A. Gould’s research while affiliated with The Ohio State University and other places

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Publications (315)


Figure 1. Cumulative distribution of the expected K-band peak magnitudes of events detected by the OGLE EWS in 2023 (blue line). For comparison, the red line shows the cumulative distribution of the K-band magnitudes of the brightest star within 30 ′′ of the event (fringe-tracking star). Only events with tE ≥ 50 day and an adaptive-optics guide star brighter than G = 14 are plotted.
Figure 7. Detection map for possible luminous blends in the VLTI epoch 2 data. The color codes the χ 2 improvement over the model without the blend. The lens is located in the origin of the coordinate system.
Figure 8. Geometry of the event. The gray solid line marks the trajectory of the source in the sky. Open symbols (red square and blue circle) mark the position of the source during the two epochs of VLTI observations, whereas the filled symbols mark the positions of the images of the source. The dashed circle shows the Einstein radius.
Log of VLTI Observations
Best-fit Parameters of the Light Curve Model (u0 > 0) for Individual Data Sets

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Observations of microlensed images with dual-field interferometry: on-sky demonstration and prospects
  • Preprint
  • File available

September 2024

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30 Reads

P. Mroz

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A. Merand

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R. W. Pogge

Interferometric observations of gravitational microlensing events offer an opportunity for precise, efficient, and direct mass and distance measurements of lensing objects, especially those of isolated neutron stars and black holes. However, such observations were previously possible for only a handful of extremely bright events. The recent development of a dual-field interferometer, GRAVITY Wide, has made it possible to reach out to significantly fainter objects, and increase the pool of microlensing events amenable to interferometric observations by two orders of magnitude. Here, we present the first successful observation of a microlensing event with GRAVITY Wide and the resolution of microlensed images in the event OGLE-2023-BLG-0061/KMT-2023-BLG-0496. We measure the angular Einstein radius of the lens with a sub-percent precision, θE=1.280±0.009\theta_{\rm E} = 1.280 \pm 0.009 mas. Combined with the microlensing parallax detected from the event light curve, the mass and distance to the lens are found to be 0.472±0.012M0.472 \pm 0.012 M_{\odot} and 1.81±0.051.81 \pm 0.05 kpc, respectively. We present the procedure for the selection of targets for interferometric observations, and discuss possible systematic effects affecting GRAVITY Wide data. This detection demonstrates the capabilities of the new instrument and it opens up completely new possibilities for the follow-up of microlensing events, and future routine discoveries of isolated neutron stars and black holes.

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Precision measurement of a brown dwarf mass in a binary system in the microlensing event OGLE-2019-BLG-0033/MOA-2019-BLG-035

March 2022

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92 Reads

Context. Brown dwarfs are poorly understood transition objects between stars and planets, with several competing mechanisms having been proposed for their formation. Mass measurements are generally difficult for isolated objects but also for brown dwarfs orbiting low-mass stars, which are often too faint for spectroscopic follow-up. Aims. Microlensing provides an alternative tool for the discovery and investigation of such faint systems. Here we present the analysis of the microlensing event OGLE-2019-BLG-0033/MOA-2019-BLG-035, which is due to a binary system composed of a brown dwarf orbiting a red dwarf. Methods. Thanks to extensive ground observations and the availability of space observations from Spitzer, it has been possible to obtain accurate estimates of all microlensing parameters, including parallax, source radius and orbital motion of the binary lens. Results. After accurate modeling, we find that the lens is composed of a red dwarf with mass M1=0.149±0.010MM_1 = 0.149 \pm 0.010M_\odot and a brown dwarf with mass M2=0.0463±0.0031MM_2 = 0.0463 \pm 0.0031M_\odot, at a projected separation of a=0.585a_\perp = 0.585 au. The system has a peculiar velocity that is typical of old metal-poor populations in the thick disk. Percent precision in the mass measurement of brown dwarfs has been achieved only in a few microlensing events up to now, but will likely become common with the Roman space telescope.


