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24 result(s) for "Hamada, Ryusei"
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KMT-2021-BLG-1150Lb: Microlensing planet detected through a densely covered planetary-caustic signal
Recently, there have been reports of various types of degeneracies in the interpretation of planetary signals induced by planetary caustics. In this work, we check whether such degeneracies persist in the case of well-covered signals by analyzing the lensing event KMT-2021-BLG-1150, for which the light curve exhibits a densely and continuously covered short-term anomaly. In order to identify degenerate solutions, we thoroughly investigate the parameter space by conducting dense grid searches for the lensing parameters. We then check the severity of the degeneracy among the identified solutions. We identify a pair of planetary solutions resulting from the well-known inner-outer degeneracy, and find that interpreting the anomaly is not subject to any degeneracy other than the inner-outer degeneracy. The measured parameters of the planet separation (normalized to the Einstein radius) and mass ratio between the lens components are \\((s, q)_{\\rm in}\\sim (1.297, 1.10\\times 10^{-3})\\) for the inner solution and \\((s, q)_{\\rm out}\\sim (1.242, 1.15\\times 10^{-3})\\) for the outer solution. According to a Bayesian estimation, the lens is a planetary system consisting of a planet with a mass \\(M_{\\rm p}=0.88^{+0.38}_{-0.36}~M_{\\rm J}\\) and its host with a mass \\(M_{\\rm h}=0.73^{+0.32}_{-0.30}~M_\\odot\\) lying toward the Galactic center at a distance \\(D_{\\rm L} =3.8^{+1.3}_{-1.2}\\)~kpc. By conducting analyses using mock data sets prepared to mimic those obtained with data gaps and under various observational cadences, it is found that gaps in data can result in various degenerate solutions, while the observational cadence does not pose a serious degeneracy problem as long as the anomaly feature can be delineated.
MOA-2022-BLG-249Lb: Nearby microlensing super-Earth planet detected from high-cadence surveys
We investigate the data collected by the high-cadence microlensing surveys during the 2022 season in search for planetary signals appearing in the light curves of microlensing events. From this search, we find that the lensing event MOA-2022-BLG-249 exhibits a brief positive anomaly that lasted for about 1 day with a maximum deviation of \\(\\sim 0.2\\)~mag from a single-source single-lens model. We analyze the light curve under the two interpretations of the anomaly: one originated by a low-mass companion to the lens (planetary model) and the other originated by a faint companion to the source (binary-source model). It is found that the anomaly is better explained by the planetary model than the binary-source model. We identify two solutions rooted in the inner--outer degeneracy, for both of which the estimated planet-to-host mass ratio, \\(q\\sim 8\\times 10^{-5}\\), is very small. With the constraints provided by the microlens parallax and the lower limit on the Einstein radius, as well as the blend-flux constraint, we find that the lens is a planetary system, in which a super-Earth planet, with a mass \\((4.83\\pm 1.44)~M_\\oplus\\), orbits a low-mass host star, with a mass \\((0.18\\pm 0.05)~M_\\odot\\), lying in the Galactic disk at a distance \\((2.00\\pm 0.42)\\)~kpc. The planet detection demonstrates the elevated microlensing sensitivity of the current high-cadence lensing surveys to low-mass planets.
The Microlensing Event Rate and Optical Depth from MOA-II 9 year Survey toward the Galactic Bulge
We present measurements of the microlensing optical depth and event rate toward the Galactic bulge using the dataset from the 2006--2014 MOA-II survey, which covers 22 bulge fields spanning ~42 deg^2 between -5 deg < l < 10 deg and -7 deg < b < -1 deg. In the central region with |l|<5 deg, we estimate an optical depth of {\\tau} = [1.75+-0.04]*10^-6exp[(0.34+-0.02)(3 deg-|b|)] and an event rate of {\\Gamma} = [16.08+-0.28]*10^-6exp[(0.44+-0.02)(3 deg-|b|)] star^-1 year^-1 using a sample consisting of 3525 microlensing events, with Einstein radius crossing times of tE < 760 days and source star magnitude of IsWe confirm our results are consistent with the latest measurements from OGLE-IV 8 year dataset (Mróz et al. 2019). We find our result is inconsistent with a prediction based on Galactic models, especially in the central region with |b|<3 deg. These results can be used to improve the Galactic bulge model, and more central regions can be further elucidated by future microlensing experiments, such as The PRime-focus Infrared Microlensing Experiment (PRIME) and Nancy Grace Roman Space Telescope.
