Develops negative-variance Gaussian theory and proves timelike DOZZ formula plus k-point functions for timelike Liouville theory under charge neutrality, with semiclassical limits as coupling goes to zero.
Title resolution pending
4 Pith papers cite this work. Polarity classification is still indexing.
4
Pith papers citing it
citation-role summary
background 1
citation-polarity summary
fields
math.PR 4verdicts
UNVERDICTED 4roles
background 1polarities
background 1representative citing papers
Nonlinear functionals of the discrete GFF with degenerate random conductances on ergodic random subgraphs converge almost surely to continuum counterparts in H^{-s}(D).
Renormalized two-point functions for CLE4 gaskets are computed probabilistically via loop soups and GFF, corresponding to Ashkin-Teller spin correlations and recovering Ising at the decoupling point.
Establishes upper and lower heat kernel bounds for √(8/3)-Liouville Brownian motion that are sharp up to polylog factors in the exponential, expressed in terms of the √(8/3)-LQG metric.
citing papers explorer
-
Rigorous results for timelike Liouville field theory
Develops negative-variance Gaussian theory and proves timelike DOZZ formula plus k-point functions for timelike Liouville theory under charge neutrality, with semiclassical limits as coupling goes to zero.
-
Scaling limits for nonlinear functionals of the discrete Gaussian free field with degenerate random conductances
Nonlinear functionals of the discrete GFF with degenerate random conductances on ergodic random subgraphs converge almost surely to continuum counterparts in H^{-s}(D).
-
Renormalised two-point functions of CLE$_4$ gaskets
Renormalized two-point functions for CLE4 gaskets are computed probabilistically via loop soups and GFF, corresponding to Ashkin-Teller spin correlations and recovering Ising at the decoupling point.
-
Two-sided heat kernel bounds for $\sqrt{8/3}$-Liouville Brownian motion
Establishes upper and lower heat kernel bounds for √(8/3)-Liouville Brownian motion that are sharp up to polylog factors in the exponential, expressed in terms of the √(8/3)-LQG metric.