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Article

Quantum Codes as an Application of Constacyclic Codes

1
Research Group of Algebraic Structures and Applications, Department of Mathematics, Faculty of Science & Arts-Rabigh, King Abdulaziz University, Rabigh 21911, Saudi Arabia
2
Department of Mathematics, Aligarh Muslim University, Aligarh 202002, India
3
Research Group of Algebraic Structures and Applications, Department of Mathematics, Faculty of Science, King Abdulaziz University, Jeddah 21589, Saudi Arabia
4
Director Academics Office, Kaushalya: The Skill University, Ahmedabad 382424, India
5
I2M, (CNRS, Aix-Marseille University, Centrale Marseille), 163 Avenue de Luminy, 13009 Marseilles, France
*
Author to whom correspondence should be addressed.
Submission received: 16 August 2024 /Revised: 14 September 2024 /Accepted: 20 September 2024 /Published: 8 October 2024
(This article belongs to the SectionAlgebra and Number Theory)

Abstract

:
The main focus of this paper is to analyze the algebraic structure of constacyclic codes over the ringR=Fp+w1Fp+w2Fp+w22Fp+w1w2Fp+w1w22Fp, wherew12α2=0,w1w2=w2w1,w23β2w2=0, andα,βFp{0}, for a primep. We begin by introducing a Gray map defined overR, which is associated with an invertible matrix. We demonstrate its advantages over the canonical Gray map through some examples. Finally, we create new and improved quantum codes from constacyclic codes overR using Calderbank–Shore–Steane (CSS) construction.
MSC:
11T71; 94B05; 94B15

    1. Introduction

    In contrast to classical information theory, quantum information theory is a relatively emerging field [1,2,3]. The concept of quantum error-correcting codes (QECCs) was initially introduced by Shor [4] and Steane [5], with a construction method outlined by Calderbank et al. [6]. Subsequently, researchers have explored various approaches to utilize classical error-correcting codes to create new quantum codes (QECCs). The quantum code database remains quite limited when compared to classical block codes. The existing database [7] encompasses finite fields of order up to 9, but it focuses exclusively on QECCs forp=2. Some static tables of quantum codes are available in [8,9], building upon the work in [10]. The online tables [9] might have been overlooked by many researchers.
    The field of quantum error-correcting codes has seen remarkable growth since the initial realization that such codes could safeguard quantum information, which is analogous to how classical error-correcting codes protects classical information. Shor’s [4] pioneering work led to the discovery of the first quantum error-correcting code. In 1998, Calderbank et al. [6] provided a systematic method for constructing quantum codes from classical error-correcting codes. Many researchers have concentrated on using Calderbank–Shor–Steane (CSS) construction to produce quantum codes from linear codes that contain their duals (see [11,12,13,14]).
    Qian et al. [15] initially presented the construction of quantum codes from cyclic codes of odd length over the chain ringF2+uF2, whereu2=0. Subsequently, Kai and Zhu [16] introduced a technique for generating quantum codes from cyclic codes of odd length over the finite chain ringF4+uF4. Qian [17] proposed a novel approach for constructing quantum error-correcting codes from cyclic codes over the finite non-chain ringF2+vF2, wherev2=v of any length. Motivated by this study, Ashraf and Mohammad [18] obtained quantum codes from cyclic codes over the non-chain ringFq+uFq+vFq+uvFq, whereu2=u,v2=v,uv=vu,q=pn, andp is an odd prime.
    Constacyclic codes, a robust extension of cyclic codes over finite non-chain rings, have proven to be a prolific source of new quantum codes. Recent research by coding theorists has explored constacyclic codes extensively. Distinguished investigations include Li et al. [19] overFp+uFp+vFp+uvFp, withu2u=0,v2v=0, anduvvu=0; Ma et al.’s [20] contributions overFp+vFp+v2Fp, withv3=v; and Gao and Wang’s [21] overFp+uFp, whereu2=1. These studies have led to the construction of numerous significantly improved quantum codes, all originating from dual-containing constacyclic codes.
    In light of these developments, it becomes evident that constacyclic codes over finite non-chain rings represent a valuable resource for generating new and better quantum codes. Therefore, this article delves into the exploration of constacyclic codes within the framework of the non-chain ringR=Fp+w1Fp+w2Fp+w22Fp+w1w2Fp+w1w22Fp, wherew12α2=0,w1w2=w2w1,w23β2w2=0, andα,βFp{0}, for a primep. The objective is to find new quantum codes over the finite fieldFp. The article makes two significant contributions:
    • Comprehensive study of the structure of constacyclic codes with the lengthl overR.
    • The construction of better quantum codes concerning their parameters, surpassing those previously documented in the literature.
    • A noteworthy aspect of this research involves the presentation of computational findings [22], highlighting the substantial impact of this work on the development of new quantum codes.

