Abstract:One formidable difficulty in quantum communication and computation is to protect information-carrying quantum states against undesired interactions with the environment. In past years, many good quantum error-correcting codes had been derived as binary stabilizer codes. Fault-tolerant quantum computation prompted the study of nonbinary quantum codes, but the theory of such codes is not as advanced as that of binary quantum codes. This paper describes the basic theory of stabilizer codes over finite fields. The… Show more
“…The ((11, 3 6 = 729, 3)) 3 code we found, the best possible additive code according to the linear programming bound in [24], falls short by a factor of 3 of saturating the K = 3 7 = 2187 QS bound, and even a nonadditive code based on this graph must have K ≤ 1990 [28].…”
Section: Cycle Graphsmentioning
confidence: 99%
“…It has been extended to cases where D is prime or a prime power in [6,24,30]. In [8] stabilizer codes were extended in a very general fashion to arbitrary D from a point of view that includes encoding.…”
Section: G-additive Codes As Stabilizer Codesmentioning
confidence: 99%
“…• d -Indicates this is not a QS code, but the largest possible additive (graph or other) code for the given n, δ and D, This follows from linear programming bounds in [23] for D = 2 and [24] for D = 3, along with the fact, Sec. III B, that for an additive code, K must be an integer power of D when D is prime.…”
Graph states are generalized from qubits to collections of n qudits of arbitrary dimension D, and simple graphical methods are used to construct both additive and nonadditive, as well as degenerate and nondegenerate, quantum error correcting codes. Codes of distance 2 saturating the quantum Singleton bound for arbitrarily large n and D are constructed using simple graphs, except when n is odd and D is even. Computer searches have produced a number of codes with distances 3 and 4, some previously known and some new. The concept of a stabilizer is extended to general D, and shown to provide a dual representation of an additive graph code.
“…The ((11, 3 6 = 729, 3)) 3 code we found, the best possible additive code according to the linear programming bound in [24], falls short by a factor of 3 of saturating the K = 3 7 = 2187 QS bound, and even a nonadditive code based on this graph must have K ≤ 1990 [28].…”
Section: Cycle Graphsmentioning
confidence: 99%
“…It has been extended to cases where D is prime or a prime power in [6,24,30]. In [8] stabilizer codes were extended in a very general fashion to arbitrary D from a point of view that includes encoding.…”
Section: G-additive Codes As Stabilizer Codesmentioning
confidence: 99%
“…• d -Indicates this is not a QS code, but the largest possible additive (graph or other) code for the given n, δ and D, This follows from linear programming bounds in [23] for D = 2 and [24] for D = 3, along with the fact, Sec. III B, that for an additive code, K must be an integer power of D when D is prime.…”
Graph states are generalized from qubits to collections of n qudits of arbitrary dimension D, and simple graphical methods are used to construct both additive and nonadditive, as well as degenerate and nondegenerate, quantum error correcting codes. Codes of distance 2 saturating the quantum Singleton bound for arbitrarily large n and D are constructed using simple graphs, except when n is odd and D is even. Computer searches have produced a number of codes with distances 3 and 4, some previously known and some new. The concept of a stabilizer is extended to general D, and shown to provide a dual representation of an additive graph code.
“…It is well known that there is a close relationship between cyclotomic cosets and cyclic codes, see [9,11]. This suggests us to use q 2 -cyclotomic cosets of modulo n to characterize BCH codes over F q 2 , see [14].…”
Section: Preliminariesmentioning
confidence: 99%
“…The following Theorem 2.4 (given in [3,11] is well-known for constructing q-ary quantum codes from Hermitian dual containing (or self-orthogonal) codes over…”
Let q = 3l + 2 be a prime power. Maximal designed distances of imprimitive Hermitian dual containing q 2 -ary narrow-sense (NS) BCH codes of length n = (q 6 −1) 3 and n = 3(q 2 − 1)(q 2 + q + 1) are determined. For each given n, non-narrow-sense (NNS) BCH codes which achieve such maximal designed distances are presented, and a series of NS and NNS BCH codes are constructed and their parameters are computed. Consequently, many families of q-ary quantum BCH codes are derived from these BCH codes. Some of these quantum BCH codes constructed from NNS BCH codes have better parameters than those quantum BCH codes available in the literature, and some others are new ones.
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