2018
DOI: 10.1214/17-aihp852
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Liouville quantum gravity on the unit disk

Abstract: Our purpose is to pursue the rigorous construction of Liouville Quantum Field Theory on Riemann surfaces initiated by F. David, A. Kupiainen and the last two authors in the context of the Riemann sphere and inspired by the 1981 seminal work by Polyakov. In this paper, we investigate the case of simply connected domains with boundary. We also make precise conjectures about the relationship of this theory to scaling limits of random planar maps with boundary conformally embedded onto the disk.

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Cited by 59 publications
(99 citation statements)
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“…The additional condition on p, p < (1 + 4 γ 2 (1 + a)) ∧ (1 + 4 γ 2 (1 + b)), comes from the presence of the insertions. A proof of the bounds (1.5) can be found in [29,14]. Now the goal of our paper is simply to prove the following exact formula for M (γ, p, a, b):…”
mentioning
confidence: 99%
“…The additional condition on p, p < (1 + 4 γ 2 (1 + a)) ∧ (1 + 4 γ 2 (1 + b)), comes from the presence of the insertions. A proof of the bounds (1.5) can be found in [29,14]. Now the goal of our paper is simply to prove the following exact formula for M (γ, p, a, b):…”
mentioning
confidence: 99%
“…Our paper also clarifies a few points that were not addressed in [4,13]. First, we justify for any background metric g the expression of the covariance of our field X g by diagonalizing an operator T defined using Neumann boundary conditions.…”
Section: Introductionmentioning
confidence: 67%
“…The probabilistic framework used throughout this paper was introduced in [4] where the authors provide a construction of LQG for the Riemann sphere. Following the same approach, the theory has been defined on the unit disk in [13], on the complex tori in [5] and on compact Riemann surfaces of higher genus in [12]. The Riemann sphere is the simplest case as it corresponds to a simply connected compact surface without boundary.…”
Section: Introductionmentioning
confidence: 99%
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“…We also record the formula c L = 1 + 6Q 2 , which is obtained by combining (1.1) and (1.3). It was shown rigorously in [DKRV16] that the partition function of LCFT transforms under conformal rescaling as the partition function of a CFT with central charge c L for c L ≥ 25, which corresponds to c M ∈ (−∞, 1], in the case of the sphere topology (see [HRV18,DRV16,GRV16] for other topologies). From the point of view of constructive quantum field theory, this means that LCFT is a CFT with central charge c L .…”
Section: Introduction 1overviewmentioning
confidence: 99%