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Shadow of rotating black holes on a standard background screen
General Relativity and Quantum Cosmology · Submitted 12 Feb 2018
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It is shown that the shape of a black hole shadow depends crucially on the angle between the plane and the view line to the distant observer.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We present the shape of the black hole shadow on the standard background screen as it is registered by the distant observer. The screen is an infinite plane, emitting the quanta uniformly distributed to a hemisphere. The source of emission is considered to be optically thin and optically thick. It is shown that the shape of a black hole shadow depends crucially on the angle between the plane and the view line to the distant observer. The shadow shapes for the different values of this angle are also presented. Both Schwarzschild and Kerr metrics are considered.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present the shape of the black hole shadow on the standard background screen as it is registered by the distant observer. | contribution 0.99 | 0.91 | 0.14 | asserted 0.99 |
| s1 | The screen is an infinite plane, emitting the quanta uniformly distributed to a hemisphere. | method 0.98 | 0.25 | 0.03 | asserted 0.99 |
| s2 | The source of emission is considered to be optically thin and optically thick. | method 0.93 | 0.35 | 0.03 | asserted 0.95 |
| s3 | It is shown that the shape of a black hole shadow depends crucially on the angle between the plane and the view line to the distant observer. | result 1.00 | 0.89 | 0.76 | asserted 1.00 |
| s4 | The shadow shapes for the different values of this angle are also presented. | contribution 0.53 | 0.90 | 0.12 | asserted 0.92 |
| s5 | Both Schwarzschild and Kerr metrics are considered. | method 0.78 | 0.70 | 0.04 | asserted 0.96 |
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The paper
Original abstract
We present the shape of the black hole shadow on the standard background screen as it is registered by the distant observer. The screen is an infinite plane, emitting the quanta uniformly distributed to a hemisphere. The source of emission is considered to be optically thin and optically thick. It is shown that the shape of a black hole shadow depends crucially on the angle between the plane and the view line to the distant observer. The shadow shapes for the different values of this angle are also presented. Both Schwarzschild and Kerr metrics are considered.
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References
How the literature uses it
6 arXiv papers cite this in 7 sentences
Papers citing it · 5 sentences without a confident label
Uses its method or tool 1 paper
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The system of six ordinary differential equations can be found in [ref] .
Black Hole Shadow Observations with Space-Ground Interferometers · Model of BH shadow · 0.95
Cites it as background 1 paper
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(see for example [ref] ).
Comparison of the spatial properties of entrances to black holes and wormholes · Introduction · 0.92
What it cites
Uses data or values from 2 papers
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The second largest is the elliptic galaxy M87 ($θ≈22$ to 41 micro arc seconds [ref] ) and the third is the Andromeda galaxy M31 ($θ≈14$ to 30 micro arc seconds [ref] ).
HST STIS spectroscopy of the triple nucleus of M31: two nested disks in Keplerian rotation around a Supermassive Black Hole · Introduction · 0.99
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The second largest is the elliptic galaxy M87 ($θ≈22$ to 41 micro arc seconds [ref] ) and the third is the Andromeda galaxy M31 ($θ≈14$ to 30 micro arc seconds [ref] ).
The M87 Black Hole Mass from Gas-dynamical Models of Space Telescope Imaging Spectrograph Observations · Introduction · 0.99
Cites as background 6 papers
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The aim of this paper is to consider the structure of the shadow in addition to the many considerations performed earlier [ref] .
Shadows of CPR black holes and tests of the Kerr metric · Introduction · 0.80
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The aim of this paper is to consider the structure of the shadow in addition to the many considerations performed earlier [ref] .
Test of relativistic gravity using microlensing of relativistically broadened lines in gravitationally lensed quasars · Introduction · 0.80
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The aim of this paper is to consider the structure of the shadow in addition to the many considerations performed earlier [ref] .
Shadows of rotating black holes in alternative theories · Introduction · 0.80
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