Microlensing brown-dwarf companions in binaries detected during the 2022 and 2023 seasons
Building on previous works to construct a homogeneous sample of brown dwarfs in binary systems, we investigate microlensing events detected by the Korea Microlensing Telescope Network (KMTNet) survey during the 2022 and 2023 seasons. Given the difficulty in distinguishing brown-dwarf events from those produced by binary lenses with nearly equal-mass components, we analyze all lensing events detected during the seasons that exhibit anomalies characteristic of binary-lens systems. Using the same criteria consistently applied in previous studies, we identify six additional brown dwarf candidates through the analysis of lensing events KMT-2022-BLG-0412, KMT-2022-BLG-2286, KMT-2023-BLG-0201, KMT-2023-BLG-0601, KMT-2023-BLG-1684, and KMT-2023-BLG-1743. An examination of the mass posteriors shows that the median mass of the lens companions ranges from 0.02 \\(M_\\odot\\) to 0.05 \\(M_\\odot\\), indicating that these companions fall within the brown-dwarf mass range. The mass of the primary lenses ranges from 0.11 \\(M_\\odot\\) to 0.68 \\(M_\\odot\\), indicating that they are low-mass stars with substantially lower masses compared to the Sun.
Four microlensing giant planets detected through signals produced by minor-image perturbations
We investigated the nature of the anomalies appearing in four microlensing events KMT-2020-BLG-0757, KMT-2022-BLG-0732, KMT-2022-BLG-1787, and KMT-2022-BLG-1852. The light curves of these events commonly exhibit initial bumps followed by subsequent troughs that extend across a substantial portion of the light curves. We performed thorough modeling of the anomalies to elucidate their characteristics. Despite their prolonged durations, which differ from the usual brief anomalies observed in typical planetary events, our analysis revealed that each anomaly in these events originated from a planetary companion located within the Einstein ring of the primary star. It was found that the initial bump arouse when the source star crossed one of the planetary caustics, while the subsequent trough feature occurred as the source traversed the region of minor image perturbations lying between the pair of planetary caustics. The estimated masses of the host and planet, their mass ratios, and the distance to the discovered planetary systems are \\((M_{\\rm host}/M_\\odot, M_{\\rm planet}/M_{\\rm J}, q/10^{-3}, \\dl/{\\rm kpc}) = (0.58^{+0.33}_{-0.30}, 10.71^{+6.17}_{-5.61}, 17.61\\pm 2.25,6.67^{+0.93}_{-1.30})\\) for KMT-2020-BLG-0757, \\((0.53^{+0.31}_{-0.31}, 1.12^{+0.65}_{-0.65}, 2.01 \\pm 0.07, 6.66^{+1.19}_{-1.84})\\) for KMT-2022-BLG-0732, \\((0.42^{+0.32}_{-0.23}, 6.64^{+4.98}_{-3.64}, 15.07\\pm 0.86, 7.55^{+0.89}_{-1.30})\\) for KMT-2022-BLG-1787, and \\((0.32^{+0.34}_{-0.19}, 4.98^{+5.42}_{-2.94}, 8.74\\pm 0.49, 6.27^{+0.90}_{-1.15})\\) for KMT-2022-BLG-1852. These parameters indicate that all the planets are giants with masses exceeding the mass of Jupiter in our solar system and the hosts are low-mass stars with masses substantially less massive than the Sun.
