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arxiv: 2010.01055 · v1 · pith:JQZIEC5Anew · submitted 2020-10-02 · 🌀 gr-qc · astro-ph.HE

Gravitational Test Beyond the First Post-Newtonian Order with the Shadow of the M87 Black Hole

Dimitrios Psaltis , Lia Medeiros , Pierre Christian , Feryal Ozel , Kazunori Akiyama , Antxon Alberdi , Walter Alef , Keiichi Asada
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Rebecca Azulay David Ball Mislav Balokovic John Barrett Dan Bintley Lindy Blackburn Wilfred Boland Geoffrey C. Bower Michael Bremer Christiaan D. Brinkerink Roger Brissenden Silke Britzen Dominique Broguiere Thomas Bronzwaer Do-Young Byun John E. Carlstrom Andrew Chael Chi-kwan Chan Shami Chatterjee Koushik Chatterjee Ming-Tang Chen Yongjun Chen Ilje Cho John E. Conway James M. Cordes Geoffrey B. Crew Yuzhu Cui Jordy Davelaar Mariafelicia De Laurentis Roger Deane Jessica Dempsey Gregory Desvignes Jason Dexter Ralph P. Eatough Heino Falcke Vincent L. Fish Ed Fomalont Raquel Fraga-Encinas Per Friberg Christian M. Fromm Charles F. Gammie Roberto Garc\'ia Olivier Gentaz Ciriaco Goddi Jose L. Gomez Minfeng Gu Mark Gurwell Kazuhiro Hada Ronald Hesper Luis C. Ho Paul Ho Mareki Honma Chih-Wei L. Huang Lei Huang David H. Hughes Makoto Inoue Sara Issaoun David J. James Buell T. Jannuzi Michael Janssen Wu Jiang Alejandra Jimenez-Rosales Michael D. Johnson Svetlana Jorstad Taehyun Jung Mansour Karami Ramesh Karuppusamy Tomohisa Kawashima Garrett K. Keating Mark Kettenis Jae-Young Kim Junhan Kim Jongsoo Kim Motoki Kino Jun Yi Koay Patrick M. Koch Shoko Koyama Michael Kramer Carsten Kramer Thomas P. Krichbaum Cheng-Yu Kuo Tod R. Lauer Sang-Sung Lee Yan-Rong Li Zhiyuan Li Michael Lindqvist Rocco Lico Jun Liu Kuo Liu Elisabetta Liuzzo Wen-Ping Lo Andrei P. Lobanov Colin Lonsdale Ru-Sen Lu Jirong Mao Sera Markoff Daniel P. Marrone Alan P. Marscher Ivan Mart\'i-Vidal Satoki Matsushita Yosuke Mizuno Izumi Mizuno James M. Moran Kotaro Moriyama Monika Moscibrodzka Cornelia Muller Gibwa Musoke Alejandro Mus Mej\'ias Hiroshi Nagai Neil M. Nagar Ramesh Narayan Gopal Narayanan Iniyan Natarajan Roberto Neri Aristeidis Noutsos Hiroki Okino Hector Olivares Tomoaki Oyama Daniel C. M. Palumbo Jongho Park Nimesh Patel Ue-Li Pen Vincent Pietu Richard Plambeck Aleksandar PopStefanija Ben Prather Jorge A. Preciado-Lopez Venkatessh Ramakrishnan Ramprasad Rao Mark G. Rawlings Alexander W. Raymond Bart Ripperda Freek Roelofs Alan Rogers Eduardo Ros Mel Rose Arash Roshanineshat Helge Rottmann Alan L. Roy Chet Ruszczyk Benjamin R. Ryan Kazi L. J. Rygl Salvador Sanchez David Sanchez-Arguelles Mahito Sasada Tuomas Savolainen F. Peter Schloerb Karl-Friedrich Schuster Lijing Shao Zhiqiang Shen Des Small Bong Won Sohn Jason SooHoo Fumie Tazaki Remo P. J. Tilanus Michael Titus Pablo Torne Tyler Trent Efthalia Traianou Sascha Trippe Ilse van Bemmel Huib Jan van Langevelde Daniel R. van Rossum Jan Wagner John Wardle Derek Ward-Thompson Jonathan Weintroub Norbert Wex Robert Wharton Maciek Wielgus George N. Wong Qingwen Wu Doosoo Yoon Andre Young Ken Young Ziri Younsi Feng Yuan Ye-Fei Yuan Shan-Shan Zhao the EHT Collaboration
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classification 🌀 gr-qc astro-ph.HE
keywords black-holegravitationalmetricshadowconstraintscontrolfirstmeasurements
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The 2017 Event Horizon Telescope (EHT) observations of the central source in M87 have led to the first measurement of the size of a black-hole shadow. This observation offers a new and clean gravitational test of the black-hole metric in the strong-field regime. We show analytically that spacetimes that deviate from the Kerr metric but satisfy weak-field tests can lead to large deviations in the predicted black-hole shadows that are inconsistent with even the current EHT measurements. We use numerical calculations of regular, parametric, non-Kerr metrics to identify the common characteristic among these different parametrizations that control the predicted shadow size. We show that the shadow-size measurements place significant constraints on deviation parameters that control the second post-Newtonian and higher orders of each metric and are, therefore, inaccessible to weak-field tests. The new constraints are complementary to those imposed by observations of gravitational waves from stellar-mass sources.

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