Abstract
The black hole images obtained with the Event Horizon Telescope (EHT) are expected to be variable at the dynamical timescale near their horizons. For the black hole at the center of the M87 galaxy, this timescale (5-61 days) is comparable to the 6 day extent of the 2017 EHT observations. Closure phases along baseline triangles are robust interferometric observables that are sensitive to the expected structural changes of the images but are free of station-based atmospheric and instrumental errors. We explored the day-to-day variability in closure-phase measurements on all six linearly independent nontrivial baseline triangles that can be formed from the 2017 observations. We showed that three triangles exhibit very low day-to-day variability, with a dispersion of ∼3°-5°. The only triangles that exhibit substantially higher variability (∼90°-180°) are the ones with baselines that cross the visibility amplitude minima on the u-v plane, as expected from theoretical modeling. We used two sets of general relativistic magnetohydrodynamic simulations to explore the dependence of the predicted variability on various black hole and accretion-flow parameters. We found that changing the magnetic field configuration, electron temperature model, or black hole spin has a marginal effect on the model consistency with the observed level of variability. On the other hand, the most discriminating image characteristic of models is the fractional width of the bright ring of emission. Models that best reproduce the observed small level of variability are characterized by thin ring-like images with structures dominated by gravitational lensing effects and thus least affected by turbulence in the accreting plasmas.
Original language | English |
---|---|
Article number | 13 |
Journal | Astrophysical Journal |
Volume | 925 |
Issue number | 1 |
DOIs | |
State | Published - 1 Jan 2022 |
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In: Astrophysical Journal, Vol. 925, No. 1, 13, 01.01.2022.
Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - The Variability of the Black Hole Image in M87 at the Dynamical Timescale
AU - Satapathy, Kaushik
AU - Psaltis, Dimitrios
AU - Özel, Feryal
AU - Medeiros, Lia
AU - Dougall, Sean T.
AU - Chan, Chi Kwan
AU - Wielgus, Maciek
AU - Prather, Ben S.
AU - Wong, George N.
AU - Gammie, Charles F.
AU - Akiyama, Kazunori
AU - Alberdi, Antxon
AU - Alef, Walter
AU - Algaba, Juan Carlos
AU - Anantua, Richard
AU - Asada, Keiichi
AU - Azulay, Rebecca
AU - Baczko, Anne Kathrin
AU - Ball, David
AU - Baloković, Mislav
AU - Barrett, John
AU - Benson, Bradford A.
AU - Bintley, Dan
AU - Blackburn, Lindy
AU - Blundell, Raymond
AU - Boland, Wilfred
AU - Bouman, Katherine L.
AU - Bower, Geoffrey C.
AU - Boyce, Hope
AU - Bremer, Michael
AU - Brinkerink, Christiaan D.
AU - Brissenden, Roger
AU - Britzen, Silke
AU - Broderick, Avery E.
AU - Broguiere, Dominique
AU - Bronzwaer, Thomas
AU - Bustamente, Sandra
AU - Byun, Do Young
AU - Carlstrom, John E.
AU - Chael, Andrew
AU - Chatterjee, Koushik
AU - Chatterjee, Shami
AU - Chen, Ming Tang
AU - Chen, Yongjun
AU - Cho, Ilje
AU - Christian, Pierre
AU - Conway, John E.
AU - Cordes, James M.
AU - Crawford, Thomas M.
AU - Crew, Geoffrey B.
AU - Cruz-Osorio, Alejandro
AU - Cui, Yuzhu
AU - Davelaar, Jordy
AU - De Laurentis, Mariafelicia
AU - Deane, Roger
AU - Dempsey, Jessica
AU - Desvignes, Gregory
AU - Dexter, Jason
AU - Doeleman, Sheperd S.
AU - Eatough, Ralph P.
AU - Falcke, Heino
AU - Farah, Joseph
AU - Fish, Vincent L.
AU - Fomalont, Ed
AU - Ford, H. Alyson
AU - Fraga-Encinas, Raquel
AU - Friberg, Per
AU - Fromm, Christian M.
AU - Fuentes, Antonio
AU - Galison, Peter
AU - García, Roberto
AU - Gentaz, Olivier
AU - Georgiev, Boris
AU - Goddi, Ciriaco
AU - Gold, Roman
AU - Gómez-Ruiz, Arturo I.
AU - Gómez, José L.
