Aspects of a new class of braid matrices: Roots of unity and hyperelliptic q for triangularity, L-algebra, link-invariants, noncommutative spaces
Author(s) -
Amlan Chakrabarti
Publication year - 2005
Publication title -
journal of mathematical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.708
H-Index - 119
eISSN - 1089-7658
pISSN - 0022-2488
DOI - 10.1063/1.1924701
Subject(s) - noncommutative geometry , mathematics , braid , root of unity , commutative property , iterated function , pure mathematics , matrix (chemical analysis) , polynomial , algebra over a field , discrete mathematics , mathematical analysis , composite material , quantum , materials science , physics , quantum mechanics
Various properties of a class of braid matrices, presented before, arestudied considering $N^2 \times N^2 (N=3,4,...)$ vector representations for twosubclasses. For $q=1$ the matrices are nontrivial. Triangularity $(\hat R^2=I)$ corresponds to polynomial equations for $q$, the solutions ranging fromroots of unity to hyperelliptic functions. The algebras of $L-$ operators arestudied. As a crucial feature one obtains $2N$ central, group-like, homogenousquadratic functions of $L_{ij}$ constrained to equality among themselves by the$RLL$ equations. They are studied in detail for $N =3$ and are proportional to$I$ for the fundamental $3\times3$ representation and hence for all iteratedcoproducts. The implications are analysed through a detailed study of the$9\times 9$ representation for N=3. The Turaev construction for link invariantsis adapted to our class. A skein relation is obtained. Noncommutative spacesassociated to our class of $\hat R$ are constructed. The transfer matrix map isimplemented, with the N=3 case as example, for an iterated construction ofnoncommutative coordinates starting from an $(N-1)$ dimensional commutativebase space. Further possibilities, such as multistate statistical models, areindicated.Comment: 34 pages, pape
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