I. A.
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and
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Mróz, P.
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Skowron, J.
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Wyrzykowski, Ł.
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Szymański, M. K.
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Soszyński, I.
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Ulaczyk, K.
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Poleski, R.
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Pietrukowicz, P.
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Kozłowski, S.
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OGLE Collaboration
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Abe, F.
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Barry, R.
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Bennett, D. P.
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Bhattacharya, A.
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Donachie, M.
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Evans, P.
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Fukui, A.
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Hirao, Y.
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Itow, Y.
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Kawasaki, K.
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Koshimoto, N.
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Li, M. C. A.
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Ling, C. H.
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Masuda, K.
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Matsubara, Y.
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Miyazaki, S.
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Munakata, H.
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Muraki, Y.
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Nagakane, M.
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Ohnishi, K.
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Ranc, C.
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Rattenbury, N.
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Saito, T.
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Sharan, A.
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Sullivan, D. J.
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Sumi, T.
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Suzuki, D.
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Tristram, P. J.
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Yamada, T.
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Yonehara, A.
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MOA Collaboration
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Street, R. A.
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Tsapras, Y.
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Bachelet, E.
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Bramich, D. M.
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DÁgo, G.
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Dominik, M.
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Figuera Jaimes, R.
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Horne, K.
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Hundertmark, M.
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Kains, N.
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Menzies, J.
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Schmidt, R.
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Snodgrass, C.
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Steele, I. A.
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Wambsganss, J.
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Robonet Collaboration
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Pogge, R. W.
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Jung, Y. K.
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Shin, I. -G.
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Yee, J. C.
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Kim, W. -T.
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μFun Collaboration
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Beichman, C.
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Carey, S.
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Calchi Novati, S.
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Zhu, W.
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Spitzer Team
Abstract
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We present the analysis of the binary-microlensing event OGLE-2014-BLG-0289. The event light curve exhibits five very unusual peaks, four of which were produced by caustic crossings and the other by a cusp approach. It is found that the quintuple-peak features of the light curve provide tight constraints on the source trajectory, enabling us to precisely and accurately measure the microlensing parallax {π }{{E}}. Furthermore, the three resolved caustics allow us to measure the angular Einstein radius {θ }{{E}}. From the combination of {π }{{E}} and {θ }{{E}}, the physical lens parameters are uniquely determined. It is found that the lens is a binary composed of two M dwarfs with masses {M}1=0.52+/- 0.04 {M}⊙ and {M}2=0.42+/- 0.03 {M}⊙ separated in projection by {a}\perp =6.4+/- 0.5 {au}. The lens is located in the disk with a distance of {D}{{L}}=3.3+/- 0.3 {kpc}. The reason for the absence of a lensing signal in the Spitzer data is that the time of observation corresponds to the flat region of the light curve.
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