Perturbing isoradial triangulations
We consider an infinite planar Delaunay graph \mathbf{G}_{\epsilon} which is obtained by locally deforming the coordinate embedding of a general isoradial graph \mathbf{G}_{\mathrm{cr}} , with respect to a real deformation parameter \epsilon . Using Kenyon’s exact and asymptotic results for the crit...
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Veröffentlicht in: | Annales de l'Institut Henri Poincaré. D. Combinatorics, physics and their interactions physics and their interactions, 2024-03, Vol.11 (4), p.715-859 |
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Sprache: | eng |
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Zusammenfassung: | We consider an infinite planar Delaunay graph
\mathbf{G}_{\epsilon}
which is obtained by locally deforming the coordinate embedding of a general isoradial graph
\mathbf{G}_{\mathrm{cr}}
, with respect to a real deformation parameter
\epsilon
. Using Kenyon’s exact and asymptotic results for the critical Green’s function on an isoradial graph, we calculate the leading asymptotics of the first- and second-order terms in the perturbative expansion of the log-determinant of the Laplace–Beltrami operator
\Delta(\epsilon)
, the David–Eynard Kähler operator
\mathcal{D}(\epsilon)
, and the conformal Laplacian
{\underline{\boldsymbol{\Delta}}}(\epsilon)
on the deformed Delaunay graph
\mathbf{G}_{\epsilon}
. We show that the scaling limits of the second-order
bi-local
term for both the Laplace–Beltrami and David–Eynard Kähler operators exist and coincide, with a shared value independent of the choice of the initial isoradial graph
\mathbf{G}_{\mathrm{cr}}
. Our results allow us to define a discrete analog of the stress-energy tensor for each of the three operators. Furthermore, we can identify a central charge (
c=-2
) in the case of both the Laplace–Beltrami and David–Eynard Kähler operators. While the scaling limit is consistent with the stress-energy tensor and the value of the central charge for the Gaussian free field (GFF), the discrete central charge value of
c=-2
for the David–Eynard Kähler operator is, however, at odds with the value of
c=-26
expected by Polyakov’s theory of 2D quantum gravity; moreover, there are problems with convergence of the scaling limit of the discrete stress-energy tensor for the David–Eynard Kähler operator. The second-order bi-local term for the conformal Laplacian involves anomalous terms corresponding to the creation of discrete
curvature dipoles
in the deformed Delaunay graph
\mathbf{G}_{\epsilon}
; we examine the difficulties in defining a convergent scaling limit in this case. Connections with some discrete statistical models at criticality are explored. |
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ISSN: | 2308-5827 2308-5835 |
DOI: | 10.4171/aihpd/178 |