    2. Preliminaries

    LetFp be a finite field of orderp (an odd prime). A subspaceC0 ofFpm is called a linear code of lengthm overFp, and its members are called the codewords. LetR=Fp+w1Fp+w2Fp+w22Fp+w1w2Fp+w1w22Fp, wherew12α2=0,w1w2=w2w1,w23β2w2=0, andα,βFp{0} be a finite commutative ring. Remember that a linear codeC over the ringR of lengthn is essentially anR-submodule of the moduleRn. One can also view an elementc=(c0,c1,,cn1) inC as a polynomialc(z)=c0+c1z++cn1zn1 within the ringR[z]znΛ. A linear codeC is called aΛ-constacyclic code of lengthn overR if and only if it is anR-submodule in the moduleR[z]znΛ. Many researchers have extensively explored constacyclic codes over finite fields and finite commutative Frobenius rings [23,24,25,26,27]. Consider the elements ofR as follows:
    κ1=12αβ2(α+w1)(β2w22),κ2=12αβ2(αw1)(β2w22),κ3=14αβ2(α+w1)(w22βw2),κ4=14αβ2(αw1)(w22βw2),κ5=14αβ2(α+w1)(w22+βw2),κ6=14αβ2(αw1)(w22+βw2).
    We can verify thatκ1+κ2+κ3+κ4+κ5+κ6=1, andκiκj=δij (Kronecker delta) fori,j{1,2,6}. Consequently, the set{κ1,κ2,,κ6} forms a set of non-zero pairwise orthogonal idempotent elements inR. This implies thatR can be expressed as a sum of submodules as follows:
    R=κ1Rκ2Rκ3Rκ4Rκ5Rκ6Rκ1Fpκ2Fpκ3Fpκ4Fpκ5Fpκ6Fp.
    Therefore, any elementr=a+w1b+w2c+w22d+w1w2e+w1w22fR can be uniquely written as
    r=a+w1b+w2c+w22d+w1w2e+w1w22f=κ1a¯+κ2b¯+κ3c¯+κ4d¯+κ5e¯+κ6f¯,
    where
    a¯=a+αb,b¯=aαb,c¯=a+αbβc+β2dαβe+αβ2f,d¯=aαbβc+β2d+αβeαβ2f,e¯=a+αb+βc+β2d+αβe+αβ2f,f¯=aαb+βc+β2dαβeαβ2f,
    are the elements ofFp.
    Suppose thatGLn(Fp) is the group of invertible matrices of ordern overFp and letNGL6(Fp) in such a way thatNNT=kI6, whereNT is the transpose of the matrixN,I6 is the identity matrix of order 6, andkFp{0}. With the above notation, we define a Gray map associated with an invertible matrixN as follows:
    :RFp6suchthat(r):=(a¯,b¯,c¯,d¯,e¯,f¯)N.
    We can extend the Gray map ∇ for each component individually, as follows:
    :RlFp6lsuchthat
    (r0,r1,,rl1)=((a¯0,b¯0,c¯0,d¯0,e¯0,f¯0)N,(a¯1,b¯1,c¯1,d¯1,e¯1,f¯1)N,,(a¯l1,b¯l1,c¯l1,d¯l1,e¯l1,f¯l1)N),
    whereri=κ1ai¯+κ2bi¯+κ3ci¯+κ4di¯+κ5ei¯+κ6fi¯R,fori{0,1,,l1}. Here, we introduce the Lee weight for the vectorrR aswL(r)=wH((r)), wherewL (resp.wH) denotes the Lee weight (resp. the Hamming weight). The Lee weight ofwL(r=(r0,r1,,rl1))=wL(r0)+wL(r1)++wL(rl1) and the Lee distance fromr torRl, is established asdL(r,r)=wL(rr)=wH((rr)). The Lee distancedL(C) for the codeC is defined as follows:
    dL(C)=min{dL(r,r)|rr}.
    It is notable that the Gray map ∇ is a linear map overFp that preserves distances and mapping vectors fromRl toFp6l. Since the Gray map ∇ is bijective, it follows that(C) forms a[6l,k,dH] linear code overFp, wheredL is equal todH.
    The Euclidean inner product of any two vectors,r=(r0,r1,,rl1) andr=(r0,r1,,rl1) inRl is defined asr·r=r0r0+r1r1++rl1rl1. The dual code ofC is formulated asC={rRl|r·r=0rC}. A codeC is called dual-containing ifCC, self-orthogonal ifCC, and self-dual ifC=C.
    Example 1.
