KMT-2018-BLG-1743: planetary microlensing event occurring on two source stars

Aims. We present the analysis of the microlensing event KMT-2018-BLG-1743. The analysis was conducted as a part of the project, in which previous lensing events detected in and before the 2019 season by the KMTNet survey were reinvestigated with the aim of finding solutions of anomalous events with...

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Veröffentlicht in:Astronomy and astrophysics (Berlin) 2021-08, Vol.652, p.A145
Hauptverfasser: Han, Cheongho, Albrow, Michael D., Chung, Sun-Ju, Gould, Andrew, Hwang, Kyu-Ha, Jung, Youn Kil, Kim, Doeon, Kim, Hyoun-Woo, Lee, Chung-Uk, Ryu, Yoon-Hyun, Shin, In-Gu, Shvartzvald, Yossi, Yee, Jennifer C., Zang, Weicheng, Cha, Sang-Mok, Kim, Dong-Jin, Kim, Seung-Lee, Lee, Dong-Joo, Lee, Yongseok, Park, Byeong-Gon, Pogge, Richard W.
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container_start_page A145
container_title Astronomy and astrophysics (Berlin)
container_volume 652
creator Han, Cheongho
Albrow, Michael D.
Chung, Sun-Ju
Gould, Andrew
Hwang, Kyu-Ha
Jung, Youn Kil
Kim, Doeon
Kim, Hyoun-Woo
Lee, Chung-Uk
Ryu, Yoon-Hyun
Shin, In-Gu
Shvartzvald, Yossi
Yee, Jennifer C.
Zang, Weicheng
Cha, Sang-Mok
Kim, Dong-Jin
Kim, Seung-Lee
Lee, Dong-Joo
Lee, Yongseok
Park, Byeong-Gon
Pogge, Richard W.
description Aims. We present the analysis of the microlensing event KMT-2018-BLG-1743. The analysis was conducted as a part of the project, in which previous lensing events detected in and before the 2019 season by the KMTNet survey were reinvestigated with the aim of finding solutions of anomalous events with no suggested plausible models. Methods. The light curve of the event, with a peak magnification A peak ~ 800, exhibits two anomaly features, one around the peak and the other on the falling side of the light curve. An interpretation with a binary lens and a single source (2L1S) cannot describe the anomalies. By conducting additional modeling that includes an extra lens (3L1S) or an extra source (2L2S) relative to a 2L1S interpretation, we find that 2L2S interpretations with a planetary lens system and a binary source best explain the observed light curve with Δ χ 2 ~ 188 and ~91 over the 2L1S and 3L1S solutions, respectively. Assuming that these Δ χ 2 values are adequate for distinguishing the models, the event is the fourth 2L2S event and the second 2L2S planetary event. The 2L2S interpretations are subject to a degeneracy, resulting in two solutions with s > 1.0 (wide solution) and s < 1.0 (close solution). Results. The masses of the lens components and the distance to the lens are ( M host / M ⊙ , M planet / M J , D L /kpc)~(0.19 −0.111 +0.27 ,0.25 −0.14 +0.34 ,6.48 −1.03 +0.94 ) and ~(0.42 −0.25 +0.34 ,1.61 −0.97 +1.30 ,6.04 −1.27 +0.93 ) according to the wide and close solutions, respectively. The source is a binary composed of an early G dwarf and a mid M dwarf. The values of the relative lens-source proper motion expected from the two degenerate solutions, μ wide ~ 2.3 mas yr −1 and μ close ~ 4.1 mas yr −1 , are substantially different, and thus the degeneracy can be broken by resolving the lens and source from future high-resolution imaging observations.