AU - Gu, Minfeng
AU - Gurwell, Mark
AU - Hada, Kazuhiro
AU - Haggard, Daryl
AU - Hecht, Michael H.
AU - Hesper, Ronald
AU - Ho, Luis C.
AU - Ho, Paul
AU - Honma, Mareki
AU - Huang, Chih Wei L.
AU - Huang, Lei
AU - Hughes, David H.
AU - Ikeda, Shiro
AU - Inoue, Makoto
AU - Issaoun, Sara
AU - James, David J.
AU - Jannuzi, Buell T.
AU - Janssen, Michael
AU - Jeter, Britton
AU - Jiang, Wu
AU - Jimenez-Rosales, Alejandra
AU - Johnson, Michael D.
AU - Jorstad, Svetlana
AU - Jung, Taehyun
AU - Karami, Mansour
AU - Karuppusamy, Ramesh
AU - Kawashima, Tomohisa
AU - Keating, Garrett K.
AU - Kettenis, Mark
AU - Kim, Dong Jin
AU - Kim, Jae Young
AU - Kim, Jongsoo
AU - Kim, Junhan
AU - Kino, Motoki
AU - Koay, Jun Yi
AU - Kofuji, Yutaro
AU - Koch, Patrick M.
AU - Koyama, Shoko
AU - Kramer, Carsten
AU - Kramer, Michael
AU - Krichbaum, Thomas P.
AU - Kuo, Cheng Yu
AU - Lauer, Tod R.
AU - Lee, Sang Sung
AU - Levis, Aviad
AU - Li, Yan Rong
AU - Li, Zhiyuan
AU - Lindqvist, Michael
AU - Lico, Rocco
AU - Lindahl, Greg
AU - Liu, Jun
AU - Liu, Kuo
AU - Liuzzo, Elisabetta
AU - Lo, Wen Ping
AU - Lobanov, Andrei P.
AU - Loinard, Laurent
AU - Lonsdale, Colin
AU - Lu, Ru Sen
AU - Macdonald, Nicholas R.
AU - Mao, Jirong
AU - Marchili, Nicola
AU - Markoff, Sera
AU - Marrone, Daniel P.
AU - Marscher, Alan P.
AU - Martí-Vidal, Iván
AU - Matsushita, Satoki
AU - Matthews, Lynn D.
AU - Menten, Karl M.
AU - Mizuno, Izumi
AU - Mizuno, Yosuke
AU - Moran, James M.
AU - Moriyama, Kotaro
AU - Moscibrodzka, Monika
AU - Müller, Cornelia
AU - Mejías, Alejandro Mus
AU - Musoke, Gibwa
AU - Nagai, Hiroshi
AU - Nagar, Neil M.
AU - Nakamura, Masanori
AU - Narayan, Ramesh
AU - Narayanan, Gopal
AU - Natarajan, Iniyan
AU - Nathanail, Antonios
AU - Neilsen, Joey
AU - Neri, Roberto
AU - Ni, Chunchong
AU - Noutsos, Aristeidis
AU - Nowak, Michael A.
AU - Okino, Hiroki
AU - Olivares, Héctor
AU - Ortiz-León, Gisela N.
AU - Oyama, Tomoaki
AU - Palumbo, Daniel C.M.
AU - Park, Jongho
AU - Patel, Nimesh
AU - Pen, Ue Li
AU - Pesce, Dominic W.
AU - Piétu, Vincent
AU - Plambeck, Richard
AU - Popstefanija, Aleksandar
AU - Porth, Oliver
AU - Pötzl, Felix M.
AU - Preciado-López, Jorge A.
AU - Pu, Hung Yi
AU - Ramakrishnan, Venkatessh
AU - Rao, Ramprasad
AU - Rawlings, Mark G.
AU - Raymond, Alexander W.
AU - Rezzolla, Luciano
AU - Ripperda, Bart
AU - Roelofs, Freek
AU - Rogers, Alan
AU - Ros, Eduardo
AU - Rose, Mel
AU - Roshanineshat, Arash
AU - Rottmann, Helge
AU - Roy, Alan L.
AU - Ruszczyk, Chet
AU - Rygl, Kazi L.J.