    LetR3=F3[w1,w2]w121,w23w2,w1w2w2w1 be a finite commutative non-chain ring. Then, we havew121=(w11)(w1+1) andw23w2=w2(w21)(w2+1). Thus, the orthogonal idempotent elements inR3 are
    κ1=2(1+w1)(1+2w22),κ2=12(1w1)(1w22)=2(1+2w1)(1+2w22),κ3=(1+w1)(w22+2w2),κ4=14(1w1)(w22w2)=(1+2w1)(w22+2w2),κ5=(1+w1)(w22+w2),κ6=14(1w1)(w22+w2)=(1+2w1)(w22+w2),
    whereκ1+κ2+κ3+κ4+κ5+κ6=1. By Chinese Remainder Theorem, we haveR3=κ1R3κ2R3κ3R3κ4R3κ5R3κ6R3κ1F3κ2F3κ3F3κ4F3κ5F3κ6F3. Therefore, any elementr=a+w1b+w2c+w22d+w1w2e+w1w22fR can be expressed as follows:
    r=a+w1b+w2c+w22d+w1w2e+w1w22f=(a+b)κ1+(a+2b)κ2+(a+b+2c+d+2e+f)κ3+(a+2b+2c+d+e+2f)κ4+(a+b+c+d+e+f)κ5+(a+2b+c+d+2e+2f)κ6.
    Hence, the Gray map:R3F36 can be established as follows:
    (r):=(a+b,a+2b,a+b+2c+d+2e+f,a+2b+2c+d+e+2f,a+b+c+d+e+f,a+2b+c+d+2e+2f)N1,
    wherea,b,c,d,e,fF3, andN1GL6(F3), where
    N1=121101112110011211210121222011201112,
    which has the property thatN1N1T=2I6.
    Example 2.
    LetR5=F5[w1,w2]w12α2,w23β2w2,w1w2w2w1 be a finite commutative non-chain ring, whereα=2 andβ=3 are non-zero elements ofF5. Then, we havew12α2=(w12)(w1+2) andw23β2w2=w2(w23)(w2+3). The orthogonal idempotent elements inR5 are as follows:
    κ1=4(2+w1)(1+w22),κ2=12αβ2(αw1)(β2w22)=4(2w1)(1+w22),κ3=2(2+w1)(w223w2),κ4=14αβ2(αw1)(w22βw2)=2(2w1)(w223w2),κ5=2(2+w1)(w22+3w2),κ6=14αβ2(αw1)(w22+βw2)=2(2w1)(w22+3w2),
    whereκ1+κ2+κ3+κ4+κ5+κ6=1. By Chinese Remainder Theorem, we haveR5=κ1R5κ2R5κ3R5κ4R5κ5R5κ6R5κ1F5κ2F5κ3F5κ4F5κ5F5κ6F5. Therefore, any elementr=a+w1b+w2c+w22d+w1w2e+w1w22fR can be expressed as follows:
    r=a+w1b+w2c+w22d+w1w2e+w1w22f=(a+2b)κ1+(a+3b)κ2+(a+2b+2c+4d+4e+3f)κ3+(a+3b+2c+4d+e+2f)κ4+(a+2b+3c+4d+e+3f)κ5+(a+3b+3c+4d+4e+2f)κ6.
    The Gray map:R5F56 can be established as follows:
    (r):=(a+2b,a+3b,a+2b+2c+4d+4e+3f,a+3b+2c+4d+e+2f,a+2b+3c+4d+e+3f,a+3b+3c+4d+4e+2f)N2,
    wherea,b,c,d,e,fF5, andN2GL6(F5), where
    N2=311111131111113111111311111131111113,
    which has the property thatN2N2T=4I6.
    Theorem 1.
    The Gray map:RlFp6l defined in Equation (2) is linear and isometric.
    Proof. 
    To prove that ∇ is a linear map, assume thatz=a1κ1+a2κ2+a3κ3+a4κ4+a5κ5+a6κ6 andy=b1κ1+b2κ2+b3κ3+b4κ4+b5κ5+b6κ6 are any two elements ofR andλ is a non-zero scalar inFp. Then, we have
    (z+y)=(a1+b1,a2+b2,a3+b3,a4+b4,a5+b5,a6+b6)N=[(a1,a2,a3,a4,a5,a6)+(b1,b2,b3,b4,b5,b6)]N=(a1,a2,a3,a4,a5,a6)N+(b1,b2,b3,b4,b5,b6)N=(z)+(y),(λ·z)=(λa1,λa2,λa3,λa4,λa5,λa6)N=λ(a1,a2,a3,a4,a5,a6)N=λ(z).
    This ensures that ∇ is a linear map. To prove that ∇ is an isometry, we shall show that the Lee distance and the Hamming distance of codeC are the same. Asz,yRl, then by definition of the Lee distance, we see that
    dL(z,y)=wtH((zy))=wtH((z)(y))=dH((z),(y)).
    Therefore, the Gray map ∇ is an isometry. □
    Theorem 2.
