We consider an embedding of the extremal four-dimensional Reissner-Nordstr\"om black hole into type IIB string theory. The equivalent type IIB configuration, in the D-brane weak-coupling picture, is a bound state of D1- and D5-branes threaded by fundamental type IIB strings. The bound state involves also a NSNS solitonic 5-brane, mimicking the role of the Kaluza-Klein magnetic monopole. The statistical entropy derived by counting the degeneracy of the BPS-saturated excitations of this bound state agrees perfectly with the (semiclassical) Bekenstein-Hawking formula
We calculate the entropy of 4-charge extremal black holes in Type IIA supersting theory by using Sen...
The Hawking Beckenstein entropy of near extremal fivebranes is calculated in terms of a gas of strin...
We present the main features of the physics of extremal black holes embedded in supersymmetric theor...
We reconsider the four dimensional extremal black hole constructed in type IIB string theory as the ...
We identify the states in string theory which are responsible for the entropy of near-extremal rotat...
A six-parameter family of five-dimensional black hole solutions is constructed which are labeled by ...
We explore the connection between D-branes and black holes in one particular case: a $D3$-brane comp...
We explore the connection between D-branes and black holes in one particular case: a D3-brane compac...
In four dimensions there are 4 different types of extremal Maxwell/scalar black holes characterized ...
In four dimensions there are 4 different types of extremal Maxwell/scalar black holes characterized ...
In four dimensions there are 4 different types of extremal Maxwell/scalar black holes characterized ...
In four dimensions there are 4 different types of extremal Maxwell/scalar black holes characterized ...
A black hole solution to low energy type IIA string theory which is extremal, non-supersymmetric, an...
In this talk I address some aspects in the recent developments for N=2 black holes in 4 dimensions. ...
The emission of a scalar with low energy $\omega$, from a $D (4\le D\le 8 )$ dimensional black hole ...
We calculate the entropy of 4-charge extremal black holes in Type IIA supersting theory by using Sen...
The Hawking Beckenstein entropy of near extremal fivebranes is calculated in terms of a gas of strin...
We present the main features of the physics of extremal black holes embedded in supersymmetric theor...
We reconsider the four dimensional extremal black hole constructed in type IIB string theory as the ...
We identify the states in string theory which are responsible for the entropy of near-extremal rotat...
A six-parameter family of five-dimensional black hole solutions is constructed which are labeled by ...
We explore the connection between D-branes and black holes in one particular case: a $D3$-brane comp...
We explore the connection between D-branes and black holes in one particular case: a D3-brane compac...
In four dimensions there are 4 different types of extremal Maxwell/scalar black holes characterized ...
In four dimensions there are 4 different types of extremal Maxwell/scalar black holes characterized ...
In four dimensions there are 4 different types of extremal Maxwell/scalar black holes characterized ...
In four dimensions there are 4 different types of extremal Maxwell/scalar black holes characterized ...
A black hole solution to low energy type IIA string theory which is extremal, non-supersymmetric, an...
In this talk I address some aspects in the recent developments for N=2 black holes in 4 dimensions. ...
The emission of a scalar with low energy $\omega$, from a $D (4\le D\le 8 )$ dimensional black hole ...
We calculate the entropy of 4-charge extremal black holes in Type IIA supersting theory by using Sen...
The Hawking Beckenstein entropy of near extremal fivebranes is calculated in terms of a gas of strin...
We present the main features of the physics of extremal black holes embedded in supersymmetric theor...