Single-lens mass measurement in the high-magnification microlensing event Gaia19bld located in the Galactic disc

January 2022

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62 Reads

Context. Microlensing provides a unique opportunity to detect non-luminous objects. In the rare cases that the Einstein radius θ_E and microlensing parallax π_E can be measured, it is possible to determine the mass of the lens. With technological advances in both ground- and space-based observatories, astrometric and interferometric measurements are becoming viable, which can lead to the more routine determination of θ_E and, if the microlensing parallax is also measured, the mass of the lens. Aims. We present the photometric analysis of Gaia19bld, a high-magnification (A ≈ 60) microlensing event located in the southern Galactic plane, which exhibited finite source and microlensing parallax effects. Due to a prompt detection by the Gaia satellite and the very high brightness of I = 9.05 mag at the peak, it was possible to collect a complete and unique set of multi-channel follow-up observations, which allowed us to determine all parameters vital for the characterisation of the lens and the source in the microlensing event. Methods. Gaia19bld was discovered by the Gaia satellite and was subsequently intensively followed up with a network of ground-based observatories and the Spitzer Space Telescope. We collected multiple high-resolution spectra with Very Large Telescope (VLT)/X-shooter to characterise the source star. The event was also observed with VLT Interferometer (VLTI)/PIONIER during the peak. Here we focus on the photometric observations and model the light curve composed of data from Gaia, Spitzer, and multiple optical, ground-based observatories. We find the best-fitting solution with parallax and finite source effects. We derived the limit on the luminosity of the lens based on the blended light model and spectroscopic distance. Results. We compute the mass of the lens to be 1.13 ± 0.03 M_⊙ and derive its distance to be 5.52_(−0.64)^(+0.35) kpc. The lens is likely a main sequence star, however its true nature has yet to be verified by future high-resolution observations. Our results are consistent with interferometric measurements of the angular Einstein radius, emphasising that interferometry can be a new channel for determining the masses of objects that would otherwise remain undetectable, including stellar-mass black holes.


MagAO observations of the binary microlens OGLE-2014-BLG-1050 prefer the higher-mass solution

December 2021

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5 Reads

We report adaptive-optics (AO) follow-up imaging of OGLE-2014-BLG-1050, which is the second binary microlensing event with space-based parallax measurements. The degeneracy in microlens parallax pi_E led to two sets of solutions, either a ~(0.9, 0.35) M_Sun binary at ~3.5 kpc, or a ~(0.2, 0.07) M_Sun binary at ~1.1 kpc. We measure the flux blended with the microlensed source by conducting Magellan AO observations, and find that the blending is consistent with the predicted lens flux from the higher-mass solution. From the combination of the AO flux measurement together with previous lensing constraints, it is estimated that} the lens system consists of a 1.050.07+0.081.05^{+0.08}_{-0.07} M_Sun primary and a 0.380.06+0.070.38^{+0.07}_{-0.06} M_Sun secondary at 3.430.21+0.193.43^{+0.19}_{-0.21} kpc.


Fig. 1. Section of the OGLE-IV reference image (2x2 arcmin). The Gaia19bld source is shown as a red cross. It shows the neighbourhood of the star prior to the event; the image is a composition of ten I-band frames taken between 5 Feb 2014 and 30 Jan 2015. North is up; east is to the left.
Fig. 2. Colour-magnitude diagram of the field stars for Gaia19bld event. The grey dots represent stars from the whole OGLE field GD1298.15, while the stars closest to the location of the event (within the 5x5 arcmin box around the target) are highlighted in black. The position of the source is given by the red star.
Photometric data collected for Gaia19bld.
Parameters of the source in the Gaia19bld event determined from spectroscopy. See B21 for more details.
Single-lens mass measurement in the high-magnification microlensing event Gaia19bld located in the Galactic disc

