OGLE-2014-BLG-0289: Precise Characterization of a Quintuple-peak Gravitational Microlensing Event
OGLE-2014-BLG-0289: Precise Characterization of a Quintuple-peak Gravitational Microlensing Event
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DOI:
10.3847/1538-4357/aaa295
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发表时间:
2018-01
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通讯作者:
A. Udalski;C. Han;V. Bozza;A. Gould;I. Bond;P. Mr'oz;J. Skowron;Ł. Wyrzykowski;M. Szyma'nski;I. Soszy'nski;K. Ulaczyk;R. Poleski;P. Pietrukowicz;S. Kozłowski;F. Abe;R. Barry;D. Bennett;A. Bhattacharya;M. Donachie;P. Evans;A. Fukui;Y. Hirao;Y. Itow;K. Kawasaki;N. Koshimoto;M. Li;C. Ling;K. Masuda;Y. Matsubara;S. Miyazaki;H. Munakata;Y. Muraki;M. Nagakane;K. Ohnishi;C. Ranc;N. Rattenbury;T. Saito;A. Sharan;D. Sullivan;T. Sumi;D. Suzuki;P. Tristram;T. Yamada;A. Yonehara;R. Street;Y. Tsapras;E. Bachelet;D. Bramich;G. D’ago;M. Dominik;R. Jaimes;K. Horne;M. Hundertmark;N. Kains;J. Menzies;R. Schmidt;C. Snodgrass;I. Steele;J. Wambsganss;R. Pogge;Y. Jung;I. Shin;J. Yee;W. Kim;C. Beichman;S. Carey;S. Novati;W. Zhu
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作者:
A. Udalski;C. Han;V. Bozza;A. Gould;I. Bond;P. Mr'oz;J. Skowron;Ł. Wyrzykowski;M. Szyma'nski;I. Soszy'nski;K. Ulaczyk;R. Poleski;P. Pietrukowicz;S. Kozłowski;F. Abe;R. Barry;D. Bennett;A. Bhattacharya;M. Donachie;P. Evans;A. Fukui;Y. Hirao;Y. Itow;K. Kawasaki;N. Koshimoto;M. Li;C. Ling;K. Masuda;Y. Matsubara;S. Miyazaki;H. Munakata;Y. Muraki;M. Nagakane;K. Ohnishi;C. Ranc;N. Rattenbury;T. Saito;A. Sharan;D. Sullivan;T. Sumi;D. Suzuki;P. Tristram;T. Yamada;A. Yonehara;R. Street;Y. Tsapras;E. Bachelet;D. Bramich;G. D’ago;M. Dominik;R. Jaimes;K. Horne;M. Hundertmark;N. Kains;J. Menzies;R. Schmidt;C. Snodgrass;I. Steele;J. Wambsganss;R. Pogge;Y. Jung;I. Shin;J. Yee;W. Kim;C. Beichman;S. Carey;S. Novati;W. Zhu
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 ⊥ = 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.