Free-Floating planet Mass Function from MOA-II 9-year survey towards the Galactic Bulge
We present the first measurement of the mass function of free-floating planets (FFP) or very wide orbit planets down to an Earth mass, from the MOA-II microlensing survey in 2006-2014. Six events are likely to be due to planets with Einstein radius crossing times, \\(t_{\\rm E}<0.5\\)days, and the shortest has \\(t_{\\rm E} = 0.057\\pm 0.016\\)days and an angular Einstein radius of \\(\\theta_{\\rm E} = 0.90\\pm 0.14\\mu\\)as. We measure the detection efficiency depending on both \\(t_{\\rm E}\\) and \\(\\theta_{\\rm E}\\) with image level simulations for the first time. These short events are well modeled by a power-law mass function, \\(dN_4/d\\log M = (2.18^{+0.52}_{-1.40})\\times (M/8\\,M_\\oplus)^{-\\alpha_4}\\) dex\\(^{-1}\\)star\\(^{-1}\\) with \\(\\alpha_4 = 0.96^{+0.47}_{-0.27}\\) for \\(M/M_\\odot < 0.02\\). This implies a total of \\(f= 21^{+23}_{-13}\\) FFP or very wide orbit planets of mass \\(0.33
KMT-2023-BLG-1866Lb: Microlensing super-Earth around an M dwarf host
We investigate the nature of the short-term anomaly that appears in the lensing light curve of KMT-2023-BLG-1866. The anomaly was only partly covered due to its short duration, less than a day, coupled with cloudy weather conditions and restricted nighttime duration. Considering intricacy of interpreting partially covered signals, we thoroughly explore all potential degenerate solutions. Through this process, we identify three planetary scenarios that equally well account for the observed anomaly. These scenarios are characterized by the specific planetary parameters: \\((s, q)_{\\rm inner} = [0.9740 \\pm 0.0083, (2.46 \\pm 1.07) \\times 10^{-5}]\\), \\((s, q)_{\\rm intermediate} = [0.9779 \\pm 0.0017, (1.56 \\pm 0.25)\\times 10^{-5}]\\), and \\((s, q)_{\\rm outer} = [0.9894 \\pm 0.0107, (2.31 \\pm 1.29)\\times 10^{-5}]\\), where \\(s\\) and \\(q\\) denote the projected separation (scaled to the Einstein radius) and mass ratio between the planet and its host, respectively. We identify that the ambiguity between the inner and outer solutions stems from the inner-outer degeneracy, while the similarity between the intermediate solution and the others is due to an accidental degeneracy caused by incomplete anomaly coverage. Through Bayesian analysis utilizing the constraints derived from measured lensing observables and blending flux, our estimation indicates that the lens system comprises a very low-mass planet orbiting an early M-type star situated approximately (6.2 -- 6.5)~kpc from Earth in terms of median posterior values for the different solutions. The median mass of the planet host is in the range of (0.48 -- 0.51)~\\(M_\\odot\\), and that of the planet's mass spans a range of (2.6 -- 4.0)~\\(M_{\\rm E}\\), varying across different solutions. The detection of KMT-2023-BLG-1866Lb signifies the extension of the lensing surveys to very low-mass planets that have been difficult to be detected from earlier surveys.
