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'''Photon sphere''' (''definition''<ref>K.S. Virbhadra and G. F.R. Ellis, Schwarzschild black hole lensing, Phys. Rev. D62, 084003 (2000); K.S. Virbhadra and G. F.R. Ellis, Gravitational lensing by naked singularities, Phys. Rev. D65, 103004 (2002).</ref>):<br />
A [[photon sphere]] of a static spherically symmetric [[Metric tensor|metric]] is a [[timelike]] hypersurface <math>\{r=r_{ps}\}</math> if the deflection angle of a light ray with the closest distance of approach <math>r_o</math> diverges  as <math>r_o \rightarrow r_{ps}.</math>
 
For a general static spherically symmetric metric
 
<math>g = - \beta\left(r\right) dt^2 - \alpha(r) dr^2 - \sigma(r) r^2 (d\theta^2 + \sin^2\theta d\phi^2),</math>
 
the photon sphere equation is:
 
<math>2\sigma(r) \beta + r \frac{d\sigma(r)}{dr} \beta(r) - r \frac{d\beta(r)}{dr} \sigma(r) = 0.</math>
 
The concept of a photon sphere in a static spherically metric was generalized to a photon surface of any metric.
 
'''Photon surface''' (''definition''<ref>Clarissa-Marie Claudel, K.S. Virbhadra, and G.F.R. Ellis, The  geometry of photon surfaces, J. Math. Phys. 42, 818-838 (2001).</ref>) : <br />
A photon surface of (M,'''g''') is an immersed, nowhere spacelike hypersurface S of  (M,''' g''')  such that, for every point p∈S and every null vector '''k'''∈''T''<sub>p</sub>S, there exists a null [[geodesic]] <math>{\gamma}</math>:(-ε,ε)→M of (M,'''g''') such that <math>{\dot{\gamma}}</math>(0)='''k''', |γ|⊂S.
 
Both definitions give the same result for a general static spherically symmetric metric.<ref>See in [2].</ref>
 
'''Theorem''':<ref>See in [2].</ref><br />
Subject to an energy condition, a [[black hole]] in any  spherically symmetric  spacetime  must be surrounded by a photon sphere. Conversely, subject to an energy condition, any photon sphere must cover more than a certain amount of matter, a black hole, or a [[naked singularity]].
 
==References==
{{Reflist}}
 
[[Category:Black holes]]
[[Category:General relativity]]

Revision as of 06:05, 29 December 2013

Template:Multiple issues

Photon sphere (definition[1]):
A photon sphere of a static spherically symmetric metric is a timelike hypersurface if the deflection angle of a light ray with the closest distance of approach diverges as

For a general static spherically symmetric metric

the photon sphere equation is:

The concept of a photon sphere in a static spherically metric was generalized to a photon surface of any metric.

Photon surface (definition[2]) :
A photon surface of (M,g) is an immersed, nowhere spacelike hypersurface S of (M, g) such that, for every point p∈S and every null vector kTpS, there exists a null geodesic :(-ε,ε)→M of (M,g) such that (0)=k, |γ|⊂S.

Both definitions give the same result for a general static spherically symmetric metric.[3]

Theorem:[4]
Subject to an energy condition, a black hole in any spherically symmetric spacetime must be surrounded by a photon sphere. Conversely, subject to an energy condition, any photon sphere must cover more than a certain amount of matter, a black hole, or a naked singularity.

References

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  1. K.S. Virbhadra and G. F.R. Ellis, Schwarzschild black hole lensing, Phys. Rev. D62, 084003 (2000); K.S. Virbhadra and G. F.R. Ellis, Gravitational lensing by naked singularities, Phys. Rev. D65, 103004 (2002).
  2. Clarissa-Marie Claudel, K.S. Virbhadra, and G.F.R. Ellis, The geometry of photon surfaces, J. Math. Phys. 42, 818-838 (2001).
  3. See in [2].
  4. See in [2].