We compute the partition function of the conformal field theory on the two-dimensional euclidean black hole background using path-integral techniques. We show that the resulting spectrum is consistent with the algebraic expectations for the SL(2,R)/U(1) coset conformal field theory construction. In particular, we find confirmation for the bound on the spin of the discrete representations and we determine the density of the continuous representations. We point out the relevance of the partition function to all string theory backgrounds that include an SL(2,R)/U(1) coset factor
In this paper we show that the matrix model techniques developed by Dijkgraaf and Vafa can be extend...
We construct a group field theory which realizes the sum of gravity amplitudes over all three dimens...
Fermi Ball is a kind of nontopological soliton with fermions trapped in its domain wall, and is sugg...
The three-dimensional real scalar model, in which the $Z_2$ symmetry spontaneously breaks, is renorm...
In this paper we study QCD and power corrections to sum rules which show up in deep inelastic lepton...
The vacuum energy response of a quantum field theory is studied as a function of complex external fi...
Using canonical method the Liouville theory has been obtained as a gravitational Wess-Zumino action ...
The phase structure of the finite SU(2)xSU(2) theory with N=2 supersymmetry, broken to N=1 by mass t...
Bound states of BPS particles in five-dimensional N=2 supergravity are counted by a topological inde...
We study the effective Hamiltonian for strong-coupling lattice QCD in the case of non-zero baryon de...
We extend the results found for Matrix String Theory to Heterotic Matrix String Theory, i.e. to a 2d...
It has recently been argued that D-branes in bosonic string theory can be described as noncommutativ...
Some aspects of asymptotic freedom are discussed in the context of a simple two-particle non-relativ...
It is shown that the quarks and leptons of the standard model, including a right-handed neutrino, ca...
The local Casimir energy for a wedge with and without a circular outer boundary due to the confineme...
In this paper we show that the matrix model techniques developed by Dijkgraaf and Vafa can be extend...
We construct a group field theory which realizes the sum of gravity amplitudes over all three dimens...
Fermi Ball is a kind of nontopological soliton with fermions trapped in its domain wall, and is sugg...
The three-dimensional real scalar model, in which the $Z_2$ symmetry spontaneously breaks, is renorm...
In this paper we study QCD and power corrections to sum rules which show up in deep inelastic lepton...
The vacuum energy response of a quantum field theory is studied as a function of complex external fi...
Using canonical method the Liouville theory has been obtained as a gravitational Wess-Zumino action ...
The phase structure of the finite SU(2)xSU(2) theory with N=2 supersymmetry, broken to N=1 by mass t...
Bound states of BPS particles in five-dimensional N=2 supergravity are counted by a topological inde...
We study the effective Hamiltonian for strong-coupling lattice QCD in the case of non-zero baryon de...
We extend the results found for Matrix String Theory to Heterotic Matrix String Theory, i.e. to a 2d...
It has recently been argued that D-branes in bosonic string theory can be described as noncommutativ...
Some aspects of asymptotic freedom are discussed in the context of a simple two-particle non-relativ...
It is shown that the quarks and leptons of the standard model, including a right-handed neutrino, ca...
The local Casimir energy for a wedge with and without a circular outer boundary due to the confineme...
In this paper we show that the matrix model techniques developed by Dijkgraaf and Vafa can be extend...
We construct a group field theory which realizes the sum of gravity amplitudes over all three dimens...
Fermi Ball is a kind of nontopological soliton with fermions trapped in its domain wall, and is sugg...