scholarly journals The uniqueness theorem for rotating black hole solutions of self-gravitating harmonic mappings

1995 ◽  
Vol 12 (8) ◽  
pp. 2021-2035 ◽  
Author(s):  
Markus Heusler
2017 ◽  
Vol 132 (2) ◽  
Author(s):  
Bobir Toshmatov ◽  
Zdeněk Stuchlík ◽  
Bobomurat Ahmedov

2005 ◽  
Vol 14 (12) ◽  
pp. 2219-2225 ◽  
Author(s):  
YUAN K. HA

A new theorem for black holes is found. It is called the horizon mass theorem. The horizon mass is the mass which cannot escape from the horizon of a black hole. For all black holes, neutral, charged or rotating, the horizon mass is always twice the irreducible mass observed at infinity. Previous theorems on black holes are: (i) the singularity theorem, (ii) the area theorem, (iii) the uniqueness theorem, (iv) the positive energy theorem. The horizon mass theorem is possibly the last general theorem for classical black holes. It is crucial for understanding Hawking radiation and for investigating processes occurring near the horizon.


2019 ◽  
Vol 34 (07n08) ◽  
pp. 1950060
Author(s):  
O. B. Zaslavskii

We consider a vacuum static spacetime in a finite size cavity. On the boundary, we specify a metric and a finite constant local temperature [Formula: see text]. No spherical or any other spatial symmetry is assumed. We show that (i) inside a cavity, only a black hole or flat spacetime are possible, whereas a curved horizonless regular spacetime is excluded, (ii) in the limit when the horizon area shrinks, the Hawking temperature diverges, (iii) for the existence of a black hole, [Formula: see text] should be high enough. When [Formula: see text], a black hole phase is favorable thermodynamically. Our consideration essentially uses the coordinate system introduced by Israel in his famous proof of the uniqueness theorem.


2002 ◽  
Vol 17 (32) ◽  
pp. 2137-2146
Author(s):  
A. A. RODRIGUES SOBREIRA ◽  
V. B. BEZERRA

We consider the scalar gravity theory in (2 + 1) dimensions and find an electrically charged and a rotating black hole solutions. The first solution was obtained by combining the scalar gravity and Maxwell equations and the second one by applying the method of complex coordinate transformation to the nonrotating counterpart solution.


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