December 2021

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79 Reads

We present the photometric analysis of Gaia19bld, a high-magnification (A60A\approx60) microlensing event located in the southern Galactic plane, which exhibited finite source and microlensing parallax effects. Due to a prompt detection by the Gaia satellite and the very high brightness of I=9.05 I = 9.05~mag at the peak, it was possible to collect a complete and unique set of multi-channel follow-up observations, which allowed us to determine all parameters vital for the characterisation of the lens and the source in the microlensing event. Gaia19bld was discovered by the Gaia satellite and was subsequently intensively followed up with a network of ground-based observatories and the Spitzer Space Telescope. We collected multiple high-resolution spectra with Very Large Telescope (VLT)/X-Shooter to characterise the source star. The event was also observed with VLT Interferometer (VLTI)/PIONIER during the peak. Here we focus on the photometric observations and model the light curve composed of data from Gaia, Spitzer, and multiple optical, ground-based observatories. We find the best-fitting solution with parallax and finite source effects. We derived the limit on the luminosity of the lens based on the blended light model and spectroscopic distance. We compute the mass of the lens to be 1.13±0.03 M1.13 \pm 0.03~M_{\odot} and derive its distance to be 5.520.64+0.35 kpc5.52^{+0.35}_{-0.64}~\mathrm{kpc}. The lens is likely a main sequence star, however its true nature has yet to be verified by future high-resolution observations. Our results are consistent with interferometric measurements of the angular Einstein radius, emphasising that interferometry can be a new channel for determining the masses of objects that would otherwise remain undetectable, including stellar-mass black holes.


Chemical evolution of the Galactic bulge as traced by microlensed dwarf and subgiant stars. VIII. Carbon and oxygen

September 2021

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10 Reads

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11 Citations

Astronomy and Astrophysics

Context. Next to H and He, carbon is, together with oxygen, the most abundant element in the Universe and widely used when modelling the formation and evolution of galaxies and their stellar populations. For the Milky Way bulge, there are currently essentially no measurements of carbon in un-evolved stars, hampering our abilities to properly compare Galactic chemical evolution models to observational data for this still enigmatic stellar population. Aims. We aim to determine carbon abundances for our sample of 91 microlensed dwarf and subgiant stars in the Galactic bulge. Together with new determinations for oxygen this forms the first statistically significant sample of bulge stars that have C and O abundances measured, and for which the C abundances have not been altered by the nuclear burning processes internal to the stars. Methods. Our analysis is based on high-resolution spectra for a sample of 91 dwarf and subgiant stars that were obtained during microlensing events when the brightnesses of the stars were highly magnified. Carbon abundances were determined through spectral line synthesis of six C I lines around 9100 Å, and oxygen abundances using the three O I lines at about 7770 Å. One-dimensional (1D) MARCS model stellar atmospheres calculated under the assumption of local thermodynamic equilibrium (LTE) were used, and non-LTE corrections were applied when calculating the synthetic spectra for both C and O. Results. Carbon abundances was possible to determine for 70 of the 91 stars in the sample and oxygen abundances for 88 of the 91 stars in the sample. The [C/Fe] ratio evolves essentially in lockstep with [Fe/H], centred around solar values at all [Fe/H]. The [O/Fe]–[Fe/H] trend has an appearance very similar to that observed for other α -elements in the bulge, with the exception of a continued decrease in [O/Fe] at super-solar [Fe/H], where other α -elements tend to level out. When dividing the bulge sample into two sub-groups, one younger than 8 Gyr and one older than 8 Gyr, the stars in the two groups follow exactly the elemental abundance trends defined by the solar neighbourhood thin and thick disks, respectively. Comparisons with recent models of Galactic chemical evolution in the [C/O]–[O/H] plane show that the models that best match the data are the ones that have been calculated with the Galactic thin and thick disks in mind. Conclusions. We conclude that carbon, oxygen, and the combination of the two support the idea that the majority of the stars in the Galactic bulge have a secular origin; that is, they are formed from disk material. We cannot exclude that a fraction of stars in the bulge could be classified as a classical bulge population, but it would have to be small. More dedicated and advanced models of the inner region of the Milky Way are needed to make more detailed comparisons to the observations.


Chemical evolution of the Galactic bulge as traced by microlensed dwarf and subgiant stars. VIII. Carbon and oxygen

