This paper studied the construction for quantum code with parameters ((n, K, d)), by use of an n-variable logic function with APC distance d' >= 2 over F-p. We discussed the parameters of the constructed quantu...
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(纸本)9780769538174
This paper studied the construction for quantum code with parameters ((n, K, d)), by use of an n-variable logic function with APC distance d' >= 2 over F-p. We discussed the parameters of the constructed quantum codes, then obtained d <= d' and the maximal K for all d = d'-k, 0 <= k <= d'-2. It was also discussed the basic states and the equivalent conditions of meeting quantum Singleton bound in this paper. With our result, for a given function wit APC distance d' >= 2, we can construct quantum codes with the minimum distance d = d'-k for all 0 <= k <= d' - 2 and presented the basic states of the constructed codes.
The construction of an infinite number of nonstabilizer codes of Clifford type was given for the first tithe by the authors. However, the method of construction was restricted to encoding from odd prime p-level quantu...
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The construction of an infinite number of nonstabilizer codes of Clifford type was given for the first tithe by the authors. However, the method of construction was restricted to encoding from odd prime p-level quantum states to 2p-level states. In this paper, the result is extended to the construction of nonstabilizer-type quantum codes which encodequantum states of arbitrary odd 2j+1-level to quantum states of 2h(2j+1)-level, where h are mutually prime 2j+1. (C) 2006 Wiley Periodicals, Inc.
We provide a new construction of quantum codes that enables integration of a broader class of classical codes into the mathematical framework of quantum stabilizer codes. Next, we present new connections between twist...
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We provide a new construction of quantum codes that enables integration of a broader class of classical codes into the mathematical framework of quantum stabilizer codes. Next, we present new connections between twisted codes and linear cyclic codes and provide novel bounds for the minimum distance of twisted codes. We show that classical tools such as the Hartmann-Tzeng minimum distance bound are applicable to twisted codes. This enabled us to discover five new infinite families and many other examples of record-breaking, and sometimes optimal, binary quantum codes. We also discuss the role of the gamma\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\gamma $$\end{document} value on the parameters of twisted codes and present new results regarding the construction of twisted codes with different gamma\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\gamma $$\end{document} values but identical parameters. Finally, we list many new record-breaking binary quantum codes that we obtained from additive twisted, linear cyclic, and constacyclic codes.
Classical locally recoverable codes (LRCs) have become indispensable in distributed storage systems. They provide efficient recovery in terms of localized errors. quantum LRCs have very recently been introduced for th...
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Classical locally recoverable codes (LRCs) have become indispensable in distributed storage systems. They provide efficient recovery in terms of localized errors. quantum LRCs have very recently been introduced for their potential application in quantum data storage. In this paper, we use classical LRCs to investigate quantum LRCs. We prove that the parameters of quantum LRCs are bounded by their classical counterparts. We deduce bounds on the parameters of quantum LRCs from bounds on the parameters of the classical ones. We establish a characterization of optimal pure quantum LRCs based on classical codes with specific properties. Using well-crafted classical LRCs as ingredients in the construction of quantum CSS codes, we offer the first construction of several families of optimal pure quantum LRCs.
Sufficient and necessary conditions for Hermitian(1 + λu)-constacyclic self-orthogonal codes over F;m +uF;m are obtained, where λ is a unit of F;m +uF;*** on this, a new method for the construction of p;ary quantu...
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Sufficient and necessary conditions for Hermitian(1 + λu)-constacyclic self-orthogonal codes over F;m +uF;m are obtained, where λ is a unit of F;m +uF;*** on this, a new method for the construction of p;ary quantum codes from the obtained Hermitian(1 + λu)-constacyclic self-orthogonal codes over F;m +uF;m is *** an example, [[p;-1, p;-2d + 1, d]];m quantum MDS codes are constructed for 1 ≤ d ≤(p;+ 1)/2 and p ≠ 2, as well as some other quantum codes.
In this article, for any odd prime p, we construct the quantum codes over Fp by using the cyclic codes of length n over R=Fp[u,v,w]/u2-1,v2-1,w2-1,uv-vu,vw-wv,wu-uw. We obtain the self-orthogonal properties of cyclic ...
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In this article, for any odd prime p, we construct the quantum codes over Fp by using the cyclic codes of length n over R=Fp[u,v,w]/u2-1,v2-1,w2-1,uv-vu,vw-wv,wu-uw. We obtain the self-orthogonal properties of cyclic codes over R and as an application, present some new quantum codes.
One central theme in quantum error-correction is to construct quantum codes that have a relatively large minimum distance. In this paper, we first present a construction of classical linear codes based on certain clas...
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One central theme in quantum error-correction is to construct quantum codes that have a relatively large minimum distance. In this paper, we first present a construction of classical linear codes based on certain classes of polynomials. Through these classical linear codes, we are able to obtain some new quantum codes. It turns out that some of the quantum codes exhibited here have better parameters than the ones available in the literature.
In this paper, we present quantum codes via algebraic geometry codes on norm-trace curves. We provide a lower bound of minimum Hamming distance for q-ary quantum code, where q = 2(e) (e >= 3). In order to get this,...
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In this paper, we present quantum codes via algebraic geometry codes on norm-trace curves. We provide a lower bound of minimum Hamming distance for q-ary quantum code, where q = 2(e) (e >= 3). In order to get this, we determine Feng-Rao function values for the elements of Weierstrass semigroups on norm-trace curves. We present the order-bound on the minimum Hamming distance of one-point dual codes. Furthermore, we give a certain increasing sequence of one-point codes on norm-trace curves. We construct quantum codes from the sequence of one-point codes via the CSS construction. These give a better lower bound on the minimum Hamming distance of q-ary quantum code than some previous results.
For an odd prime p and a positive integer m, let F-pm be the finite field with p(m) elements. For D-1 = {d is an element of F*(pm) : Tr-e(m) (d(2)) = 0) = {d(1), d(2), ..., d(n))(say) and D-2 = {d is an element of F-p...
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For an odd prime p and a positive integer m, let F-pm be the finite field with p(m) elements. For D-1 = {d is an element of F*(pm) : Tr-e(m) (d(2)) = 0) = {d(1), d(2), ..., d(n))(say) and D-2 = {d is an element of F-pm : d(k) = 1} {k = p(l) - 1 for a divisor l of m), first we define classical linear codes by C-D(1) = {(Tr-e(m) (ad(1)), Tr-e(m) (ad(2)), ..., Tr-e(m) (ad(n))) : a is an element of F-pm};(C) over bar (D1) = {(u + Tr-e(m)(ad(1)), u + Tr-e(m) (ad2), ..., u + Tr-e(m) (ad(n))) : a is an element of F-pm, u is an element of F-pe} C-D(2) = {(Tr-e(m) (ad(1)), ..., Tr-e(m)(ad(k)), u + Tr-e(m) (ad(1)), ..., u +Tr-e(m) (ad(k))) : a is an element of F-pm, u is an element of F-pe}, where Tr-e(m) denotes the trace function from F-pm onto F-pe and e is a divisor of m. Then we determine weight distribution of the code (C) over bar (D1) \C-D(1) and construct quantum codes from the codes C-D1 and (C) over bar (D1) based on CSS code construction. Finally, we construct quantum code from the code C-D(2) and show that the code obtained from C-D2 is MDS if and only if s = 1, where s = m/e.
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