    Let C be a linear code with parameters[l,k,dL] overR.
    (i)
    Then,(C) is a linear code with parameters[6l,k,dH] overFp, wheredL anddH are the same.
    (ii)
    The image(C) is self-orthogonal overFp, provided C is self-orthogonal overR.
    (iii)
    The image(C) is a dual-containing code overFp, provided C is a dual-containing code overR.
    (iv)
    C is a self-dual code overR if and only if(C) is a self-dual code overFp.
    Proof. 
    (i)
    The proof follows by Theorem 1.
    (ii)
    IfC is self-orthogonal overR. Then, for any codewordsz=(z1,z2,,zl) andy=(y1,y2,,yl) inC, wherezi=a1iκ1+a2iκ2+a3iκ3+a4iκ4+a5iκ5+a6iκ6 andyi=b1iκ1+b2iκ2+b3iκ3+b4iκ4+b5iκ5+b6iκ6 are elements ofR for1il, we havez·y=0. This suggests thataj1bj1+aj2bj2++ajlbjl=0 for1j6. Letz,y(C) be any two elements, then somez,yC exists such thatz=(z) andy=(y), i.e.,
    z=((z1),(z2),,(zl))=((a11,a21,a31,a41,a51,a61)N,(a12,a22,a32,a42,a52,a62)N,,(a1l,a2l,a3l,a4l,a5l,a6l)N),y=((y1),(y2),,(yl))=((b11,b21,b31,b41,b51,b61)N,(b12,b22,b32,b42,b52,b62)N,,(b1l,b2l,b3l,b4l,b5l,b6l)N),
    whereNGL6(Fp) such thatNNT=λI6,λFp{0}. Now, we have
    z·y=(z)·(y)=(z)·(y)T=i=1l(a1i,a2i,a3i,a4i,a5i,a6i)NNT.(b1i,b2i,b3i,b4i,b5i,b6i)=i=1l(a1i,a2i,a3i,a4i,a5i,a6i)λI6.(b1i,b2i,b3i,b4i,b5i,b6i)=i=1lλ(a1ib1i+a2ib2i+a3ib3i+a4ib4i+a5ib5i+a6ib6i)=i=j6λ(aj1bj1+aj2bj2++ajlbjl)=0.
    Thus, we havez·y=(z)·(y)=0 for allz,y(C) ifC is self-orthogonal overR. Hence,(C) is a self-orthogonal code of length6l overFp, providedC is a self-orthogonal code overR.
    (iii)
    Suppose thatCC, then by the linearity of ∇, we have(C)(C). To prove that(C) is dual-containing, it remains to show that(C)=(C). For this, letz=(z1,z2,,zl)C andy=(y1,y2,,yl)C, wherezi=a1iκ1+a2iκ2+a3iκ3+a4iκ4+a5iκ5+a6iκ6 andyi=b1iκ1+b2iκ2+b3iκ3+b4iκ4+b5iκ5+b6iκ6 are elements ofR for1il. Now,x·y=0 gives thataj1bj1+aj2bj2++ajlbjl=0 for1j6. Consider
    (z)=((a11,a21,a31,a41,a51,a61)N,(a12,a22,a32,a42,a52,a62)N,,(a1l,a2l,a3l,a4l,a5l,a6l)N),(y)=((b11,b21,b31,b41,b51,b61)N,(b12,b22,b32,b42,b52,b62)N,,(b1l,b2l,b3l,b4l,b5l,b6l)N),
    Now,(z)·(y)=0 suggests that(y)(C). Thus, we have(C)(C). Contrarily, ∇ is a bijective linear map, so the sizes of(C) and(C) are the same. Thus,(C)=(C). Hence,(C) is a dual-containing code overFp providedC is a dual-containing code overR.
    (iv)
    It follows from part (iii).
    Theorem 3
    ([11]).LetC=κ1C1¯κ2C2¯κ3C3¯κ4C4¯κ5C5¯κ6C6¯ be a linear code overR. Then:
    (i)
    C=κ1C1¯κ2C2¯κ3C3¯κ4C4¯κ5C5¯κ6C6¯;
    (ii)
    C is self-dual overR ifCi¯ are self-dual codes overFp for1i6.
    Here, we define the direct sum and the direct product as defined by Dinh et al. [24] in the following ways:
    D1D2={d1+d2|djDj;j=1,2},
    D1D2={(d1,d2)|djDj;j=1,2}.
