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Author

T. Yamada

Other affiliations: Osaka University
Bio: T. Yamada is an academic researcher from Kyoto Sangyo University. The author has contributed to research in topics: Gravitational microlensing & Light curve. The author has an hindex of 10, co-authored 13 publications receiving 244 citations. Previous affiliations of T. Yamada include Osaka University.

Papers
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Journal ArticleDOI
TL;DR: In this article, the authors reported the discovery of a microlensing planet, MOA-2016-BLG-227Lb, with a large planet/host mass ratio of q ≃ 9 × 10^(−3).
Abstract: We report the discovery of a microlensing planet—MOA-2016-BLG-227Lb—with a large planet/host mass ratio of q ≃ 9 × 10^(−3). This event was located near the K2 Campaign 9 field that was observed by a large number of telescopes. As a result, the event was in the microlensing survey area of a number of these telescopes, and this enabled good coverage of the planetary light-curve signal. High angular resolution adaptive optics images from the Keck telescope reveal excess flux at the position of the source above the flux of the source star, as indicated by the light-curve model. This excess flux could be due to the lens star, but it could also be due to a companion to the source or lens star, or even an unrelated star. We consider all these possibilities in a Bayesian analysis in the context of a standard Galactic model. Our analysis indicates that it is unlikely that a large fraction of the excess flux comes from the lens, unless solar-type stars are much more likely to host planets of this mass ratio than lower mass stars. We recommend that a method similar to the one developed in this paper be used for other events with high angular resolution follow-up observations when the follow-up observations are insufficient to measure the lens–source relative proper motion.

