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Related papers: Modified Braid Equations for SO_q (3) and noncommu…

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Modified braid equations satisfied by generalized ${\hat R}$ matrices (for a {\em given} set of group relations obeyed by the elements of ${\sf T}$ matrices ) are constructed for q-deformed quantum groups $GL_q (N), SO_q (N)$ and $Sp_q (N)$…

Quantum Algebra · Mathematics 2015-06-26 A. Chakrabarti , R. Chakrabarti

With the known group relations for the elements $(a,b,c,d)$ of a quantum matrix $T$ as input a general solution of the $RTT$ relations is sought without imposing the Yang - Baxter constraint for $R$ or the braid equation for $\hat{R} = PR$.…

Quantum Algebra · Mathematics 2015-06-26 A. Chakrabarti

The Modified Tetrahedron Equation (MTE) with affine Weyl quantum variables at N-th root of unity is solved by a rational mapping operator which is obtained from the solution of a linear problem. We show that the solutions can be…

Exactly Solvable and Integrable Systems · Physics 2008-11-26 G. von Gehlen , S. Pakuliak , S. Sergeev

Various properties of a class of braid matrices, presented before, are studied considering $N^2 \times N^2 (N=3,4,...)$ vector representations for two subclasses. For $q=1$ the matrices are nontrivial. Triangularity $(\hat R^2 =I)$…

Quantum Algebra · Mathematics 2009-11-10 A. Chakrabarti

This work presents an unfitted boundary algebraic equation (BAE) method for solving three-dimensional elliptic partial differential equations on complex geometries using finite difference on structured meshes. We demonstrate that replacing…

Numerical Analysis · Mathematics 2025-02-11 Qing Xia

There is a need for covariant solutions of bound state equations in order to construct realistic QCD based models of mesons and baryons. Furthermore, we ideally need to know the structure of these bound states in all kinematical regimes,…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. G. Williams , K. Kusaka , K. M. Simpson

A large class of 3-dimensional integrable lattice spin models is constructed. The starting point is an invertible canonical mapping operator in the space of a triple Weyl algebra. This operator is derived postulating a current branching…

Exactly Solvable and Integrable Systems · Physics 2009-11-10 G. von Gehlen , S. Pakuliak , S. Sergeev

We present most general one-parametric solutions of the Yang-Baxter equations (YBE) for one spectral parameter dependent $R_{ij}(u)$-matrices of the six- and eight-vertex models, where the only constraint is the particle number conservation…

Mathematical Physics · Physics 2013-05-09 Sh. Khachatryan , A. Sedrakyan

We introduce a new Baxterisation for R-matrices that depend separately on two spectral parameters. The Baxterisation is based on a new algebra, close to but different from the braid group. This allows us to recover the R-matrix of the…

Mathematical Physics · Physics 2017-01-12 N. Crampe , L. Frappat , E. Ragoucy , M. Vanicat

A bijective map $r: X^2 \longrightarrow X^2$, where $X = \{x_1, ..., x_n \}$ is a finite set, is called a \emph{set-theoretic solution of the Yang-Baxter equation} (YBE) if the braid relation $r_{12}r_{23}r_{12} = r_{23}r_{12}r_{23}$ holds…

Quantum Algebra · Mathematics 2015-06-26 Tatiana Gateva-Ivanova

In this paper we discuss representations of the Birman-Wenzl-Murakami algebra as well as of its dilute extension containing several free parameters. These representations are based on superalgebras and their baxterizations permit us to…

Exactly Solvable and Integrable Systems · Physics 2015-06-26 W. Galleas , M. J. Martins

We formulate the algebraic Bethe ansatz solution of the SU(N) vertex models with rather general non-diagonal toroidal boundary conditions. The reference states needed in the Bethe ansatz construction are found by performing gauge…

Exactly Solvable and Integrable Systems · Physics 2015-06-26 G. A. P. Ribeiro , M. J. Martins , W. Galleas

In the continuity of our previous paper arXiv:1509.05516, we define three new algebras, $A_{n}(a,b,c)$, $B_{n}$ and $C_{n}$, that are close to the braid algebra. They allow to build solutions to the braided Yang-Baxter equation with…

Mathematical Physics · Physics 2025-03-13 N. Crampe , E. Ragoucy , M. Vanicat

A unified approach is applied in the consideration of the multi-parametric (colored) Yang-Baxter equations (YBE) and the usual YBE with two-parametric R-matrices, relying on the existence of the arbitrary functions in the general solutions.…

Mathematical Physics · Physics 2015-06-17 Sh. Khachatryan

Recently, the Shifted Boundary Method (SBM) was proposed within the class of unfitted (or immersed, or embedded) finite element methods. By reformulating the original boundary value problem over a surrogate (approximate) computational…

Numerical Analysis · Mathematics 2023-07-19 Nabil M. Atallah , Claudio Canuto , Guglielmo Scovazzi

A class of $(2n)^2\times(2n)^2$ multiparameter braid matrices are presented for all $n$ $(n\geq 1)$. Apart from the spectral parameter $\theta$, they depend on $2n^2$ free parameters $m_{ij}^{(\pm)}$, $i,j=1,...,n$. For real parameters the…

Quantum Algebra · Mathematics 2008-11-26 B. Abdesselam , A. Chakrabarti , V. K. Dobrev , S. G. Mihov

We introduce the free quantum noncommutative fields as described by braided tensor products. The multiplication of such fields is decomposed into three operations, describing the multiplication in the algebra M of functions on…

High Energy Physics - Theory · Physics 2015-05-28 Jerzy Lukierski , Mariusz Woronowicz

A fundamental open problem in algebraic combinatorics is to find a positive combinatorial formula for Kronecker coefficients, which are multiplicities of the decomposition of the tensor product of two \S_r-irreducibles into irreducibles.…

Representation Theory · Mathematics 2014-05-19 Jonah Blasiak

We argue that one can relax the requirements of the non-associative three-algebras recently used in constructing D=3, N=8 superconformal field theories, and introduce the notion of ``relaxed three-algebras''. We present a specific…

High Energy Physics - Theory · Physics 2009-05-05 M. Ali-Akbari , M. M. Sheikh-Jabbari , J. Simon

Braid matrices $\hat{R}(\theta)$, corresponding to vector representations, are spectrally decomposed obtaining a ratio $f_{i}(\theta)/f_{i}(-\theta)$ for the coefficient of each projector $P_{i}$ appearing in the decomposition. This…

Quantum Algebra · Mathematics 2015-06-26 A. Chakrabarti
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