2017
DOI: 10.1103/revmodphys.89.025001
|View full text |Cite
|
Sign up to set email alerts
|

Testing black hole candidates with electromagnetic radiation

Abstract: Astrophysical black hole candidates are thought to be the Kerr black holes of general relativity, but there is not yet direct observational evidence that the spacetime geometry around these objects is described by the Kerr solution. The study of the properties of the electromagnetic radiation emitted by gas or stars orbiting these objects can potentially test the Kerr black hole hypothesis. This paper reviews the state of the art of this research field, describing the possible approaches to test the Kerr metri… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
256
0

Year Published

2017
2017
2023
2023

Publication Types

Select...
6
3

Relationship

5
4

Authors

Journals

citations
Cited by 275 publications
(258 citation statements)
references
References 337 publications
(392 reference statements)
0
256
0
Order By: Relevance
“…The intensity profile for a corona with arbitrary geometry is often approximated by a power law (∝ 1=r q , where q is the emissivity index) or by a broken power law (∝ 1=r q 1 for r < r br and ∝ 1=r q 2 for r > r br , where q 1 and q 2 are, respectively, the inner and the outer emissivity indices and r br is the breaking radius). Figure 2 shows the iron line shapes calculated in black hole solutions 1-12, assuming that the intensity profile scales as 1=r 3 (Newtonian limit at large radii for a lamppost corona), that the inclination angle of the disk with respect to the line of sight of the distant observer is i ¼ 45°, and that the rest frame energy of the line is 6.4 keV. The calculations are done with the code described in Refs.…”
Section: X-ray Reflection Spectrummentioning
confidence: 99%
See 1 more Smart Citation
“…The intensity profile for a corona with arbitrary geometry is often approximated by a power law (∝ 1=r q , where q is the emissivity index) or by a broken power law (∝ 1=r q 1 for r < r br and ∝ 1=r q 2 for r > r br , where q 1 and q 2 are, respectively, the inner and the outer emissivity indices and r br is the breaking radius). Figure 2 shows the iron line shapes calculated in black hole solutions 1-12, assuming that the intensity profile scales as 1=r 3 (Newtonian limit at large radii for a lamppost corona), that the inclination angle of the disk with respect to the line of sight of the distant observer is i ¼ 45°, and that the rest frame energy of the line is 6.4 keV. The calculations are done with the code described in Refs.…”
Section: X-ray Reflection Spectrummentioning
confidence: 99%
“…There are two main lines of research to test the nature of astrophysical black holes: the study of the properties of the electromagnetic radiation emitted by gas or stars orbiting these objects [3,4] or the analysis of the gravitational wave signal emitted by a system with a black hole [5,6]. Tests with electromagnetic radiation include, but are not limited to, the study of the thermal spectrum of thin accretion disks [7][8][9][10], the analysis of the reflection spectrum of thin disks [11][12][13][14], the measurements of the frequencies of quasiperiodic oscillations [15][16][17][18], and the possible future detection of black hole shadows [19][20][21][22][23][24][25].…”
Section: Introductionmentioning
confidence: 99%
“…The study of the properties of the electromagnetic radiation emitted by the gas in the accretion disk can potentially probe the spacetime metric around astrophysical black holes and test the Kerr nature of these objects [4]. Previous work has shown that x-ray reflection spectroscopy (the so-called iron line method) [5] is a promising technique to do this job [6].…”
mentioning
confidence: 99%
“…We close with a brief summary and outlook in Section 3. Although we limit the following discussion to General Relativity's Kerr metric in Boyer-Lindquist (BL Boyer & Lindquist 1967) coordinates, the results can easily be adapted to work for other stationary, axisymmetric, and asymptotically flat black hole spacetimes (see Johannsen 2016;Bambi 2017, for recent reviews describing observational constraints on alternative black hole spacetimes).…”
Section: Introductionmentioning
confidence: 99%