49 citations

Journal ArticleDOI
Yoon-Hyun Ryu1, Jennifer C. Yee2, Andrzej Udalski3, Ian A. Bond4, Yossi Shvartzvald5, Weicheng Zang6, Weicheng Zang7, R. Figuera Jaimes8, R. Figuera Jaimes9, U. G. Jørgensen10, Wei Zhu11, Chelsea X. Huang12, Chelsea X. Huang13, Y. K. Jung2, Michael D. Albrow14, S. J. Chung15, S. J. Chung1, Andrew Gould16, Andrew Gould11, Andrew Gould1, Chang S. Han17, Kyu-Ha Hwang1, I.-G. Shin2, Sang-Mok Cha18, Sang-Mok Cha1, D.-J. Kim1, Hyoun-Woo Kim1, Shinyoung Kim1, Shinyoung Kim15, C.-U. Lee1, C.-U. Lee15, Dong-Joo Lee1, Yongseok Lee18, Yongseok Lee1, Byeong-Gon Park1, Byeong-Gon Park15, Richard W. Pogge11, S. Calchi Novati5, S. Calchi Novati19, Sean Carey5, Calen B. Henderson5, C. A. Beichman5, B. S. Gaudi11, P. Mróz3, Radosław Poleski3, Radosław Poleski11, Jan Skowron3, Michał K. Szymański3, Igor Soszyński3, S. Kozlowski3, P. Pietrukowicz3, Krzysztof Ulaczyk3, M. Pawlak3, Fumio Abe20, Yuichiro Asakura20, Richard K. Barry21, David P. Bennett21, A. Bhattacharya20, Martin Donachie22, Phil Evans22, Akihiko Fukui, Yuki Hirao23, Yoshitaka Itow20, Kohei Kawasaki23, Naoki Koshimoto23, Man Cheung Alex Li22, C. H. Ling4, Kimiaki Masuda20, Yutaka Matsubara20, Shota Miyazaki23, Yasushi Muraki20, Masayuki Nagakane23, Kouji Ohnishi, Clément Ranc21, Nicholas J. Rattenbury22, To. Saito24, A. Sharan22, Denis J. Sullivan25, Takahiro Sumi23, Daisuke Suzuki26, Daisuke Suzuki21, Paul J. Tristram14, T. Yamada27, Atsunori Yonehara27, G. Bryden5, Steve B. Howell28, Savannah Jacklin29, Matthew T. Penny11, Shude Mao30, Shude Mao7, Shude Mao31, Pascal Fouqué32, Tianshu Wang7, Rachel Street33, Yiannis Tsapras34, M. Hundertmark34, M. Hundertmark10, Etienne Bachelet33, Martin Dominik8, Z. Li33, Simon Cross33, Arnaud Cassan35, Keith Horne8, R. W. Schmidt34, Joachim Wambsganss34, S. K. Ment34, D. Maoz36, Colin Snodgrass37, Iain A. Steele38, Valerio Bozza19, Valerio Bozza39, Martin Burgdorf40, Simona Ciceri41, Giuseppe D'Ago42, Daniel F. Evans43, Tobias C. Hinse1, Eamonn Kerins31, Rosita Kokotanekova16, Rosita Kokotanekova37, P. Longa44, J. MacKenzie10, A. Popovas10, Markus Rabus45, Sohrab Rahvar46, Sedighe Sajadian47, Jesper Skottfelt37, John Southworth43, C. von Essen48 
TL;DR: The OGLE-2016-BLG-1190Lb is the first Spitzer microlensing planet in the Galactic bulge/bar, an assignation that can be confirmed by two epochs of high-resolution imaging of the combined source-lens baseline object as discussed by the authors.
Abstract: We report the discovery of OGLE-2016-BLG-1190Lb, which is likely to be the first Spitzer microlensing planet in the Galactic bulge/bar, an assignation that can be confirmed by two epochs of high-resolution imaging of the combined source–lens baseline object. The planet's mass, M p = 13.4 ± 0.9 M J , places it right at the deuterium-burning limit, i.e., the conventional boundary between "planets" and "brown dwarfs." Its existence raises the question of whether such objects are really "planets" (formed within the disks of their hosts) or "failed stars" (low-mass objects formed by gas fragmentation). This question may ultimately be addressed by comparing disk and bulge/bar planets, which is a goal of the Spitzer microlens program. The host is a G dwarf, M host = 0.89 ± 0.07 M ⊙, and the planet has a semimajor axis a ~ 2.0 au. We use Kepler K2 Campaign 9 microlensing data to break the lens-mass degeneracy that generically impacts parallax solutions from Earth–Spitzer observations alone, which is the first successful application of this approach. The microlensing data, derived primarily from near-continuous, ultradense survey observations from OGLE, MOA, and three KMTNet telescopes, contain more orbital information than for any previous microlensing planet, but not quite enough to accurately specify the full orbit. However, these data do permit the first rigorous test of microlensing orbital-motion measurements, which are typically derived from data taken over <1% of an orbital period.

39 citations

Journal ArticleDOI
TL;DR: In this paper, the authors present the result of microlensing event MOA-2016-BLG-290, which received observations from the two-wheel Kepler (K2), Spitzer, as well as ground-based observatories.
Abstract: We present the result of microlensing event MOA-2016-BLG-290, which received observations from the two-wheel Kepler (K2), Spitzer, as well as ground-based observatories. A joint analysis of data from K2 and the ground leads to two degenerate solutions of the lens mass and distance. This degeneracy is effectively broken once the (partial) Spitzer light curve is included. Altogether, the lens is found to be an extremely low-mass star or brown dwarf (77^(+34)_(-23) M_J) located in the Galactic bulge (6.8 ± 0.4 kpc). MOA-2016-BLG-290 is the first microlensing event for which we have signals from three well-separated (~1 au) locations. It demonstrates the power of two-satellite microlensing experiment in reducing the ambiguity of lens properties, as pointed out independently by S. Refsdal and A. Gould several decades ago.