June 2021

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2 Reads

CONTEXT: [ABRIDGED]. For the Milky Way bulge, there are currently essentially no measurements of carbon in un-evolved stars, hampering our abilities to properly compare Galactic chemical evolution models to observational data for this still enigmatic stellar population. AIMS: We aim to determine carbon abundances for our sample of 91 microlensed bulge dwarf and subgiant stars. Together with new determinations for oxygen this forms the first statistically significant sample of bulge stars that have C and O abundances measured, and for which the C abundances have not been altered by the nuclear burning processes internal to the stars. METHODS: The analysis is based on high-resolution spectra for a sample of 91 dwarf and subgiant stars that were obtained during microlensing events when the brightnesses of the stars were highly magnified. Carbon abundances were determined through spectral line synthesis of five CI lines around 9100 A, and oxygen abundances using the three OI lines at about 7770 A. [ABRIDGED] RESULTS: Carbon abundances was possible to determine for 70 of the 91 stars in the sample and oxygen abundances for 88 of the 91 stars in the sample. The [C/Fe] ratio evolves essentially in lockstep with [Fe/H], centred around solar values at all [Fe/H]. The [O/Fe]-[Fe/H] trend has an appearance very similar to that observed for other alpha-elements in the bulge, [ABRIDGED]. When dividing the bulge sample into two sub-groups, one younger than 8 Gyr and one older than 8 Gyr, the stars in the two groups follow exactly the elemental abundance trends defined by the solar neighbourhood thin and thick disks, respectively. Comparisons with recent models of Galactic chemical evolution in the [C/O]-[O/H] plane shows that the models that best match the data are the ones that have been calculated with the Galactic thin and thick disks in mind. [ABRIDGED] ....


MagAO Observations of the Binary Microlens OGLE-2014-BLG-1050 Prefer the Higher-mass Solution

February 2021

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11 Reads

The Astronomical Journal

We report adaptive optics (AO) follow-up imaging of OGLE-2014-BLG-1050, which is the second binary microlensing event with space-based parallax measurements. The degeneracy in microlens parallax π E led to two sets of solutions, either a ∼ (0.9, 0.35) M ⊙ binary at ∼3.5 kpc or a ∼(0.2, 0.07) M ⊙ binary at ∼1.1 kpc. We measure the flux blended with the microlensed source by conducting Magellan AO observations, and find that the blending is consistent with the predicted lens flux from the higher-mass solution. From the combination of the AO flux measurement together with previous lensing constraints, it is estimated that the lens system consists of a primary and a secondary at kpc.


A terrestrial-mass rogue planet candidate detected in the shortest-timescale microlensing event

September 2020

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25 Reads

Some low-mass planets are expected to be ejected from their parent planetary systems during early stages of planetary system formation. According to planet-formation theories, such as the core accretion theory, typical masses of ejected planets should be between 0.3 and 1.0 MM_{\oplus}. Although in practice such objects do not emit any light, they may be detected using gravitational microlensing via their light-bending gravity. Microlensing events due to terrestrial-mass rogue planets are expected to have extremely small angular Einstein radii (< 1 uas) and extremely short timescales (< 0.1 day). Here, we present the discovery of the shortest-timescale microlensing event, OGLE-2016-BLG-1928, identified to date (tE0.0288 day=41.5mint_{\rm E} \approx 0.0288\ \mathrm{day} = 41.5 \mathrm{min}). Thanks to the detection of finite-source effects in the light curve of the event, we were able to measure the angular Einstein radius of the lens θE=0.842±0.064\theta_{\rm E} = 0.842 \pm 0.064 uas, making the event the most extreme short-timescale microlens discovered to date. Depending on its unknown distance, the lens may be a Mars- to Earth-mass object, with the former possibility favored by the Gaia proper motion measurement of the source. We rule out stellar companions up to the projected distance of 8.0 au from the planet. Our discovery demonstrates that terrestrial-mass free-floating planets can be detected and characterized using microlensing.


A Wide-orbit Exoplanet OGLE-2012-BLG-0838Lb

May 2020

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26 Reads

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5 Citations

The Astronomical Journal

We present the discovery of a planet on a very wide orbit in the microlensing event OGLE-2012-BLG-0838. The signal of the planet is well separated from the main peak of the event and the planet–star projected separation is found to be twice the Einstein ring radius, which corresponds to a projected separation of ≈4 au. Similar planets around low-mass stars are very hard to find using any technique other than microlensing. We discuss microlensing model fitting in detail and discuss the prospects for measuring the mass and distance of the lens system directly.


