In 1973, R. Penrose presented an argument that the total mass of a space-time which contains black holes with event horizons of total area $A$ should be at least $\sqrt{A/16\pi}$. An important special case of this physical statement translates into a very beautiful mathematical inequality in Riemannian geometry known as the Riemannian Penrose inequality. This inequality was first established by G. Huisken and T. Ilmanen in 1997 for a single black hole and then by one of the authors (H.B.) in 1999 for any number of black holes. The two approaches use two different geometric flow techniques and are described here. We further present some background material concerning the problem at hand, discuss some applications of Penrose-type inequalities...
The classical Penrose inequality specifies a lower bound on the total mass in terms of the area of c...
The classical Penrose inequality specifies a lower bound on the total mass in terms of the area of c...
In this paper we revisit Brill's proof of positive mass for three-dimensional, time-symmetric, axisy...
We prove the Riemannian Penrose Conjecture, an important case of a con-jecture [41] made by Roger Pe...
The Penrose inequality estimates the lower bound of the mass of a black hole in terms of the area of...
The classical Penrose inequality relates the mass of an asymptotically flat spacetime to the total a...
The classical Penrose inequality relates the mass of an asymptotically flat spacetime to the total a...
The classical Penrose inequality gives a variational characterization of Schwarzschild data as that ...
Our current picture of black hole gravitational collapse relies on two assumptions: i) the resulting...
The conformal flow of metrics has been used to successfully establish a special case of the Penrose ...
Penrose's inequality which relates the total mass of a space-time containing a black hole with the a...
It is well known that the three parameters that characterize the Kerr black hole (mass, angular mome...
We demonstrate that the Penrose inequality is valid for spherically symmetric geometries even when t...
We establish a Penrose-type inequality with angular momentum for four-dimensional, biaxially symmetr...
We establish a Penrose-type inequality with angular momentum for four-dimensional, biaxially symmetr...
The classical Penrose inequality specifies a lower bound on the total mass in terms of the area of c...
The classical Penrose inequality specifies a lower bound on the total mass in terms of the area of c...
In this paper we revisit Brill's proof of positive mass for three-dimensional, time-symmetric, axisy...
We prove the Riemannian Penrose Conjecture, an important case of a con-jecture [41] made by Roger Pe...
The Penrose inequality estimates the lower bound of the mass of a black hole in terms of the area of...
The classical Penrose inequality relates the mass of an asymptotically flat spacetime to the total a...
The classical Penrose inequality relates the mass of an asymptotically flat spacetime to the total a...
The classical Penrose inequality gives a variational characterization of Schwarzschild data as that ...
Our current picture of black hole gravitational collapse relies on two assumptions: i) the resulting...
The conformal flow of metrics has been used to successfully establish a special case of the Penrose ...
Penrose's inequality which relates the total mass of a space-time containing a black hole with the a...
It is well known that the three parameters that characterize the Kerr black hole (mass, angular mome...
We demonstrate that the Penrose inequality is valid for spherically symmetric geometries even when t...
We establish a Penrose-type inequality with angular momentum for four-dimensional, biaxially symmetr...
We establish a Penrose-type inequality with angular momentum for four-dimensional, biaxially symmetr...
The classical Penrose inequality specifies a lower bound on the total mass in terms of the area of c...
The classical Penrose inequality specifies a lower bound on the total mass in terms of the area of c...
In this paper we revisit Brill's proof of positive mass for three-dimensional, time-symmetric, axisy...