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Abstract

Centraliser codes are codes of length n2n2 defined as centralisers of a given matrix A of order n. Their dimension, parity-check matrices, syndromes, and automorphism groups are investigated. A lower bound on the dimension is n, the order of A. This bound is met when the minimal polynomial is equal to the annihilator, i.e. for so-called cyclic (a.k.a. non-derogatory) matrices. If, furthermore, the matrix is separable and the adjacency matrix of a graph, the automorphism group of that graph is shown to be abelian and to be even trivial if the alphabet field is of even characteristic.

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... It is easy to see that C F q (A, γ) is a linear subspace of the matrix space F n×n q over F q , and hence C F q (A, γ) is a linear code, called a twisted centralizer code, whose elements (i.e., codewords) are matrices, that can be viewed as vectors of length n 2 , by reading them column-by-column. The notion of twisted centralizer codes is a generalization of centralizer codes [1], since a centralizer code is a twisted centralizer code, twisted by 1 = γ ∈ F q . ...
... Regarding twisted centralizer codes, so far, Alahmadi et al. ( [2], [3]) have determined an upper and lower bound for the dimension, and obtained the exact values of the dimension only for cyclic or diagonalizable matrices A. Moreover, they [1] also state, "In general determining the dimension of such a code 2 given A is a non-trivial problem, and we were only able to give a spectral characterization of the dimension over an extension of the base field". 3 Continuing and improving the results obtained by Alahmadi et al. ...
... Namely, a twisted centralizer code with γ = 1. 3[1], p. 76. ...
Article
Alahmadi et al. (2017) [2] introduced the notion of twisted centralizer codes, CFq(A,γ), defined asCFq(A,γ)={X∈Fqn×n:AX=γXA}, for A∈Fqn×n, and γ∈Fq. Moreover, Alahmadi et al. (2017) [3] also investigated the dimension of such codes and obtained upper and lower bounds for the dimension, and the exact value of the dimension only for cyclic or diagonalizable matrices A. Generalizing and sharpening Alahmadi et al.'s results, in this paper, we determine the exact value of the dimension as well as provide an algorithm to construct an explicit basis of the codes for any given matrix A.
... If |I| = 1 we write C(A, B) instead of C({A}, {B}). Centralizer codes [1] have the form C(A, A) and twisted centralizer codes [2,3] have the form C(A, αA) where A ∈ F r×s and α ∈ F . Intertwining codes C(A, B) are more general still, so our dimension formula (Theorem 2.8) has particularly wide applicability. ...
... Our construction uses k linearly independent 1 × s row vectors u 1 , . . . , u k which give the first k rows of S ∈ GL(s, F ), and k linearly independent r × 1 column vectors v (1) , . . . , v (k) which give the first k columns of R −1 ∈ GL(r, F ). ...
... Since |F | 3, we may choose γ ∈ F \ {1, 1 − s}. As v (1) , . . . , v (k) are linearly independent, there exists an r × r invertible matrix, which we call R −1 , whose first k columns are v (1) , . . . ...
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The barrier of the family of centralizer codes is the length which is always n². In our paper, we have taken codes generated by two matrices A and C of different orders n × n and k × k respectively. This family of codes are termed as intertwining codes and denoted by . Specialty of this code is the length nk which gives a new approach to characterize family of centralizer codes. In this article, we show an upper bound on the minimum distance of intertwining codes. Besides, we establish two decoding methods which can be fitted to intertwining codes as well as for any linear codes. Moreover, we have shown a condition for which a linear code can be represented as an intertwining code.
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Given an n×nn\times n matrix A over a field F and a scalar aFa\in F, we consider the linear codes C(A,a):={BFn×nAB=aBA}C(A,a):=\{B\in F^{n\times n}\mid \,AB=aBA\} of length n2n^2. We call C(A,a) a twisted centralizer code. We investigate properties of these codes including their dimensions, minimum distances, parity-check matrices, syndromes, and automorphism groups. The minimal distance of a centralizer code (when a=1) is at most n, however for a0,1a\ne 0,1 the minimal distance can be much larger, as large as n2n^2.
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Given a field F, a scalar λF\lambda\in F and a matrix AFn×nA\in F^{n\times n}, the twisted centralizer code CF(A,λ):={BFn×nABλBA=0}C_F(A,\lambda):=\{B\in F^{n\times n}\mid AB-\lambda BA=0\} is a linear code of length n2n^2. When A is cyclic and λ0\lambda\ne0 we prove that dimCF(A,λ)=deg(gcd(cA(t),λncA(λ1t)))\dim C_F(A,\lambda)=\mathrm{deg}(\gcd(c_A(t),\lambda^n c_A(\lambda^{-1}t))) where cA(t)c_A(t) denotes the characteristic polynomial of A. We also show how CF(A,λ)C_F(A,\lambda) decomposes, and we estimate the probability that CF(A,λ)C_F(A,\lambda) is nonzero when F|F| is finite. Finally, we prove dimCF(A,λ)n2/2\dim C_F(A,\lambda)\leqslant n^2/2 for λ∉{0,1}\lambda\not\in\{0,1\} and `almost all' matrices A.
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Let R be a non-commutative ring. The commuting graph of R denoted by Γ(R), is a graph with vertex set R⧹Z(R), and two distinct vertices a and b are adjacent if ab = ba. In this paper we investigate some properties of Γ(R), whenever R is a finite semisimple ring. For any finite field F, we obtain minimum degree, maximum degree and clique number of Γ(Mn(F)). Also it is shown that for any two finite semisimple rings R and S, if Γ(R) ≃ Γ(S), then there are commutative semisimple rings R1 and S1 and semisimple ring T such that R ≃ T × R1, S ≃ T × S1 and ∣R1∣ = ∣S1∣.
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This is a substantial revision of a much-quoted monograph, first published in 1974. The structure is unchanged, but the text has been clarified and the notation brought into line with current practice. A large number of 'Additional Results' are included at the end of each chapter, thereby covering most of the major advances in the last twenty years. Professor Biggs' basic aim remains to express properties of graphs in algebraic terms, then to deduce theorems about them. In the first part, he tackles the applications of linear algebra and matrix theory to the study of graphs; algebraic constructions such as adjacency matrix and the incidence matrix and their applications are discussed in depth. There follows an extensive account of the theory of chromatic polynomials, a subject which has strong links with the 'interaction models' studied in theoretical physics, and the theory of knots. The last part deals with symmetry and regularity properties. Here there are important connections with other branches of algebraic combinatorics and group theory. This new and enlarged edition this will be essential reading for a wide range of mathematicians, computer scientists and theoretical physicists.
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The Kronecker product
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B.J. Broxson, The Kronecker product, PhD dissertation, University of North Florida, 2006.
Online tables of linear codes
  • M Grassl
M. Grassl, Online tables of linear codes, www.codetables.de.
An overview of the recent progress on matrix multiplication
  • V V Williams
V.V. Williams, An overview of the recent progress on matrix multiplication, http://theory.stanford. edu/~virgi/sigactcolumn.pdf, 2012, ACM SIGACT News.