Citations (70)


... Indeed, one can determine θ E = θ * /ρ, where ρ is the source radius in Einstein units, and θ * the physical source size in µas. The first parameter is derived from the light curve fit, and the latter from available information on the source star color (Bensby et al. 2013) and brightness (Nataf et al. 2013), and empirical color/brightness relations (Kervella et al. 2004). Thus, the lens-source relative proper motion is derived by µ = θ E /t E . ...

Reference:

Finding planets via gravitational microlensing
Chemical evolution of the Galactic bulge as traced by microlensed dwarf and subgiant stars. VIII. Carbon and oxygen
  • Citing Article
  • September 2021

Astronomy and Astrophysics

... Stellar oscillations can be used to derive precise distances by constraining the luminosity, and thus help constrain the properties of planets detected using microlensing. First detections have already been made using OGLE (Figure 4) [36]. Time-domain stellar variability from oscillation and granulation imprinted on microlensing light curves may allow the systematic characterization of lens and source stars in microlensing detections with the Roman GBTDS. ...

OGLE-2017-BLG-1186: first application of asteroseismology and Gaussian processes to microlensing

Monthly Notices of the Royal Astronomical Society

... As also noted in Paper I, the investigation and publication of all by-eye discoveries serves as an important check on the AnomalyFinder system. For 2018, two by-eye discoveries were not recovered by AnomalyFinder: OGLE-2018-BLG-0677 (Herrera-Martin et al. 2020), which failed to meet the selection criteria, and KMT-2018-BLG-1996(Han et al. 2021b, which was recovered in the machine phase of AnomalyFinder but was not finally selected by eye. Among the ∼70 previously discovered planets from 2016-2019 that met the selection criteria, KMT-2018-BLG-1996 was one of only two that were not recovered. ...

OGLE-2018-BLG-0677Lb: A Super-Earth Near the Galactic Bulge

The Astronomical Journal

... Although the xallarap effect has been examined in the past (e.g., Bennett et al. 2008;Sumi et al. 2010), few events have been able to eliminate possibilities of systematic errors and clearly identify the xallarap signal. Miyazaki et al. (2020) analyzed the planetary microlensing event OGLE-2013-BLG-0911 and found a significant xallarap signal. They conclude from the fitting parameters that the source companion, OGLE-2013-BLG-0911Sb has a mass M S,C = 0.14 ± 0.02 M e , an orbital period P ξ = 36.7 ± 0.8 days, and a semimajor axis a S = 0.225 ± 0.004 au. ...

OGLE-2013-BLG-0911Lb: A Secondary on the Brown-dwarf Planet Boundary around an M Dwarf

The Astronomical Journal

... Despite the discernment of multiple production sites, the constraints on stellar yields remain inadequate. For instance, observations indicate a potential decrease in Li abundance among cool field main sequence (MS) stars at super-solar metallicities (Delgado Mena et al. 2015;Guiglion et al. 2016;Bensby et al. 2020;Stonkutė et al. 2020). Several studies propose a correlation between the observed decrease in Li abundance and radial migration (Guiglion et al. 2019;Dantas et al. 2022;Zhang et al. 2023). ...

Chemical evolution of the Galactic bulge as trace by microlensed dwarf and subgiant stars. VII. Lithium
  • Citing Article
  • January 2020

Astronomy and Astrophysics

... We also check the 2L1S/1L2S degeneracy (Gaudi 1998), which Shin et al. (2019) demonstrated can exist in a wider range of cases than those presented in Gaudi (1998). This is especially true for light curves that are sparsely covered. ...

The 2L1S/1L2S Degeneracy for Two Microlensing Planet Candidates Discovered by the KMTNet Survey in 2017

