the vaidya black holes in non-flat backgrounds c v vishveshwara

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The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara

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Page 1: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara

The Vaidya Black Holes in Non-flat Backgrounds

C V Vishveshwara

Page 2: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara
Page 3: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara

THEN A MIRACLE OCCURS !

Page 4: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara
Page 5: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara
Page 6: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara

tent of the field from the Einstein equations is given by :

Page 7: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara

The Event Horizon

Vaidya-Einstein- Kerr (VEK)

Vaidya-Einstein-Schwarzschild (VES) Set a = 0 above

Vaidya-Robertson-Walker (VRW)

Page 8: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara

Work Done

K. Rajesh Nayak, Malcolm MacCallum, CVVVES: Matched to Schwarzschild at horizon and to Einstein universe outside.

B.S. Ramachandra and CVV ; BSR, KRN, CVV Geometrical and physical properties of VES and VEK

P.S.Joshi and J.V.NarlikarBlack hole physics in globally hyperbolic spacetime with VRW as example.

Page 9: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara

What Next?

1. Match VEK to Kerr metric at the horizon. Cannot be matched at stationary limit.

2. VRW: Is the ‘horizon’ a null surface?

3. Further properties of the Vaidya black-hole spacetimes.

4. Explore Whittaker’s spacetimes with: Density +3 X Pressure=Constant( Non-zero).

5. Realistic models of black holes with matter.

Page 10: The Vaidya Black Holes in Non-flat Backgrounds C V Vishveshwara