doi_str_mv 10.1051/0004-6361/202140923
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We present the analysis of the microlensing event KMT-2018-BLG-1743. The analysis was conducted as a part of the project, in which previous lensing events detected in and before the 2019 season by the KMTNet survey were reinvestigated with the aim of finding solutions of anomalous events with no suggested plausible models. Methods. The light curve of the event, with a peak magnification A peak ~ 800, exhibits two anomaly features, one around the peak and the other on the falling side of the light curve. An interpretation with a binary lens and a single source (2L1S) cannot describe the anomalies. By conducting additional modeling that includes an extra lens (3L1S) or an extra source (2L2S) relative to a 2L1S interpretation, we find that 2L2S interpretations with a planetary lens system and a binary source best explain the observed light curve with Δ χ 2 ~ 188 and ~91 over the 2L1S and 3L1S solutions, respectively. Assuming that these Δ χ 2 values are adequate for distinguishing the models, the event is the fourth 2L2S event and the second 2L2S planetary event. The 2L2S interpretations are subject to a degeneracy, resulting in two solutions with s &gt; 1.0 (wide solution) and s &lt; 1.0 (close solution). Results. The masses of the lens components and the distance to the lens are ( M host / M ⊙ , M planet / M J , D L /kpc)~(0.19 −0.111 +0.27 ,0.25 −0.14 +0.34 ,6.48 −1.03 +0.94 ) and ~(0.42 −0.25 +0.34 ,1.61 −0.97 +1.30 ,6.04 −1.27 +0.93 ) according to the wide and close solutions, respectively. The source is a binary composed of an early G dwarf and a mid M dwarf. The values of the relative lens-source proper motion expected from the two degenerate solutions, μ wide ~ 2.3 mas yr −1 and μ close ~ 4.1 mas yr −1 , are substantially different, and thus the degeneracy can be broken by resolving the lens and source from future high-resolution imaging observations.</description><identifier>ISSN: 0004-6361</identifier><identifier>EISSN: 1432-0746</identifier><identifier>DOI: 10.1051/0004-6361/202140923</identifier><language>eng</language><publisher>Heidelberg: EDP Sciences</publisher><subject>Anomalies ; Image resolution ; Lenses ; Light curve ; Microlenses</subject><ispartof>Astronomy and astrophysics (Berlin), 2021-08, Vol.652, p.A145</ispartof><rights>Copyright EDP Sciences Aug 2021</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c322t-a1c1535c62f638bedb7896e649d2edd354b9abfc7bd9196e38c5a9dcdbdd7c573</citedby><cites>FETCH-LOGICAL-c322t-a1c1535c62f638bedb7896e649d2edd354b9abfc7bd9196e38c5a9dcdbdd7c573</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,3713,27903,27904</link.rule.ids></links><search><creatorcontrib>Han, Cheongho</creatorcontrib><creatorcontrib>Albrow, Michael D.</creatorcontrib><creatorcontrib>Chung, Sun-Ju</creatorcontrib><creatorcontrib>Gould, Andrew</creatorcontrib><creatorcontrib>Hwang, Kyu-Ha</creatorcontrib><creatorcontrib>Jung, Youn Kil</creatorcontrib><creatorcontrib>Kim, Doeon</creatorcontrib><creatorcontrib>Kim, Hyoun-Woo</creatorcontrib><creatorcontrib>Lee, Chung-Uk</creatorcontrib><creatorcontrib>Ryu, Yoon-Hyun</creatorcontrib><creatorcontrib>Shin, In-Gu</creatorcontrib><creatorcontrib>Shvartzvald, Yossi</creatorcontrib><creatorcontrib>Yee, Jennifer C.</creatorcontrib><creatorcontrib>Zang, Weicheng</creatorcontrib><creatorcontrib>Cha, Sang-Mok</creatorcontrib><creatorcontrib>Kim, Dong-Jin</creatorcontrib><creatorcontrib>Kim, Seung-Lee</creatorcontrib><creatorcontrib>Lee, Dong-Joo</creatorcontrib><creatorcontrib>Lee, Yongseok</creatorcontrib><creatorcontrib>Park, Byeong-Gon</creatorcontrib><creatorcontrib>Pogge, Richard W.