A GENERAL RELATIVISTIC NULL HYPOTHESIS TEST WITH EVENT HORIZON TELESCOPE OBSERVATIONS OF THE BLACK HOLE SHADOW IN Sgr A

ABSTRACT The half opening angle of a Kerr black hole shadow is always equal to (5 0.2)GM/Dc2, where M is the mass of the black hole and D is its distance from the Earth. Therefore, measuring the size of a shadow and verifying whether it is within this 4% range constitutes a null hypothesis test of g...

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Published inThe Astrophysical journal Vol. 814; no. 2; pp. 115 - 14
Main Authors Psaltis, Dimitrios, Özel, Feryal, Chan, Chi-Kwan, Marrone, Daniel P.
Format Journal Article
LanguageEnglish
Published United States The American Astronomical Society 01.12.2015
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ISSN0004-637X
1538-4357
1538-4357
DOI10.1088/0004-637X/814/2/115

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Abstract ABSTRACT The half opening angle of a Kerr black hole shadow is always equal to (5 0.2)GM/Dc2, where M is the mass of the black hole and D is its distance from the Earth. Therefore, measuring the size of a shadow and verifying whether it is within this 4% range constitutes a null hypothesis test of general relativity. We show that the black hole in the center of the Milky Way, Sgr A*, is the optimal target for performing this test with upcoming observations using the Event Horizon Telescope (EHT). We use the results of optical/IR monitoring of stellar orbits to show that the mass-to-distance ratio for Sgr A* is already known to an accuracy of ∼4%. We investigate our prior knowledge of the properties of the scattering screen between Sgr A* and the Earth, the effects of which will need to be corrected for in order for the black hole shadow to appear sharp against the background emission. Finally, we explore an edge detection scheme for interferometric data and a pattern matching algorithm based on the Hough/Radon transform and demonstrate that the shadow of the black hole at 1.3 mm can be localized, in principle, to within ∼9%. All these results suggest that our prior knowledge of the properties of the black hole, of scattering broadening, and of the accretion flow can only limit this general relativistic null hypothesis test with EHT observations of Sgr A* to 10%.
AbstractList The half opening angle of a Kerr black hole shadow is always equal to (5 + or - 0.2)GM/Dc super(2), where M is the mass of the black hole and D is its distance from the Earth. Therefore, measuring the size of a shadow and verifying whether it is within this 4% range constitutes a null hypothesis test of general relativity. We show that the black hole in the center of the Milky Way, Sgr A*, is the optimal target for performing this test with upcoming observations using the Event Horizon Telescope (EHT). We use the results of optical/IR monitoring of stellar orbits to show that the mass-to-distance ratio for Sgr A* is already known to an accuracy of ~4%. We investigate our prior knowledge of the properties of the scattering screen between Sgr A* and the Earth, the effects of which will need to be corrected for in order for the black hole shadow to appear sharp against the background emission. Finally, we explore an edge detection scheme for interferometric data and a pattern matching algorithm based on the Hough/Radon transform and demonstrate that the shadow of the black hole at 1.3 mm can be localized, in principle, to within ~9%. All these results suggest that our prior knowledge of the properties of the black hole, of scattering broadening, and of the accretion flow can only limit this general relativistic null hypothesis test with EHT observations of Sgr A* to [<, ~]10%.