31 citations

Journal ArticleDOI
TL;DR: The OGLE project has received funding from the National Science Centre, Poland, grant MAESTRO 2014/14/A/ST9/00121 to AU as discussed by the authors, and the data were obtained at three host sites of CTIO in Chile, SAAO in South Africa, and SSO in Australia.
Abstract: Work by K.H.H. was support by KASI grant 2017-1-830-03. Work by W.Z., Y.K.J., and A.G. were supported by AST-1516842 from the US NSF. W.Z., I.G.S., and A.G. were supported by JPL grant 1500811. This research has made use of the KMTNet system operated by the Korea Astronomy and Space Science Institute (KASI) and the data were obtained at three host sites of CTIO in Chile, SAAO in South Africa, and SSO in Australia. Work by C.H. was supported by the grant (2017R1A4A101517) of National Research Foundation of Korea. The OGLE Team thanks Prof. G. Pietrzynski for his contribution to the collection of the OGLE photometric data. The OGLE project has received funding from the National Science Centre, Poland, grant MAESTRO 2014/14/A/ST9/00121 to AU. The MOA project is supported by JSPS KAKENHI Grant Number JSPS24253004, JSPS26247023, JSPS23340064, JSPS15H00781, and JP16H06287.

30 citations

Journal ArticleDOI
Akihiko Fukui1, Akihiko Fukui2, Daisuke Suzuki3, Naoki Koshimoto4, Naoki Koshimoto1, Etienne Bachelet5, Tonny Vanmunster, D. Storey6, Hiroyuki Maehara7, Kenshi Yanagisawa, T. Yamada8, Atsunori Yonehara8, Teruyuki Hirano9, David P. Bennett10, David P. Bennett4, Valerio Bozza11, Valerio Bozza12, D. Mawet13, Matthew T. Penny14, Supachai Awiphan15, A. Oksanen6, T. M. Heintz16, T. M. Heintz17, Thomas E. Oberst17, Víctor J. S. Béjar2, Víctor J. S. Béjar18, Núria Casasayas-Barris2, Núria Casasayas-Barris18, Guo Chen2, Guo Chen19, N. Crouzet2, N. Crouzet18, N. Crouzet20, D. Hidalgo18, D. Hidalgo2, Peter Klagyivik18, Peter Klagyivik2, Felipe Murgas18, Felipe Murgas2, Norio Narita, Enric Palle2, Enric Palle18, Hannu Parviainen18, Hannu Parviainen2, Noriharu Watanabe21, N. Kusakabe22, Mayuko Mori1, Yuka Terada1, J. P. de Leon1, Andrés Felipe Valencia Hernández2, Andrés Felipe Valencia Hernández18, Rafael Luque18, Rafael Luque2, Matteo Monelli18, Matteo Monelli2, Pilar Montañés-Rodríguez2, Pilar Montañés-Rodríguez18, Jorge Prieto-Arranz2, Jorge Prieto-Arranz18, K. L. Murata9, S. Shugarov23, S. Shugarov24, Y. Kubota8, C. Otsuki8, A. Shionoya8, Taku Nishiumi8, A. Nishide8, Misato Fukagawa, K. Onodera, S. Villanueva25, Rachel Street5, Yiannis Tsapras26, M. Hundertmark26, Masayuki Kuzuhara22, M. Fujita9, C. A. Beichman13, C. A. Beichman27, J.-P. Beaulieu28, J.-P. Beaulieu29, Roi Alonso18, Roi Alonso2, Daniel E. Reichart30, Nobuyuki Kawai9, Motohide Tamura22, Motohide Tamura1 
TL;DR: In this article, Nucita et al. reported the analysis of additional multiband photometry and spectroscopy and new adaptive optics (AO) imaging of the nearby planetary microlensing event TCP J05074264+2447555 (Kojima-1), which was discovered toward the Galactic anticenter in 2017.
Abstract: We report the analysis of additional multiband photometry and spectroscopy and new adaptive optics (AO) imaging of the nearby planetary microlensing event TCP J05074264+2447555 (Kojima-1), which was discovered toward the Galactic anticenter in 2017 (Nucita et al.). We confirm the planetary nature of the light-curve anomaly around the peak while finding no additional planetary feature in this event. We also confirm the presence of apparent blending flux and the absence of significant parallax signal reported in the literature. The AO image reveals no contaminating sources, making it most likely that the blending flux comes from the lens star. The measured multiband lens flux, combined with a constraint from the microlensing model, allows us to narrow down the previously unresolved mass and distance of the lens system. We find that the primary lens is a dwarf on the K/M boundary (0.581 ± 0.033 M⊙) located at 505 ± 47 pc, and the companion (Kojima-1Lb) is a Neptune-mass planet (20.0 ± 2.0 M⊕) with a semimajor axis of 1.08^(+0.62)_(-0.18) au. This orbit is a few times smaller than those of typical microlensing planets and is comparable to the snow-line location at young ages. We calculate that the a priori detection probability of Kojima-1Lb is only ~35%, which may imply that Neptunes are common around the snow line, as recently suggested by the transit and radial velocity techniques. The host star is the brightest among the microlensing planetary systems (K_s = 13.7), offering a great opportunity to spectroscopically characterize this system, even with current facilities.