    Suppose thatC is a linear code with lengthl overR. Consider the following sets:
    C1¯={a¯Fpl|κ1a¯+κ2b¯+κ3c¯+κ4d¯+κ5e¯+κ6f¯C;forsomeb¯,c¯,d¯,e¯,f¯Fpl};C2¯={b¯Fpl|κ1a¯+κ2b¯+κ3c¯+κ4d¯+κ5e¯+κ6f¯C;forsomea¯,c¯,d¯,e¯,f¯Fpl};C3¯={c¯Fpl|κ1a¯+κ2b¯+κ3c¯+κ4d¯+κ5e¯+κ6f¯C;forsomea¯,b¯,d¯,e¯,f¯Fpl};C4¯={d¯Fpl|κ1a¯+κ2b¯+κ3c¯+κ4d¯+κ5e¯+κ6f¯C;forsomea¯,b¯,c¯,e¯,f¯Fpl};C5¯={e¯Fpl|κ1a¯+κ2b¯+κ3c¯+κ4d¯+κ5e¯+κ6f¯C;forsomea¯,b¯,c¯,d¯,f¯Fpl};C6¯={f¯Fpl|κ1a¯+κ2b¯+κ3c¯+κ4d¯+κ5e¯+κ6f¯C;forsomea¯,b¯,c¯,d¯,e¯Fpl}.
    It can be seen thatCi¯ for1i6 is a linear code with lengthl overFp. Therefore, we can express a linear codeC with lengthl overR asC=κ1C1¯κ2C2¯κ3C3¯κ4C4¯κ5C5¯κ6C6¯. IfGi is the generator matrix ofCi¯ for1i6, then the generator matrix(G) of the Gray image(C) is given as follows:
    (G)=(κ1G1)(κ2G2)(κ3G3)(κ4G4)(κ5G5)(κ6G6).

    3.Λ-Constacyclic Codes overR

    A constacyclic code is an important class of linear error-correcting codes. It is a generalization of cyclic codes, which are themselves a subset of linear codes. Suppose thatΛ=κ1a+κ2b+κ3c+κ4d+κ5e+κ6f is a unit element inR. Then, a linear code C with lengthl overR is called aΛ-constacyclic code if, for any codewordc=(c0,c1,,cl1) inC, it satisfies the property thatωΛ(c)=(Λcl1,c0,,cl2) is again a member ofC. In particular, ifΛ=1, thenΛ-constacyclic codeC becomes a cyclic code, and ifΛ=1, thenC becomes a negacyclic code.
    Lemma 1.
    LetΛ=κ1a+κ2b+κ3c+κ4d+κ5e+κ6fR be a non-zero element. Then, the elementΛR is a unit element inR ifa,b,c,d,e,f are unit elements inFp. Moreover, whenΛR is a unit element, then its inverse is given byΛ1=κ1a1+κ2b1+κ3c1+κ4d1+κ5e1+κ6f1.
    Proof. 
    Suppose thatΛ=κ1a+κ2b+κ3c+κ4d+κ5e+κ6fR is a unit element. Then, an elementΛ1=κ1a1+κ2b1+κ3c1+κ4d1+κ5e1+κ6f1R exists such thatΛΛ1=1. Using the idempotent orthogonality ofκi for1i6, we haveκ1aa1+κ2bb1+κ3cc1+κ4dd1+κ5ee1+κ6ff1=1. Putting the values ofκi for1i6 and comparing the constant term and coefficients ofw1,w2,w22,w1w2,w1w22, we obtain
    aa1+bb1=2,aa1bb1=0,cc1dd1+ee1+ff1=0,cc1+dd1+ee1+ff1=4,cc1+dd1+ee1ff1=0,cc1dd1+ee1ff1=0.
    Solving these equations, we obtainaa1=1,bb1=1,cc1=1,dd1=1,ee1=1, andff1=1. Therefore, we haveΛ1=κ1a1+κ2b1+κ3c1+κ4d1+κ5e1+κ6f1.
    The converse part can be performed in a similar way. □
    Theorem 4.
    LetC=κ1C1¯κ2C2¯κ3C3¯κ4C4¯κ5C5¯κ6C6¯ be a linear code overR andΛ=κ1Λ1+κ2Λ2+κ3Λ3+κ4Λ4+κ5Λ5+κ6Λ6R be a unit element. Then, C is aΛ-constacyclic code overR ifCi¯ is aΛi-constacyclic code for1i6 overFp.
    Proof. 
    Suppose thatC is aΛ-constacyclic code with lengthl overR. Ifc=(r0,r1,,rl1)C, whererj=κ1a1,j+κ2a2,j+κ3a3,j+κ4a4,j+κ5a5,j+κ6a6,j such thatai,jFp for1i6 and0jl1, then we have(ai,0,ai,1,,ai,l1)Ci¯. Thus, theΛ-constacyclic shift ofc isωΛ(c)=(Λrl1,r0,,rl2)C, where
    Λrl1=κ1Λ1a1,l1+κ2Λ2a2,l1+κ3Λ3a3,l1+κ4Λ4a4,l1+κ5Λ5a5,l1+κ6Λ6a6,l1.