Terrestrial and Neptune mass free-floating planet candidates from the MOA-II 9-year Galactic Bulge survey
We report the discoveries of low-mass free-floating planet (FFP) candidates from the analysis of 2006-2014 MOA-II Galactic bulge survey data. In this dataset, we found 6,111 microlensing candidates and identified a statistical sample consisting of 3,535 high quality single lens events with Einstein radius crossing times in the range \\(0.057 < t_{\\rm E}/{\\rm days} < 757\\), including 13 events that show clear finite source effects with angular Einstein radii of \\(0.90<\\theta_{\\rm E}/{\\rm \\mu as} <332.54\\). Two of the 12 events with \\(t_{\\rm E} < 1\\) day have significant finite source effects, and one event, MOA-9y-5919, with \\(t_{\\rm E}=0.057\\pm 0.016\\) days and \\(\\theta_{\\rm E}= 0.90 \\pm 0.14\\) \\(\\mu\\)as, is the second terrestrial mass FFP candidate to date. A Bayesian analysis indicates a lens mass of \\(0.75^{+1.23}_{-0.46}\\) \\(M_\\oplus\\) for this event. The low detection efficiency for short duration events implies a large population of low-mass FFPs. The microlensing detection efficiency for low-mass planet events depends on both the Einstein radius crossing times and the angular Einstein radii, so we have used image-level simulations to determine the detection efficiency dependence on both \\(t_{\\rm E}\\) and \\(\\theta_{\\rm E}\\). This allows us to use a Galactic model to simulate the \\(t_{\\rm E}\\) and \\(\\theta_{\\rm E}\\) distribution of events produced by the known stellar populations and models of the FFP distribution that are fit to the data. Methods like this will be needed for the more precise FFP demographics determinations from Nancy Grace Roman Space Telescope data.
KMT-2021-BLG-0284, KMT-2022-BLG-2480, and KMT-2024-BLG-0412: Three microlensing events involving two lens masses and two source stars
We carried out a project involving the systematic analysis of microlensing data from the Korea Microlensing Telescope Network survey. The aim of this project is to identify lensing events with complex anomaly features that are difficult to explain using standard binary-lens or binary-source models. Our investigation reveals that the light curves of microlensing events KMT-2021-BLG-0284, KMT-2022-BLG-2480, and KMT-2024-BLG-0412 display highly complex patterns with three or more anomaly features. These features cannot be adequately explained by a binary-lens (2L1S) model alone. However, the 2L1S model can effectively describe certain segments of the light curve. By incorporating an additional source into the modeling, we identified a comprehensive model that accounts for all the observed anomaly features. Bayesian analysis, based on constraints provided by lensing observables, indicates that the lenses of KMT-2021-BLG-0284 and KMT-2024-BLG-0412 are binary systems composed of M dwarfs. For KMT-2022-BLG-2480, the primary lens is an early K-type main-sequence star with an M dwarf companion. The lenses of KMT-2021-BLG-0284 and KMT-2024-BLG-0412 are likely located in the bulge, whereas the lens of KMT-2022-BLG-2480 is more likely situated in the disk. In all events, the binary stars of the sources have similar magnitudes due to a detection bias favoring binary source events with a relatively bright secondary source star, which increases detection efficiency.
OGLE-2014-BLG-0221Lb: A Jupiter Mass Ratio Companion Orbiting either a Late-Type Star or a Stellar Remnant
We present the analysis of microlensing event OGLE-2014-BLG-0221, a planetary candidate event discovered in 2014. The photometric light curve is best described by a binary-lens single-source model. Our light curve modeling finds two degenerate models, with event timescales of \\(t_\\mathrm{E}\\sim70\\) days and \\(\\sim110\\) days. These timescales are relatively long, indicating that the discovered system would possess a substantial mass. The two models are similar in their planetary parameters with a Jupiter mass ratio of \\(q \\sim 10^{-3}\\) and a separation of \\(s \\sim 1.1\\). While the shorter timescale model shows marginal detection of a microlensing parallax signal, the longer timescale model requires a higher order effect of microlensing parallax, lens orbital motion or xallarap to explain the deviation in the light curve. However, the modeling shows significant correlation between the higher order effects and suffers the ecliptic degeneracy that results in a failure to determine the parallax parameters. Bayesian inference is used to estimate the physical parameters of the lens, revealing the lens to be either a late-type star supported by the shorter timescale model or a stellar remnant supported by the longer timescale model. If the lens is a remnant, this would be the second planet found by microlensing around a stellar remnant. Since the models predict different values for relative proper motion and source flux, future high angular resolution follow-up observations (e.g. Keck adaptive optics) are required to rule out either of the models.