AU - Sánchez, Salvador
AU - Sánchez-Arguelles, David
AU - Sasada, Mahito
AU - Savolainen, Tuomas
AU - Schloerb, F. Peter
AU - Schuster, Karl Friedrich
AU - Shao, Lijing
AU - Shen, Zhiqiang
AU - Small, Des
AU - Sohn, Bong Won
AU - Soohoo, Jason
AU - Sun, He
AU - Tazaki, Fumie
AU - Tetarenko, Alexandra J.
AU - Tiede, Paul
AU - Tilanus, Remo P.J.
AU - Titus, Michael
AU - Toma, Kenji
AU - Torne, Pablo
AU - Traianou, Efthalia
AU - Trent, Tyler
AU - Trippe, Sascha
AU - Van Bemmel, Ilse
AU - Van Langevelde, Huib Jan
AU - Van Rossum, Daniel R.
AU - Wagner, Jan
AU - Ward-Thompson, Derek
AU - Wardle, John
AU - Weintroub, Jonathan
AU - Wex, Norbert
AU - Wharton, Robert
AU - Wiik, Kaj
AU - Wu, Qingwen
AU - Yoon, Doosoo
AU - Young, André
AU - Young, Ken
AU - Younsi, Ziri
AU - Yuan, Feng
AU - Yuan, Ye Fei
AU - Zensus, J. Anton
AU - Zhao, Guang Yao
AU - Zhao, Shan Shan
N1 - Publisher Copyright: © 2022. The Author(s). Published by the American Astronomical Society.
PY - 2022/1/1
Y1 - 2022/1/1
N2 - The black hole images obtained with the Event Horizon Telescope (EHT) are expected to be variable at the dynamical timescale near their horizons. For the black hole at the center of the M87 galaxy, this timescale (5-61 days) is comparable to the 6 day extent of the 2017 EHT observations. Closure phases along baseline triangles are robust interferometric observables that are sensitive to the expected structural changes of the images but are free of station-based atmospheric and instrumental errors. We explored the day-to-day variability in closure-phase measurements on all six linearly independent nontrivial baseline triangles that can be formed from the 2017 observations. We showed that three triangles exhibit very low day-to-day variability, with a dispersion of ∼3°-5°. The only triangles that exhibit substantially higher variability (∼90°-180°) are the ones with baselines that cross the visibility amplitude minima on the u-v plane, as expected from theoretical modeling. We used two sets of general relativistic magnetohydrodynamic simulations to explore the dependence of the predicted variability on various black hole and accretion-flow parameters. We found that changing the magnetic field configuration, electron temperature model, or black hole spin has a marginal effect on the model consistency with the observed level of variability. On the other hand, the most discriminating image characteristic of models is the fractional width of the bright ring of emission. Models that best reproduce the observed small level of variability are characterized by thin ring-like images with structures dominated by gravitational lensing effects and thus least affected by turbulence in the accreting plasmas.
AB - The black hole images obtained with the Event Horizon Telescope (EHT) are expected to be variable at the dynamical timescale near their horizons. For the black hole at the center of the M87 galaxy, this timescale (5-61 days) is comparable to the 6 day extent of the 2017 EHT observations. Closure phases along baseline triangles are robust interferometric observables that are sensitive to the expected structural changes of the images but are free of station-based atmospheric and instrumental errors. We explored the day-to-day variability in closure-phase measurements on all six linearly independent nontrivial baseline triangles that can be formed from the 2017 observations. We showed that three triangles exhibit very low day-to-day variability, with a dispersion of ∼3°-5°. The only triangles that exhibit substantially higher variability (∼90°-180°) are the ones with baselines that cross the visibility amplitude minima on the u-v plane, as expected from theoretical modeling. We used two sets of general relativistic magnetohydrodynamic simulations to explore the dependence of the predicted variability on various black hole and accretion-flow parameters. We found that changing the magnetic field configuration, electron temperature model, or black hole spin has a marginal effect on the model consistency with the observed level of variability. On the other hand, the most discriminating image characteristic of models is the fractional width of the bright ring of emission. Models that best reproduce the observed small level of variability are characterized by thin ring-like images with structures dominated by gravitational lensing effects and thus least affected by turbulence in the accreting plasmas.
UR - http://www.scopus.com/inward/record.url?scp=85125877065&partnerID=8YFLogxK
U2 - 10.3847/1538-4357/ac332e
DO - 10.3847/1538-4357/ac332e
M3 - Article
AN - SCOPUS:85125877065
SN - 0004-637X
VL - 925
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 13
ER -