    Therefore, we obtainωΛ(c)=i=16κi(Λiai,l1,ai,0,ai,1,,ai,l2)C, which leads to(Λiai,l1,ai,0,ai,1,,ai,l2)Ci¯. Therefore,Ci¯ is aΛi-constacyclic code for1i6 of lengthl overFp.
    Conversely, assume thatCi¯ is aΛi-constacyclic code of lengthl overFp for1i6. Then, for a vectorai¯=(ai,0,ai,1,,ai,l1)Ci¯, we haveωΛi(ai)¯=(Λiai,l1,ai,0,ai,1,,ai,l2)Ci¯. Thus, we have
    i=16κiωΛi(ai)¯=i=16κi(Λiai,l1,ai,0,ai,1,,ai,l2)=(Λrl1,r0,,rl2)=ωΛ(c).
    Therefore, ifCi¯ is aΛi-constacyclic code for1i6 of lengthl overFp, thenC is aΛ-constacyclic code overR. □
    Theorem 5.
    LetC=κ1C1¯κ2C2¯κ3C3¯κ4C4¯κ5C5¯κ6C6¯ be aΛ-constacyclic code overR andpi(z)Fp[z]zlΛi a unique monic polynomial of the lowest degree such thatCi¯=pi(z) andpi(z)|(zlΛi) for1i6. Then,C=p(z), wherep(z)=κ1p1(z)+κ2p2(z)+κ3p3(z)+κ4p4(z)+κ5p5(z)+κ6p6(z) andp(z)|(zlΛ).
    Proof. 
    Suppose thatC=κ1C1¯κ2C2¯κ3C3¯κ4C4¯κ5C5¯κ6C6¯ is aΛ-constacyclic code with lengthl overR, then eachCi¯ is aΛi-constacyclic code overFp for1i6. Therefore,Ci¯Fp[z]zlΛi is a principal ideal generated by a monic polynomialpi(z)Fp[z]zlΛi of lowest degree such thatpi(z)|(zlΛi) for1i6. Thus,κipi(z) are the generator polynomials ofC.
    If we takep(z)=κ1p1(z)+κ2p2(z)+κ3p3(z)+κ4p4(z)+κ5p5(z)+κ6p6(z), thenp(z)C. Furthermore, we see thatκip(z)=κipi(z)p(z) implies thatCp(z). Thus, we conclude thatC=p(z).
    Moreover, we havepi(z)Fp[z]zlΛi such thatpi(z)|(zlΛi). Thus, polynomialsqi(z)Fp[z] exist such that(zlΛi)=pi(z)qi(z) for1i6. Thus, we have
    p(z)(i=16κiqi(z))=i=16κipi(z)qi(z)=κi(zlΛi)=zlΛ.
    Thus, we conclude thatp(z)|(zlΛ). □
    Corollary 1.
    LetC=i=16κiCi¯ be aΛ-constacyclic code overR, andCi¯=pi(z) such thatzlΛi=pi(z)qi(z) for1i6. Then:
    (i)
    C=i=16κiCi¯ is aΛ1-constacyclic code overR;
    (ii)
    C=i=16κiqi*(z), whereqi*(z) is the reciprocal polynomial ofqi(z), which is defined asqi*(z)=zdeg(qi(z))qi(z1) for1i6;
    (iii)
    |C|=pi=16deg(pi(z)).

    4. Dual-ContainingΛ-Constacyclic Codes

    The dual-containing code is a very important class of code for the construction of quantum error-correcting codes.
    Definition 1.
    Suppose that C is aΛ-constacyclic code of length l overR, whereΛ is a unit element ofR. Then, C is said to be dual-containing ifCC.
    Proposition 1.
    Let C be aΛ-constacyclic code overR, whereΛ=κ1Λ1+κ2Λ2+κ3Λ3+κ4Λ4+κ5Λ5+κ6Λ6R. If C is a non-trivial dual-containing code, thenΛi=±1 for1i6, i.e.,Λ{±κ1±κ2±κ3±κ4±κ5±κ6}R.
    Remark 1.
    Suppose that C is aΛ-constacyclic code overR, then from Proposition 1 we conclude that:
    (i)
    IfΛ=1, thenΛi=1 andCi is a cyclic code overFp for1i6.
    (ii)
    IfΛ=1, thenΛi=1 andCi is a negacyclic code overFp for1i6.
    (iii)
    IfΛi=1 andΛj=1, thenCi is a cyclic code, andCj is a negacyclic code overFp for1ij6.
    Example 3.
    Let C be a(w1w22w1w22)-constacyclic code overR, thenΛ1=1 implies thatC1 is a cyclic code, andΛj=1 further implies thatCj is a negacyclic code for2j6 overFp.
    Example 4.
