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Related papers: Minimal model fusion rules from 2-groups

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Building upon the Jones-Wassermann program of studying Conformal Field Theory using operator algebraic tools, and the work of A. Wassermann on the loop group of LSU(n) (Invent. Math. 133 (1998), 467-538), we give a solution to the problem…

Operator Algebras · Mathematics 2009-09-29 V. Toledano-Laredo

From the defining exchange relations of the A_{q,p}(gl_{N}) elliptic quantum algebra, we construct subalgebras which can be characterized as q-deformed W_N algebras. The consistency conditions relating the parameters p,q,N and the central…

Quantum Algebra · Mathematics 2008-11-26 D. Arnaudon , J. Avan , L. Frappat , E. Ragoucy , J. Shiraishi

Fusion is defined for arbitrary lowest weight representations of $W$-algebras, without assuming rationality. Explicit algorithms are given. A category of quasirational representations is defined and shown to be stable under fusion.…

High Energy Physics - Theory · Physics 2011-07-18 Werner Nahm

We characterise the minimum weight codewords of the $p$-ary linear code of intersecting lines in ${\rm PG}(3,q)$, $q=p^h$, $q\geq19$, $p$ prime, $h\geq 1$. If $q$ is even, the minimum weight equals $q^3+q^2+q+1$. If $q$ is odd, the minimum…

Combinatorics · Mathematics 2026-01-28 Sam Adriaensen , Robin Simoens , Leo Storme

We consider the W-extended logarithmic minimal model WLM(p,p'). As in the rational minimal models, the so-called fundamental fusion algebra of WLM(p,p') is described by a simple graph fusion algebra. The fusion matrices in the regular…

High Energy Physics - Theory · Physics 2010-05-07 Jorgen Rasmussen

A natural construction of the logarithmic extension of the M(2,p) minimal models is presented, which generalises our previous model [0708.0802] of percolation (p=3). Its key aspect is the replacement of the minimal model irreducible modules…

High Energy Physics - Theory · Physics 2008-11-26 Pierre Mathieu , David Ridout

We construct new Yang-Baxter integrable boundary conditions in the lattice approach to the logarithmic minimal model WLM(1,p) giving rise to reducible yet indecomposable representations of rank 1 in the continuum scaling limit. We interpret…

High Energy Physics - Theory · Physics 2011-09-16 Jorgen Rasmussen

The initial classification of fusion rules have shown that rational conformal field theory is very limited. In this paper we study the fusion rules of extend ed current algebras. Explicit formulas are given for the S matrix and the fusion…

High Energy Physics - Theory · Physics 2009-10-30 Ernest Baver , Doron Gepner

We glue four refined topological vertices to obtain the building block of 5D $U(2)$ quiver instanton partition functions. We take the 4D limit of the result to obtain the building block of 4D instanton partition functions which, using the…

High Energy Physics - Theory · Physics 2015-08-07 Omar Foda , Jian-Feng Wu

The quon algebra is an approach to particle statistics in order to provide a theory in which the Pauli exclusion principle and Bose statistics are violated by a small amount. The quons are particles whose annihilation and creation operators…

Combinatorics · Mathematics 2018-07-09 Hery Randriamaro

Since Ref. [1] shows the emergence of non-Abelian fusion rules in some examples of a class of Abelian models, but does not prove whether these rules also exist in other cases, the purpose of this paper is to present such proof emphasizing…

Quantum Physics · Physics 2025-11-21 M. F. Araujo de Resende , J. P. Ibieta Jimenez , J. Lorca Espiro

We classify minimal complex surfaces of general type with $p_g=q=3$. More precisely, we show that such a surface is either the symmetric product of a curve of genus 3 or a free $\Z_2-$quotient of the product of a curve of genus 2 and a…

Algebraic Geometry · Mathematics 2007-05-23 Christopher D. Hacon , Rita Pardini

We continue the study of null-vector equations in relation with partition functions of (systems of) Schramm-Loewner Evolutions (SLEs) by considering the question of fusion. Starting from $n$ commuting SLEs seeded at distinct points, the…

Probability · Mathematics 2015-06-18 Julien Dubédat

The product-group unification is a model of unified theories, in which masslessness of the two Higgs doublets and absence of dimension-five proton decay are guaranteed by a symmetry. It is based on SU(5) x U(N) (N=2,3) gauge group. It is…

High Energy Physics - Phenomenology · Physics 2014-11-17 Taizan Watari , T. Yanagida

An analog of the minimal unitary series representations for the deformed Virasoro algebra is constructed using vertex operators of the quantum affine algebra $U_q(\hat{sl}_2)$. A similar construction is proposed for the elliptic algebra…

q-alg · Mathematics 2008-02-03 Michio Jimbo , Jun'ichi Shiraishi

We provide polynomial upper bounds for the minimal sizes of distal cell decompositions in several kinds of distal structures, particularly weakly $o$-minimal and $P$-minimal structures. The bound in general weakly $o$-minimal structures…

Logic · Mathematics 2026-02-11 Aaron Anderson

Most of the analysis of composite Higgs have focussed on the Minimal Composite Higgs Model, based on the coset SO(5)$\times$U(1)$_X$/SO(4)$\times$U(1)$_X$. We consider a model based on the coset of simple groups SO(7)/SO(6), with…

High Energy Physics - Phenomenology · Physics 2020-01-29 Leandro Da Rold , Alejo N. Rossia

Recently, a relation between Schreier-type sets and Tur\'{a}n graphs was discovered. In this note, we give a combinatorial proof and obtain a generalization of the relation. Specifically, for $p, q\ge 1$, let $$\mathcal{A}_q :=…

Combinatorics · Mathematics 2022-05-18 Hung Viet Chu

Inspired by 5d supersymmetric Yang-Mills theories placed on the compact space $\mathbb{S}^5$, we propose an intriguing algebraic construction for the $q$-Virasoro algebra. We show that, when multiple $q$-Virasoro "chiral" sectors have to be…

High Energy Physics - Theory · Physics 2017-11-16 Fabrizio Nieri , Yiwen Pan , Maxim Zabzine

Let A, B and S be three subsets of a finite Abelian group G. The restricted sumset of A and B with respect to S is defined as A\wedge^{S} B= {a+b: a in A, b in B and a-b not in S}. Let L_S=max_{z in G}| {(x,y): x,y in G, x+y=z and x-y in…

Number Theory · Mathematics 2013-05-14 Yahya ould Hamidoune , Susana C. Lopez , Alain Plagne