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 in | The Astrophysical journal Vol. 814; no. 2; pp. 115 - 14 | 
|---|---|
| Main Authors | , , , | 
| Format | Journal Article | 
| Language | English | 
| Published | 
        United States
          The American Astronomical Society
    
        01.12.2015
     | 
| Subjects | |
| Online Access | Get full text | 
| ISSN | 0004-637X 1538-4357 1538-4357  | 
| DOI | 10.1088/0004-637X/814/2/115 | 
Cover
| 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%. | 
    
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| 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  | 
    
| Author_xml | – sequence: 1 givenname: Dimitrios orcidid: 0000-0003-4058-2837 surname: Psaltis fullname: Psaltis, Dimitrios organization: University of Arizona Astronomy Department, 933 N. Cherry Ave, Tucson, AZ 85721, USA – sequence: 2 givenname: Feryal surname: Özel fullname: Özel, Feryal organization: University of Arizona Astronomy Department, 933 N. Cherry Ave, Tucson, AZ 85721, USA – sequence: 3 givenname: Chi-Kwan orcidid: 0000-0003-2313-4581 surname: Chan fullname: Chan, Chi-Kwan organization: University of Arizona Astronomy Department, 933 N. Cherry Ave, Tucson, AZ 85721, USA – sequence: 4 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 | 
    
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