    Let C be a(12w22)-constacyclic code overR, thenΛi=1 implies thatCi is a cyclic code fori=1,2, andΛj=1 further implies thatCj is a negacyclic code for3j6 overFp.
    Example 5.
    Let C be a(112w232w22w1w2+w1w22)-constacyclic code overR, thenΛi=1 implies thatCi is a cyclic code fori=1,2,3, andΛj=1 further implies thatCj is a negacyclic code forj=4,5,6 overFp.
    Lemma 2
    ([6]).LetCj be aΛj-constacyclic code with generator polynomialpj(z) overFp. Then,Cj is a dual-containing code ifznΛj0mod(pj(z)pj*(z)), whereΛj=±1 andpj*(z) is the reciprocal polynomial ofpj(z), forj=1,2,,6.
    Lemma 3.
    Let C be a linear code overR andC be the dual of C. If is a Gray map as defined in Equation (2), then(C)=(C). Moreover, if C is a self-orthogonal (self-dual) code overR, then(C) is a self-orthogonal (resp. self-dual) code overFp.
    Proof. 
    The setK={κ1,κ2,,κ6} forms a basis for 6-dimensional vector spaceR overFp. An elementrR can be uniquely expressed asr=κ1a1+κ2a2+κ3a3+κ4a4+κ5a5+κ6a6, whereaiFp for1i6. Then, we have
    (r)=(a1,a2,a3,a4,a5,a6)M,
    whereMGL6(Fp) such thatMMT=αI6 andαFp{0}. Letz=(z0,z1,,zl1)CRl, wherezj=κ1a1j+κ2a2j+κ3a3j+κ4a4j+κ5a5j+κ6a6jR for0jl1. Then, we havez=κ1a1+κ2a2+κ3a3+κ4a4+κ5a5+κ6a6, whereai=(ai0,ai1,,ail1)Fpl. Suppose thaty=κ1b1+κ2b2+κ3b3+κ4b4+κ5b5+κ6b6C. Then, we obtain thatz·y=0 implies that
    κ1a1b1+κ2a2b2+κ3a3b3+κ4a4b4+κ5a5b5+κ6a6b6=0.
    SinceK is linearly independent, we obtainaibi=0 for1i6. Also, we have(z)=(a1,a2,a3,a4,a5,a6)M(C) and(y)=(b1,b2,b3,b4,b5,b6)M(C). Consider
    (z)·(y)=(z)·(y)T=(a1,a2,a3,a4,a5,a6)MMT(b1,b2,b3,b4,b5,b6)=α(a1b1+a2b2+a3b3+a4b4+a5b5+a6b6)=0.
    Therefore,(y)(C), i.e.,(C)(C). Since the Gray map ∇ is bijective,|(C)|=|(C)| suggests that(C)=(C). IfC is a self-orthogonal code, thenCC, and hence,(C)(C)=(C). Therefore,(C) is a self-orthogonal code. □
    Theorem 6
    ([25]).LetC1=[n,k1,d1]q andC2=[n,k2,d2]q be two linear codes overGF(q) withC2C1. Then, a QECC exists with parameters[[n,k1+k2n,d]]q, whered=min{wt(v):v(C1C2)(C2C1)}min{d1,d2}. Moreover, ifC1 is a dual-containing code, then a QECC with parameters[[n,2k1n,d1]]q exists, whered1=min{wt(v):vC1C1}.
    Theorem 7
    ([6]).Let C be aΛ-constacyclic code overFp having a generator polynomialp(z). Then, C is dual-containing if(zlΛ)0mod(p(z)p*(z)), whereΛ=±1.
    The dual-containing cyclic and negacyclic codes overFp are provided by Theorem 7. Using this outcome, we can now ascertain the prerequisites and requirements forΛ-constacyclic codes overR to have their duals, as demonstrated in the following theorem.
    Theorem 8.
    LetC=i=16κiCi¯ be aΛ-constacyclic code of length l overR, whereΛ=κ1Λ1+κ2Λ2++κ6Λ6R andC=p(z)=κ1p1(z)+κ2p2(z)++κ6p6(z), wherepi(z) is the generating polynomial of codeCi¯ overFp for1i6. Then, C is a dual-containing code if and only if(zlΛi)0mod(pi(z)pi*(z)), whereΛi=±1 for1i6.
    Proof. 
    Suppose thatC=i=16κiCi¯ is aΛ-constacyclic code overR, whereΛ=κ1Λ1+κ2Λ2++κ6Λ6R. Then, by Theorem 4, the codeCi¯ is aΛi-constacyclic code with generating polynomialpi(z) overFp. IfC is a dual-containing code, then we havei=16κiCi¯i=16κiCi¯. Since this expression is unique, we haveCi¯Ci¯. Therefore, by Lemma 2 we have(zlΛi)0mod(pi(z)·pi*(z)). □
    Corollary 2.
