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journal contribution
posted on 2025-01-15, 00:59authored byJ Skowron, A Udalski, A Gould, S Dong, LAG Monard, C Han, CR Nelson, J McCormick, D Moorhouse, G Thornley, A Maury, DM Bramich, J Greenhill, S Kozlowski, I Bond, R Poleski, L Wyrzykowski, K Ulaczyk, M Kubiak, MK Szymanski, G Pietrzynski, I Soszynski, BS Gaudi, JC Yee, LW Hung, RW Pogge, DL DePoy, CU Lee, BG Park, W Allen, F Mallia, J Drummond, G Bolt, A Allan, P Browne, N Clay, M Dominik, S Fraser, K Horne, N Kains, C Mottram, C Snodgrass, I Steele, RA Street, Y Tsapras, F Abe, DP Bennett, CS Botzler, D Douchin, M Freeman, A Fukui, K Furusawa, F Hayashi, JB Hearnshaw, S Hosaka, Y Itow, K Kamiya, PM Kilmartin, A Korpela, W Lin, CH Ling, S Makita, K Masuda, Y Matsubara, Y Muraki, T Nagayama, N Miyake, K Nishimoto, K Ohnishi, YC Perrott, N Rattenbury, To Saito, L Skuljan, DJ Sullivan, T Sumi, D Suzuki, WL Sweatman, PJ Tristram, K Wada, PCM Yock, Jean-Philippe BeaulieuJean-Philippe Beaulieu, P Fouque, MD Albrow, V Batista, S Brillant, JAR Caldwell, A Cassan, Andrew ColeAndrew Cole, KH Cook, CH Coutures, S Dieters, D Dominis Prester, J Donatowicz, SR Kane, D Kubas, JB Marquette, R Martin, J Menzies, KC Sahu, J Wambsganss, A Williams, M Zub
We present the first example of binary microlensing for which the parameter measurements can be verified (or contradicted) by future Doppler observations. This test is made possible by a confluence of two relatively unusual circumstances. First, the binary lens is bright enough (I = 15.6) to permit Doppler measurements. Second, we measure not only the usual seven binary-lens parameters, but also the “microlens parallax” (which yields the binary mass) and two components of the instantaneous orbital velocity. Thus, we measure, effectively, six “Kepler+1” parameters (two instantaneous positions, two instantaneous velocities, the binary total mass, and the mass ratio). Since Doppler observations of the brighter binary component determine five Kepler parameters (period, velocity amplitude, eccentricity, phase, and position of periapsis), while the same spectroscopy yields the mass of the primary, the combined Doppler + microlensing observations would be verconstrained by 6 + (5 + 1)−(7 + 1) = 4 degrees of freedom. This makes possible an extremely strong test of the microlensing solution.We also introduce a uniform microlensing notation for single and binary lenses, define conventions, summarize all known microlensing degeneracies, and extend a set of parameters to describe full Keplerian motion of the binary lenses.
History
Publication title
The Astrophysical Journal: An International Review of Astronomy and Astronomical Physics
Volume
738
Issue
1
Article number
87
Number
87
Pagination
1-21
ISSN
0004-637X
Department/School
School of Natural Sciences, Physics
Publisher
Institute of Physics Publishing Inc
Publication status
Published
Place of publication
United States
Rights statement
Copyright 2011 American Astronomical Society
Socio-economic Objectives
280120 Expanding knowledge in the physical sciences