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Consistent dimer models on surfaces with boundary

Published online by Cambridge University Press:  10 July 2025

Jonah Berggren
Affiliation:
University of Kentucky; E-mail: jrberggren@uky.edu
Khrystyna Serhiyenko*
Affiliation:
University of Kentucky
*
E-mail: khrystyna.serhiyenko@uky.edu (corresponding author)

Abstract

A dimer model is a quiver with faces embedded in a surface. We define and investigate notions of consistency for dimer models on general surfaces with boundary which restrict to well-studied consistency conditions in the disk and torus case. We define weak consistency in terms of the associated dimer algebra and show that it is equivalent to the absence of bad configurations on the strand diagram. In the disk and torus case, weakly consistent models are nondegenerate, meaning that every arrow is contained in a perfect matching; this is not true for general surfaces. Strong consistency is defined to require weak consistency as well as nondegeneracy. We prove that the completed as well as the noncompleted dimer algebra of a strongly consistent dimer model are bimodule internally 3-Calabi-Yau with respect to their boundary idempotents. As a consequence, the Gorenstein-projective module category of the completed boundary algebra of suitable dimer models categorifies the cluster algebra given by their underlying quiver. We provide additional consequences of weak and strong consistency, including that one may reduce a strongly consistent dimer model by removing digons and that consistency behaves well under taking dimer submodels.

Information

Type
Algebra
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2025. Published by Cambridge University Press
Figure 0

Figure 1 An example of a cycle-removing morph.

Figure 1

Figure 2 The top left shows a clockwise cycle p at v. The bottom left shows $m_\alpha (p)$. In the notation of Definition 3.2, $a=b$ and the paths $p',q',R',q"$ are all constant paths at v; hence, $\omega _\alpha (p)$ is constant. The top right shows a clockwise cycle q at a different v, and the bottom right shows $m_\alpha (q)$. In this case, $q"R'q'$ is the clockwise square face containing v, so $\omega _\alpha (q)$ is defined to be constant.

Figure 2

Figure 3 The paths p and q bound two disks and p is to the right of q.

Figure 3

Figure 4 The path q is to the right of p and r is to the right of q, but r is not to the right of p.

Figure 4

Figure 5 On the left is a counter-clockwise cycle p at v. Cycle-removing right-morphing p at the arrow $\alpha $ results in a clockwise cycle which does not enclose p.

Figure 5

Figure 6 On the left, r winds to the right from $t(p)$ to $t(\alpha )$. On the left, r winds to the left from $t(p)$ to $h(\alpha )$. In both cases, there is no way to complete the beginning of r (pictured) to a path from $t(p)$ to $h(p)$ without breaking elementariness or entering $q^{-1}p$.

Figure 6

Figure 7 One oriented (left) and two alternating (right) regions. The bold segment is boundary.

Figure 7

Figure 8 The three bad configurations. The shaded areas are contractible.

Figure 8

Figure 9 The arrows between two alternating faces. The bold arrow is a boundary arrow.

Figure 9

Figure 10 An example of a self-intersection (left), interior cycle (middle), and bad lens (right). All of these give rise to irreducible pairs.

Figure 10

Figure 11 The disk model on the left is not weakly consistent, since it has a homologically trivial interior cycle. When we delete the center face by taking the submodel induced by all other faces, this cycle still exists but is no longer homologically trivial. The result is a weakly consistent dimer model on an annulus.

Figure 11

Figure 12 On the left, a dimer model on a disk with its plabic graph overlayed is pictured. The two pictures on the right show two different perfect matchings, both as collections of arrows of the quiver and as collections of edges of the plabic graph.

Figure 12

Figure 13 A dimer model on a disk which is not weakly consistent but has a perfect matching.

Figure 13

Figure 14 A weakly consistent dimer model on a torus with a disk taken out which has no perfect matching. Opposite dashed edges are identified.

Figure 14

Figure 15 On the left is a strongly consistent dimer model on an annulus which is Noetherian but not boundary-finite. In the middle is a weakly consistent dimer model on an annulus which is boundary-finite but not Noetherian. On the right is a strongly consistent dimer model on an annulus which is boundary-finite but not Noetherian.

Figure 15

Figure 16 Two strongly consistent dimer models on annuli satisfying Noetherianness and boundary finiteness.

Figure 16

Figure 17 A strongly consistent dimer model on an annulus satisfying Noetherianness and boundary finiteness. The left and right sides should be identified. The strands going up are shown in red, while the strands going down are left out for readability.

Figure 17

Figure 18 Removing an internal digon.

Figure 18

Figure 19 Removing a boundary digon.

Figure 19

Figure 20 One way that that a digon could be incident to only one other face. The strand diagram has a bad lens; hence, this configuration is not possible in a weakly consistent dimer model.

Figure 20

Figure 21 A reduced dimer model on an annulus with a digon which may not be removed.

Figure 21

Figure 22 Shown is a dimer model on an infinite half-strip. If all digons were removed, then there would only be one infinite face making up the entire non-compact surface, which is impossible.

Figure 22

Figure 23 Shown on the left is a dimer model on a torus. Opposite dashed edges should be identified. Shown on the right is a piece of its universal cover model.