19 citations


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Journal ArticleDOI
TL;DR: In this paper, it was shown that Earth mass planets orbiting stars in the Galactic disk and bulge can be detected by monitoring microlensed stars in a Galactic bulge, and that the planetary signal remains detectable for planetary masses as small as an Earth mass when realistic source star sizes are included in the lightcurve calculation.
Abstract: We show that Earth mass planets orbiting stars in the Galactic disk and bulge can be detected by monitoring microlensed stars in the Galactic bulge. The star and its planet act as a binary lens which generates a lightcurve which can differ substantially from the lightcurve due only to the star itself. We show that the planetary signal remains detectable for planetary masses as small as an Earth mass when realistic source star sizes are included in the lightcurve calculation. These planets are detectable if they reside in the ``lensing zone" which is centered between 1 and 4 AU from the lensing star and spans about a factor of 2 in distance. If we require a minimum deviation of 4\% from the standard point-lens microlensing lightcurve, then we find that more than 2\% of all $\mearth$ planets and 10\% of all $10\mearth$ in the lensing zone can be detected. If a third of all lenses have no planets, a third have $1\mearth$ planets and the remaining third have $10\mearth$ planets then we estimate that an aggressive ground based microlensing planet search program could find one earth mass planet and half a dozen $10\mearth$ planets per year.

210 citations

Journal ArticleDOI
TL;DR: In this paper, the Japanese collaboration for gravitational wave electro-magnetic (J-GEM) follow-up observations of SSS17a, an electromagnetic counterpart of GW170817, showed a 2.5mag decline in the z band during the period between 1.7 and 7.7 d after the merger.
Abstract: GW170817 is the first detected gravitational wave source from a neutron star merger. We present the Japanese collaboration for gravitational-wave electro-magnetic (J-GEM) follow-up observations of SSS17a, an electromagnetic counterpart of GW170817. SSS17a shows a 2.5mag decline in the z band during the period between 1.7 and 7.7 d after the merger. Such a rapid decline is not comparable with supernovae light curves at any epoch. The color of SSS17a also evolves rapidly and becomes redder during later epochs: the z - H color has changed by approximately 2.5mag during the period between 0.7 and 7.7 d. The rapid evolutions of both the color and the optical brightness are consistent with the expected properties of a kilonova that is powered by the radioactive decay of newly synthesized r-process nuclei. Kilonova models with Lanthanide elements can reproduce the aforementioned observed properties well, which suggests that r-process nucleosynthesis beyond the second peak takes place in SSS17a. However, the absolute magnitude of SSS17a is brighter than the expected brightness of the kilonova models with an ejectamass of 0.01M(circle dot), which suggests a more intensemass ejection (similar to 0.03M(circle dot)) or possibly an additional energy source.

