2D gravity and random matrices
P Di Francesco, P Ginsparg, J Zinn-Justin - Physics Reports, 1995 - Elsevier
We review recent progress in 2D gravity coupled to d< 1 conformal matter, based on a
representation of discrete gravity in terms of random matrices. We discuss the saddle point …
representation of discrete gravity in terms of random matrices. We discuss the saddle point …
Topological field theory
D Birmingham, M Blau, M Rakowski, G Thompson - Physics Reports, 1991 - Elsevier
6.1. 3. Evaluation of the partition function 252 A. 2. Supersymmetric quantum mechanics 319
6.1. 4. Evaluation ofthe observables: knot A. 3. Topological sigma models 320 invariants 255 …
6.1. 4. Evaluation ofthe observables: knot A. 3. Topological sigma models 320 invariants 255 …
JT gravity as a matrix integral
We present exact results for partition functions of Jackiw-Teitelboim (JT) gravity on two-
dimensional surfaces of arbitrary genus with an arbitrary number of boundaries. The …
dimensional surfaces of arbitrary genus with an arbitrary number of boundaries. The …
[PDF][PDF] Quantum Gravity
C Rovelli - 2004 - 117.250.119.200
Quantum gravity poses the problem of merging quantum mechanics and general relativity,
the two great conceptual revolutions in the physics of the twentieth century. The loop and …
the two great conceptual revolutions in the physics of the twentieth century. The loop and …
Two-dimensional gravity and intersection theory on moduli space
E Witten - The Large N Expansion In Quantum Field Theory And …, 1993 - World Scientific
These are notes based on two lectures given at the Conference on Geometry and Topology
(Harvard University, April 1990). The first was mainly devoted to explaining a conjecture …
(Harvard University, April 1990). The first was mainly devoted to explaining a conjecture …
Exactly solvable field theories of closed strings
E Brezin, VA Kazakov - Physics Letters B, 1990 - Elsevier
Field theories of closed strings are shown to be exactly solvable for a central charge of
matter fields c= 1− 6/m (m+ 1), m= 1, 2, 3,…. The two-point function χ (λ, N), in which λ is the …
matter fields c= 1− 6/m (m+ 1), m= 1, 2, 3,…. The two-point function χ (λ, N), in which λ is the …
Strings in less than one dimension
MR Douglas, SH Shenker - Nuclear Physics B, 1990 - Elsevier
Starting from the random triangulation definition of two-dimensional euclidean quantum
gravity, we define the continuum limit and compute the partition function for closed surfaces …
gravity, we define the continuum limit and compute the partition function for closed surfaces …
Conformal field theories coupled to 2-D gravity in the conformal gauge
F David - Modern Physics Letters A, 1988 - World Scientific
The coupling of conformal field theories to 2-d gravity may be studied in the conformal
gauge. As an application, the results of Knizhnik, Polyakov and Zamolodchikov for the …
gauge. As an application, the results of Knizhnik, Polyakov and Zamolodchikov for the …
Nonperturbative two-dimensional quantum gravity
We propose a nonperturbative definition of two-dimensional quantum gravity, based on a
double-scaling limit of the random-matrix model. We derive an exact differential equation for …
double-scaling limit of the random-matrix model. We derive an exact differential equation for …
Conformal bootstrap in Liouville field theory
A Zamolodchikov, A Zamolodchikov - Nuclear Physics B, 1996 - Elsevier
We consider the recently proposed analytic expression for the three-point function in the
Liouville field theory on a sphere. It is verified that in the classical limit this expression …
Liouville field theory on a sphere. It is verified that in the classical limit this expression …