The half opening angle of a Kerr black hole shadow is always equal to (5 ± 0.2)GM/Dc{sup 2}, where M is the mass of the black hole and D is its distance from the Earth. Therefore, measuring the size of a shadow and verifying whether it is within this 4% range constitutes a null hypothesis test of general relativity. We show that the black hole in the center of the Milky Way, Sgr A*, is the optimal target for performing this test with upcoming observations using the Event Horizon Telescope (EHT). We use the results of optical/IR monitoring of stellar orbits to show that the mass-to-distance ratio for Sgr A* is already known to an accuracy of ∼4%. We investigate our prior knowledge of the properties of the scattering screen between Sgr A* and the Earth, the effects of which will need to be corrected for in order for the black hole shadow to appear sharp against the background emission. Finally, we explore an edge detection scheme for interferometric data and a pattern matching algorithm based on the Hough/Radon transform and demonstrate that the shadow of the black hole at 1.3 mm can be localized, in principle, to within ∼9%. All these results suggest that our prior knowledge of the properties of the black hole, of scattering broadening, and of the accretion flow can only limit this general relativistic null hypothesis test with EHT observations of Sgr A* to ≲10%.
ABSTRACT The half opening angle of a Kerr black hole shadow is always equal to (5 0.2)GM/Dc2, where M is the mass of the black hole and D is its distance from the Earth. Therefore, measuring the size of a shadow and verifying whether it is within this 4% range constitutes a null hypothesis test of general relativity. We show that the black hole in the center of the Milky Way, Sgr A*, is the optimal target for performing this test with upcoming observations using the Event Horizon Telescope (EHT). We use the results of optical/IR monitoring of stellar orbits to show that the mass-to-distance ratio for Sgr A* is already known to an accuracy of ∼4%. We investigate our prior knowledge of the properties of the scattering screen between Sgr A* and the Earth, the effects of which will need to be corrected for in order for the black hole shadow to appear sharp against the background emission. Finally, we explore an edge detection scheme for interferometric data and a pattern matching algorithm based on the Hough/Radon transform and demonstrate that the shadow of the black hole at 1.3 mm can be localized, in principle, to within ∼9%. All these results suggest that our prior knowledge of the properties of the black hole, of scattering broadening, and of the accretion flow can only limit this general relativistic null hypothesis test with EHT observations of Sgr A* to 10%.
Author Chan, Chi-Kwan
Özel, Feryal
Marrone, Daniel P.
Psaltis, Dimitrios
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  surname: Özel
  fullname: Özel, Feryal
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  orcidid: 0000-0003-2313-4581
  surname: Chan
  fullname: Chan, Chi-Kwan
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  givenname: Daniel P.
  orcidid: 0000-0002-2367-1080
  surname: Marrone
  fullname: Marrone, Daniel P.
  organization: University of Arizona Astronomy Department, 933 N. Cherry Ave, Tucson, AZ 85721, USA
BackLink https://www.osti.gov/biblio/22521851$$D View this record in Osti.gov
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Snippet ABSTRACT The half opening angle of a Kerr black hole shadow is always equal to (5 0.2)GM/Dc2, where M is the mass of the black hole and D is its distance from...
The half opening angle of a Kerr black hole shadow is always equal to (5 + or - 0.2)GM/Dc super(2), where M is the mass of the black hole and D is its distance...
The half opening angle of a Kerr black hole shadow is always equal to (5 ± 0.2)GM/Dc{sup 2}, where M is the mass of the black hole and D is its distance from...
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SubjectTerms ACCRETION DISKS
accretion, accretion disks
ALGORITHMS
ASTROPHYSICS, COSMOLOGY AND ASTRONOMY
black hole physics
BLACK HOLES
Black holes (astronomy)
DISTANCE
Earth
Event horizon
Galaxy: center
GENERAL RELATIVITY THEORY
IMAGE PROCESSING
MASS
MILKY WAY
Null hypothesis
ORBITS
RELATIVISTIC RANGE
SCATTERING
Shadows
techniques: image processing
TELESCOPES
Title A GENERAL RELATIVISTIC NULL HYPOTHESIS TEST WITH EVENT HORIZON TELESCOPE OBSERVATIONS OF THE BLACK HOLE SHADOW IN Sgr A
URI https://iopscience.iop.org/article/10.1088/0004-637X/814/2/115
https://www.proquest.com/docview/1790966078
https://www.proquest.com/docview/1815985418
https://www.osti.gov/biblio/22521851
Volume 814
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