174 citations

Journal ArticleDOI
TL;DR: The first detected gravitational wave from a neutron star merger was GW170817 as discussed by the authors, which showed a 2.5-mag decline in the $z-H$ band from 1.7 days to 7 days after the merger, which is not comparable with supernovae light curves at any epoch.
Abstract: The first detected gravitational wave from a neutron star merger was GW170817. In this study, we present J-GEM follow-up observations of SSS17a, an electromagnetic counterpart of GW170817. SSS17a shows a 2.5-mag decline in the $z$-band from 1.7 days to 7.7 days after the merger. Such a rapid decline is not comparable with supernovae light curves at any epoch. The color of SSS17a also evolves rapidly and becomes redder for later epochs; the $z-H$ color changed by approximately 2.5 mag in the period of 0.7 days to 7.7 days. The rapid evolution of both the optical brightness and the color are consistent with the expected properties of a kilonova that is powered by the radioactive decay of newly synthesized $r$-process nuclei. Kilonova models with Lanthanide elements can reproduce the aforementioned observed properties well, which suggests that $r$-process nucleosynthesis beyond the second peak takes place in SSS17a. However, the absolute magnitude of SSS17a is brighter than the expected brightness of the kilonova models with the ejecta mass of 0.01 $\Msun$, which suggests a more intense mass ejection ($\sim 0.03 \Msun$) or possibly an additional energy source.

172 citations

Journal ArticleDOI
TL;DR: In this article, the authors used Gaia DR2 data on the distances and proper motions of non-blended sources and recompute the masses of lenses in parallax events.
Abstract: Context. Gravitational microlensing is sensitive to compact-object lenses in the Milky Way, including white dwarfs, neutron stars, or black holes, and could potentially probe a wide range of stellar-remnant masses. However, the mass of the lens can be determined only in very limited cases, due to missing information on both source and lens distances and their proper motions.Aims. Our aim is to improve the mass estimates in the annual parallax microlensing events found in the eight years of OGLE-III observations towards the Galactic Bulge with the use of Gaia Data Release 2 (DR2).Methods. We use Gaia DR2 data on distances and proper motions of non-blended sources and recompute the masses of lenses in parallax events. We also identify new events in that sample which are likely to have dark lenses; the total number of such events is now 18.Results. The derived distribution of masses of dark lenses is consistent with a continuous distribution of stellar-remnant masses. A mass gap between neutron star and black hole masses in the range between 2 and 5 solar masses is not favoured by our data, unless black holes receive natal kicks above 20−80 km s−1 . We present eight candidates for objects with masses within the putative mass gap, including a spectacular multi-peak parallax event with mass of located just at 600 pc. The absence of an observational mass gap between neutron stars and black holes, or conversely the evidence of black hole natal kicks if a mass gap is assumed, can inform future supernova modelling efforts.

82 citations

Journal ArticleDOI
TL;DR: In this article, an analysis of the simultaneous high-resolution images from the Hubble Space Telescope and Keck adaptive optics system of the planetary event OGLE-2012-BLG-0950 was presented.
Abstract: We present the analysis of the simultaneous high-resolution images from the Hubble Space Telescope and Keck adaptive optics system of the planetary event OGLE-2012-BLG-0950 that determine that the system consists of a 0.58 ± 0.04 M_⊕ host star orbited by a 39 ± 8 M_⊕ planet at a projected separation of 2.54 ± 0.23 au. The planetary system is located at a distance of 2.19 ± 0.23 kpc from Earth. This is the second microlens planet beyond the snow line with a mass measured to be in the mass range 20–80 M_⊕. The runaway gas accretion process of the core accretion model predicts fewer planets in this mass range. This is because giant planets are thought to be growing rapidly at these masses, and they rarely complete growth at this mass. So this result suggests that the core accretion theory may need revision. This analysis also demonstrates the techniques that will be used to measure the masses of planets and their host stars by the WFIRST exoplanet microlensing survey: one-dimensional microlensing parallax combined with the separation and brightness measurement of the unresolved source and host stars to yield multiple redundant constraints on the masses and distance of the planetary system.

74 citations