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Large N limit of the Yang–Mills measure on compact surfaces II: Makeenko–Migdal equations and the planar master field

Published online by Cambridge University Press:  28 January 2025

Antoine Dahlqvist*
Affiliation:
University of Sussex, School of Mathematical and Physical Sciences, Pevensey 3 Building, Brighton, UK;
Thibaut Lemoine
Affiliation:
Collège de France, 3, rue d’Ulm, Paris, 75005, France; E-mail: thibaut.lemoine@college-de-france.fr
*
E-mail: a.dahlqvist@sussex.ac.uk (corresponding author)

Abstract

This paper considers the large N limit of Wilson loops for the two-dimensional Euclidean Yang–Mills measure on all orientable compact surfaces of genus larger or equal to $1$, with a structure group given by a classical compact matrix Lie group. Our main theorem shows the convergence of all Wilson loops in probability, given that it holds true on a restricted class of loops, obtained as a modification of geodesic paths. Combined with the result of [20], a corollary is the convergence of all Wilson loops on the torus. Unlike the sphere case, we show that the limiting object is remarkably expressed thanks to the master field on the plane defined in [3, 39], and we conjecture that this phenomenon is also valid for all surfaces of higher genus. We prove that this conjecture holds true whenever it does for the restricted class of loops of the main theorem. Our result on the torus justifies the introduction of an interpolation between free and classical convolution of probability measures, defined with the free unitary Brownian motion but differing from t-freeness of [5] that was defined in terms of the liberation process of Voiculescu [67]. In contrast to [20], our main tool is a fine use of Makeenko–Migdal equations, proving uniqueness of their solution under suitable assumptions, and generalising the arguments of [21, 33].

Information

Type
Probability
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 Makeenko–Migdal deformation near an intersection point.

Figure 1

Figure 2 Desingularisation at a simple intersection point.

Figure 2

Figure 3 In this example, it is impossible to change the area around any intersection point, respecting the constraint of Makeenko–Migdal given in Figure 1, without raising the number of intersection points.

Figure 3

Figure 4 Discrete homotopy towards a loop included in a disc preserving the algebraic area. Faces are labelled by their area. Faces without label have area $0$.

Figure 4

Figure 5 A map embedded in the torus, with $\vert V\vert = 1$, $\vert E_+\vert = 3$ and $\vert F_+\vert = 2$. The edges named a are glued together, and same for the edges named b. There are two positively oriented faces, with respective boundaries $ea^{-1}b$ and $ab^{-1}e^{-1}$; the orientations are represented by the counterclockwise green arrows. Euler’s formula is indeed satisfied.

Figure 5

Figure 6 On the left: a map embedded in the sphere (in plain lines), and its dual map (in dashed lines). On the right: the orientation convention of an edge and its dual. We have $ \underline {e}, \overline {e}\in V=F^{*}$ and $ \underline {e^{*}}, \overline {e^{*}}\in F=V^{*}$.

Figure 6

Figure 7 Two examples of map cuts. In the first line, a genus 2 map is cut along $\ell $ into two genus 1 maps with boundary $\ell $; hence, it is an essential cut. In the second line, a genus 1 map is cut into a genus 1 and a genus 0 maps, with boundary $\ell $. It is therefore not essential.

Figure 7

Figure 8 A representant of the winding number function with $c\in R$, for a loop $\ell $ of null homology, on a map of genus $2$. The loop is drawn in green, and the value on each positively oriented face is displayed on each $2$-cell.

Figure 8

Figure 9 The three main types of transverse simple intersections. In each case, the dotted paths might be arbitrarily complicated and have multiple intersections outside $\{e_1,e_2,e_3,e_4\}$. Only the first case corresponds to a tame loop.

Figure 9

Figure 10 A tame loop in a graph with one vertex and $2$ faces. The value of $\mu _v$ is displayed on each face in blue.

Figure 10

Figure 11 Three representations of a 4-bouquet. From left to right: as a polygon whose sides are identified pairwise (and whose vertices are all identified), as a graph embedded in a surface of genus 2, and as the skeleton of the corresponding CW complex.

Figure 11

Figure 12 On the left: a regular loop with base v in a regular map of genus 1. On the right: its lift on the universal cover, with base $\tilde {v}$. It has a tiling length of 4, as it crosses four times the boundaries of tiles (at the purple crosses).

Figure 12

Figure 13 Discrete homotopy at a left turn of $\ell $ when $g=2$ and $k=7.$ The latter vertex is shown as a green dot; contracted faces are shown in green. The second rim is displayed with dotted lines. A lift $\tilde \ell $ of the initial loop in displayed in plain orange line, while a lift $\tilde \ell '$ of the terminal loop is displayed in dashed red line.

Figure 13

Figure 14 Left: a nested loop. Right: this is not a nested loop.

Figure 14

Figure 15 A marked loop. Its nested part is drawn in blue. There are exactly one central face coloured in blue and one outer face filled with dashed green lines.

Figure 15

Figure 16 Left: A marked loop with the nested part drawn in blue. New edges of the modified regular map are drawn with dashed lines. The union of faces of $F_{stem}$ is a stroke with dashed lines. Right: Pull of the left marked loop along the path of the dual drawn in orange.

Figure 16

Figure 17 Left: A marked loop with the nested part drawn in blue. The chosen moving edge is drawn in orange. Right: n-twist of the left marked loop, with $n=-2$ and the chosen moving edge. The new moving edge is displayed in orange.

Figure 17

Figure 18 Faces are labelled by their area. Faces without label have area $0$. In the left figure, $\pm $ symbols stand for the area change involved in the decomposition of $\delta _aF$ as a signed sum of Makeenko–Migdal vectors at four vertices acting on $\psi .$ Here, only the vertex highlighted with a red circle yields a desingularisation with only null-homology loops.

Figure 18

Figure 19 Example of a n-left twist with $n=3.$ We consider here $k=2$; the area of $F_2$ needs to be ‘moved’ into $f_1$. We have $a(f_1)=a(f_2)=a(f_3)=0=a'(f_1)=a'(f_2).$ For all $0 define $b_2$ setting $b_2(f_1)=b(F_1)+(t-s)a'(F_1)$ and $0$ for other faces. Denote $a_{s,t}=sa+(t-s)a'+b$ and $\tilde a_{s,t}=sa+b_2$. On the one hand, for any face $f\not \in F_1$, $a_{s,t}(f)=a^{\prime }_{s,t}(f)$ while $a_{s,t}(F_1)=a^{\prime }_{s,t}(F_1)$; therefore, $\Psi _{\ell _2}^N(a_{s,t})=\Psi _{\ell _2}^N(\tilde a_{s,t}).$ On the other hand, $\tilde a_{s,t}(F_2)=0$ so that $\Psi _{\ell _2}^N(\tilde a_{s,t})=\Psi _\ell ^N(\tilde a_{s,t}).$