</creatorcontrib><title>KMT-2018-BLG-1743: planetary microlensing event occurring on two source stars</title><title>Astronomy and astrophysics (Berlin)</title><description>Aims. We present the analysis of the microlensing event KMT-2018-BLG-1743. The analysis was conducted as a part of the project, in which previous lensing events detected in and before the 2019 season by the KMTNet survey were reinvestigated with the aim of finding solutions of anomalous events with no suggested plausible models. Methods. The light curve of the event, with a peak magnification A peak ~ 800, exhibits two anomaly features, one around the peak and the other on the falling side of the light curve. An interpretation with a binary lens and a single source (2L1S) cannot describe the anomalies. By conducting additional modeling that includes an extra lens (3L1S) or an extra source (2L2S) relative to a 2L1S interpretation, we find that 2L2S interpretations with a planetary lens system and a binary source best explain the observed light curve with Δ χ 2 ~ 188 and ~91 over the 2L1S and 3L1S solutions, respectively. Assuming that these Δ χ 2 values are adequate for distinguishing the models, the event is the fourth 2L2S event and the second 2L2S planetary event. The 2L2S interpretations are subject to a degeneracy, resulting in two solutions with s &gt; 1.0 (wide solution) and s &lt; 1.0 (close solution). Results. The masses of the lens components and the distance to the lens are ( M host / M ⊙ , M planet / M J , D L /kpc)~(0.19 −0.111 +0.27 ,0.25 −0.14 +0.34 ,6.48 −1.03 +0.94 ) and ~(0.42 −0.25 +0.34 ,1.61 −0.97 +1.30 ,6.04 −1.27 +0.93 ) according to the wide and close solutions, respectively. The source is a binary composed of an early G dwarf and a mid M dwarf. 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We present the analysis of the microlensing event KMT-2018-BLG-1743. The analysis was conducted as a part of the project, in which previous lensing events detected in and before the 2019 season by the KMTNet survey were reinvestigated with the aim of finding solutions of anomalous events with no suggested plausible models. Methods. The light curve of the event, with a peak magnification A peak ~ 800, exhibits two anomaly features, one around the peak and the other on the falling side of the light curve. An interpretation with a binary lens and a single source (2L1S) cannot describe the anomalies. By conducting additional modeling that includes an extra lens (3L1S) or an extra source (2L2S) relative to a 2L1S interpretation, we find that 2L2S interpretations with a planetary lens system and a binary source best explain the observed light curve with Δ χ 2 ~ 188 and ~91 over the 2L1S and 3L1S solutions, respectively. Assuming that these Δ χ 2 values are adequate for distinguishing the models, the event is the fourth 2L2S event and the second 2L2S planetary event. The 2L2S interpretations are subject to a degeneracy, resulting in two solutions with s &gt; 1.0 (wide solution) and s &lt; 1.0 (close solution). Results. The masses of the lens components and the distance to the lens are ( M host / M ⊙ , M planet / M J , D L /kpc)~(0.19 −0.111 +0.27 ,0.25 −0.14 +0.34 ,6.48 −1.03 +0.94 ) and ~(0.42 −0.25 +0.34 ,1.61 −0.97 +1.30 ,6.04 −1.27 +0.93 ) according to the wide and close solutions, respectively. The source is a binary composed of an early G dwarf and a mid M dwarf. The values of the relative lens-source proper motion expected from the two degenerate solutions, μ wide ~ 2.3 mas yr −1 and μ close ~ 4.1 mas yr −1 , are substantially different, and thus the degeneracy can be broken by resolving the lens and source from future high-resolution imaging observations.</abstract><cop>Heidelberg</cop><pub>EDP Sciences</pub><doi>10.1051/0004-6361/202140923</doi><oa>free_for_read</oa></addata></record>
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subjects Anomalies
Image resolution
Lenses
Light curve
Microlenses
title KMT-2018-BLG-1743: planetary microlensing event occurring on two source stars
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