Observational distinction between black holes and naked singularities: the role of the redshift function
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Publication:2786657
DOI10.1088/0264-9381/32/24/247001zbMath1331.83048arXiv1401.4227OpenAlexW2146864838MaRDI QIDQ2786657
Néstor Ortiz, Olivier Sarbach, Thomas Zannias
Publication date: 23 February 2016
Published in: Classical and Quantum Gravity (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/1401.4227
Black holes (83C57) Space-time singularities, cosmic censorship, etc. (83C75) Equations of motion in general relativity and gravitational theory (83C10)
Related Items (7)
No-hair theorem in the wake of Event Horizon Telescope ⋮ Can we distinguish black holes from naked singularities by the images of their accretion disks? ⋮ Static vacuum solutions on curved space–times with torsion ⋮ Deflection angle analysis under the influence of non-plasma medium and plasma medium for regular black hole with cosmic string ⋮ The shadow of a collapsing dark star ⋮ Calculating black hole shadows: review of analytical studies ⋮ Generating rotating spacetime in Ricci-based gravity: naked singularity as a black hole mimicker
Cites Work
- The instability of naked singularities in the gravitational collapse of a scalar field.
- Gravitational blueshift from a collapsing object
- Examples of naked singularity formation in the gravitational collapse of a scalar field
- Odd-parity perturbations of the self-similar LTB spacetime
- Conformal diagrams for the gravitational collapse of a spherical dust cloud
- Strengths of naked singularities in Tolman-Bondi spacetimes
- Cauchy horizon stability in a collapsing spherical dust cloud: II. Energy bounds for test fields and odd-parity gravitational perturbations
- Distinguishing black holes from naked singularities through their accretion disc properties
- Cauchy horizon stability in a collapsing spherical dust cloud: I. Geometric optics approximation and spherically symmetric test fields
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