The Astronomical Journal

... Microlens parallax π E can also be measured via 'satellite microlens parallax', which is done by observing the same microlensing event from Earth and one or more well-separated ( ∼ AU ) satellite (Refsdal 1966 ;Gould 1994Gould , 1995. The feasibility of satellite microlens parallax measurements has been demonstrated by the Spitzer satellite telescope (Dong et al. 2007 ;Calchi Novati et al. 2015a ;Yee et al. 2015a ;Udalski et al. 2015b ;Zhu et al. 2015 ), the two-wheel Kepler satellite telescope (Zhu et al. 2017a ;Zang et al. 2018 ;Poleski et al. 2019 ), the Gaia satellite (Wyrzykowski et al. 2020 ) and the joint observations of Spitzer and Kepler (Zhu et al. 2017c ). Since 2014, the Spitzer satellite observed about 1100 microlensing events and yielded satellite parallax measurements for ten microlens planetary events: OGLE-2014-BLG-0124 (Udalski et al. 2015b ;Beaulieu et al. 2018 ), OGLE-2015-BLG-0966 (Street et al. 2016 ), OGLE-2016-BLG-1067(Calchi Novati et al. 2019, OGLE-2016-BLG-1190(Ryu et al. 2018, OGLE-2016-BLG-1195(Bond et al. 2017Shv artzv ald et al. 2017 ), OGLE-2017-BLG-0406 (Hirao et al. 2020 ), OGLE-2017-BLG-1140(Calchi Novati et al. 2018, OGLE-2018-BLG-0596 (Jung et al. 2019 ), KMT-2018-BLG-0029 (Gould et al. 2020, and Kojima-1 (Nucita et al. 2018 ;Fukui et al. 2019 ;Zang et al. 2020b ). ...

Photometry of K2 Campaign 9 bulge data
  • Citing Article
  • May 2019

Astronomy and Astrophysics

... Zang) identified 133 anomalous events. Of them, 10 were already published using by-eye searches, including six unambiguous planets Shin et al. 2019a;Han et al. 2021Han et al. , 2022, two planet candidates consisting of binary-lens single-source/ single-lens binary-source (2L1S/1L2S; Gaudi 1998) degeneracy (Shin et al. 2019a), and two finite-source point-lens (Gould 1994;Nemiroff & Wickramasinghe 1994;Witt & Mao 1994) events (Shvartzvald et al. 2019;Han et al. 2020). For the remaining events, detailed light-curve analysis shows that 14 are potentially planetary with q online < 0.05, where q online is the mass ratio from a fitting to the online data. ...

Two Jupiter-mass Planets Discovered by the KMTNet Survey in 2017
  • Citing Article
  • March 2019

The Astronomical Journal

... Luo et al. 2015), the Gaia-ESO spectroscopic survey (G. Gilmore et al. 2012), and projects involving next-generation optical and near-infrared (NIR) spectrographs such as the 4 m Multi-Object Spectroscopic Telescope (R. S. de Jong et al. 2012de Jong et al. , 2019, the WHT Enhanced Area Velocity Explorer (G. Dalton et al. 2012), the Multi-Object Optical and Near-Infrared Spectrograph on board ESOʼs Very Large Telescope (W. ...

4MOST: Project overview and information for the First Call for Proposals

... Gravitational lensing has become a powerful probe in many areas of astrophysics and cosmology (Mao & Witt 2012;Medezinski et al. 2013;Fu & Fan 2014;Rahvar 2015;Bartelmann & Maturi 2017;Mandelbaum 2018). The phenomenon has been detected since Walsh et al. (1979) and over a wide range of scales, from megaparsec in the weak-lensing regime (Bacon et al. 2000;Hamana et al. 2003;Castro et al. 2005;Schmidt 2008;Jee et al. 2016;Kilbinger et al. 2017;Troxel et al. 2018) to kiloparsec in strong lensing (Lynds & Petrosian 1986;Soucail et al. 1987, Fort et al. 1988Hewitt 1988;Hudson et al. 1998; Barvainis & Ivison 2002;Oldham et al. 2017;Talbot et al. 2018;Stacey & McKean 2018) and down to parsec and subparsec scales probed by microlensing (Shvartzvald et al. 2017;Bruce et al. 2017;Han et al. 2018). Therefore, gravitational lensing can be used to measure the mass distribution in the universe (Newman et al. 2013;Han et al. 2015;Diego et al. 2018;Jauzac et al. 2018), improve the study of lensed high-redshift galaxies (Coe et al. 2013;Jones et al. 2013;Dye et al. 2015;Stark et al. 2015), and constrain cosmological parameters (Suyu et al. 2013;Liao et al. 2014;Suyu et al. 2014;Magaña et al. 2015), among other applications. ...

OGLE-2017-BLG-0039: Microlensing Event with Light from a Lens Identified from Mass Measurement

The Astrophysical Journal