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Although symmetry methods and analysis are a necessary ingredient in every physicist's toolkit, rather less use has been made of combinatorial methods. One exception is in the realm of Statistical Physics, where the calculation of the…

Quantum Physics · Physics 2007-05-23 Allan I. Solomon , Pawel Blasiak , Gerard Duchamp , Andrzej Horzela , Karol A. Penson

We consider the problem of finding orthogonal projections $P$ of a rank $r$ that give rise to representations of the Hecke algebra $H_N(q)$ in which the generators of the algebra act locally on the $N$-th tensor power of the space ${\mathbb…

Representation Theory · Mathematics 2023-01-04 Andrei Bytsko

In the paper we give consecutive description of functional methods of quantum field theory for systems of interacting q-particles. These particles obey exotic statistics and appear in many problems of condensed matter physics, magnetism and…

High Energy Physics - Theory · Physics 2009-10-30 K. N. Ilinski , G. V. Kalinin , A. S. Stepanenko

In this paper, we initiate a study into the explicit construction of irreducible representations of the Hecke algebra $H_n(q)$ of type $A_{n-1}$ in the non-generic case where $q$ is a root of unity. The approach is via the Specht modules of…

q-alg · Mathematics 2009-10-28 T. A. Welsh

We revisit a formula for the number of plane partitions due to Almkvist. Using the circle method, we provide modifications to his formula along with estimates of the errors. We show that the improved formula continues to be an asymptotic…

Number Theory · Mathematics 2014-07-30 Suresh Govindarajan , Naveen S. Prabhakar

This is the second of a series of two papers devoted to the partition function realization of Wilson surfaces in strict higher gauge theory. A higher 2--dimensional counterpart of the topological coadjoint orbit quantum mechanical model…

High Energy Physics - Theory · Physics 2023-01-25 Roberto Zucchini

Starting from the defining transformations of complex matrices for the SO(4) group, we construct the fundamental representation and the tensor and spinor representations of the group SO(4). Given the commutation relations for the…

General Relativity and Quantum Cosmology · Physics 2015-06-25 M. Lorente , P. Kramer

We present a detailed algorithm to construct symbolic encodings for chaotic attractors of three-dimensional flows. It is based on a topological analysis of unstable periodic orbits embedded in the attractor and follows the approach proposed…

chao-dyn · Physics 2009-10-31 Jerome Plumecoq , Marc Lefranc

We consider the Potts model in a magnetic field on an arbitrary graph $G$. Using a formula of F. Y. Wu for the partition function $Z$ of this model as a sum over spanning subgraphs of $G$, we prove some properties of $Z$ concerning…

Statistical Mechanics · Physics 2015-05-13 Shu-Chiuan Chang , Robert Shrock

States in quantum field theory (QFT) are represented by many-particle wave functions, such that a state describing n particles depends on n spacetime positions. Since a general state is a superposition of states with different numbers of…

High Energy Physics - Theory · Physics 2014-11-18 H. Nikolic

We argue that MacMahon representation of Ding-Iohara-Miki (DIM) algebra spanned by plane partitions is closely related to the Hilbert space of a 3d field theory. Using affine matrix model we propose a generalization of Bethe equations…

High Energy Physics - Theory · Physics 2018-06-05 Yegor Zenkevich

We discuss some basic properties of Lie group representations in rigged Hilbert spaces. In particular, we show that a differentiable representation in a rigged Hilbert space may be obtained as the projective limit of a family of continuous…

Mathematical Physics · Physics 2009-11-10 S. Wickramasekara , A. Bohm

The universal enveloping algebra of ${\cal W}_{1+\infty}$ is isomorphic to the affine Yangian of $\mathfrak{gl}_1$. We study the ${\cal N}=2$ supersymmetric version of this correspondence, and identify the full set of defining relations of…

High Energy Physics - Theory · Physics 2018-12-26 Matthias R. Gaberdiel , Wei Li , Cheng Peng

By work of Bringmann, Ono, and Rhoades it is known that the generating function of the $M_2$-rank of partitions without repeated odd parts is the so-called holomorphic part of a certain harmonic Maass form. Here we improve the standing of…

Number Theory · Mathematics 2017-02-10 Chris Jennings-Shaffer

In this paper, we use a branch of polyhedral geometry, Ehrhart theory, to expand our combinatorial understanding of congruences for partition functions. Ehrhart theory allows us to give a new decomposition of partitions, which in turn…

Combinatorics · Mathematics 2015-08-04 Felix Breuer , Dennis Eichhorn , Brandt Kronholm

We present a new group field theory describing 3d Riemannian quantum gravity coupled to matter fields for any choice of spin and mass. The perturbative expansion of the partition function produces fat graphs colored with SU(2) algebraic…

General Relativity and Quantum Cosmology · Physics 2009-11-11 Daniele Oriti , James Ryan

The Ponzano-Regge model of three-dimensional quantum gravity is well-defined when the observables satisfy a certain condition involving the twisted cohomology. In this case, the partition function is defined in terms of the Reidemeister…

General Relativity and Quantum Cosmology · Physics 2007-05-23 John W. Barrett , Ileana Naish-Guzman

The generating function for $p_N(n)$, the number of partitions of $n$ into at most $N$ parts, may be written as a product of $N$ factors. We find the behavior of coefficients in the partial fraction decomposition of this product as $N \to…

Number Theory · Mathematics 2015-07-30 Cormac O'Sullivan

This paper represents one approach to making explicit some of the assumptions and conditions implied in the widespread representation of numbers by composite quantum systems. Any nonempty set and associated operations is a set of natural…

Quantum Physics · Physics 2009-11-06 Paul Benioff

Let A and M be nonempty sets of positive integers. A partition of the positive integer n with parts in A and multiplicities in M is a representation of n in the form n = \sum_{a\in A} m_a a, where m_a is in M U {0} for all a in A, and m_a…

Number Theory · Mathematics 2013-04-15 Zeljka Ljujic , Melvyn B. Nathanson