    LetC=i=16κiCi¯ be aΛ-constacyclic code overR. Then, C is a dual-containing code overR if and only ifCi is a dual-containing code overFp for1i6.
    Theorem 9.
    LetC=i=16κiCi¯ be aΛ-constacyclic code of length l overR, and be the Gray map. If(C) has parameters[6l,k,dH], wherek=k1+k2++k6 is the dimension of(C) anddL is the Lee distance of C, if C is a dual-containing code, then a QECC exists with parameters[6l,2k6l,dH] overFp.
    Proof. 
    Suppose thatC is a dual-containing code overR and ∇ is a Gray map. Then,(C) is also a dual-containing code with parameters[6l,k,dH] overFp. Therefore, by Theorem 6, a QECC with parameters[[6l,2k6l,dH]]p exists overFp. □
    Example 6.
    LetR3=F3[w1,w2]w121,w23w2,w1w2w2w1 be a finite non-chain ring. Suppose thatΛ=2w221 is a unit element inR3. Then,Λ1=Λ2=1 andΛ3=Λ4=Λ5=Λ6=1. Thus, inF3[z], we have
    z91=(z+2)9z9+1=(z+1)9.
    Letp1(z)=p2(z)=(z+1)4,p3(z)=p4(z)=(z+2), andp5(z)=p6(z)=1 be the generator polynomials ofCi¯ for1i6, respectively. Then,C=κ1p1(z)+κ2p2(z)++κ6p6(z) is a(2w221)-constacyclic code of length9 overR3. LetN1GL6(F3), as given in Example 1, thenN1N1T=2I6 and the Gray image(C) has the parameters[54,44,4]. Moreover,(x9Λi)0mod(pi(z)pi*(z)) for1i6; thus, by Theorem 8, we find that C is a dual-containing code; so, by Theorem 9, we have a QECC[[54,34,4]]3, which is a new QECC with this parameter.
    Remark 2.
    In the previous example, we have seen that the Gray image(C) is a linear code with parameters[54,44,4] over the fieldF3. Specifically, for a code with a length9, the Gray image’s length is54, and its dimension is equal to the rational sum of the dimensions of the individual codes, yielding44 as a result. LetGi denote the generator matrix ofCi¯=pi(z) fori{1,2,,6}. Then, the generator matrix for(C) is given inSection 2.
    After providing the generator matrix(G) as input to the Magma Computation System [22], it was determined that the minimum distance of(C) is4. Based on this computation, it is crucial to note that the minimum distance of the Gray image is greater than the distance of eachCi. As in Example 6,dH(C1)=dH(C2)=3,dH(C3)=dH(C4)=2, anddH(C5)=dH(C6)=1, while the Lee distance is4. Notably, employing the canonical Gray map rather than the Gray map would result in a Lee distance of1 instead of4. Which underlines one of the primary advantages of using the Gray map.
    Example 7.
    LetR5=F5[w1,w2]w124,w234w2,w1w2w2w1 be a non-chain ring. Suppose thatΛ=1+w2(1+3w1)(1+3w2) is a unit element inR5. Then,Λ1=Λ2=Λ3=1 andΛ4=Λ5=Λ6=1. Thus, inF5[z], we have
    z151=(z+4)5(z2+z+1)5z15+1=(z+1)5(z2+4z+1)5.
    Letp1(z)=(z2+z+1),p2(z)=(z+4)2,p3(z)=1, andp4(z)=p5(z)=p6(z)=(z+1) be the generator polynomials ofCi¯ for1i6, respectively. Then,C=κ1p1(z)+κ2p2(z)++κ6p6(z) is a(1+12(1w1)(w2w22))-constacyclic code with length15 overR5. LetN2GL6(F5), as given in Example 2, thenN2N2T=4I6 and the Gray image(C) has the parameters[90,83,3]. Moreover,(z15Λi)0mod(pi(z)pi*(z)) for1i6; thus, by Theorem 8, we find that C is a dual-containing code; hence, by Theorem 9 we have a new QECC[[90,76,3]]5, with this parameter. Again, here we can see that the distance of(C)dH(Ci¯) for1i6.
    Example 8.
    LetR5=F5[w1,w2]w12+1,w234w2,w1w2w2w1 be a non-chain ring. Suppose thatΛ=4 is a unit element inR5. Then,Λ1=1=Λ2 andΛ3=1=Λ4=Λ5=Λ6. Thus, inF5[z], we have
    z351=(z+4)5(z6+z5+z4+z3+z2+z+1)5z35+1=(z+1)5(z6+4z5+z4+4z3+z2+4z+1)5.
    Letp1(z)=(z6+4z5+z4+4z3+z2+4z+1),p2(z)=(z+1)2,p3(z)=1, andp4(z)=p5(z)=p6(z)=(z+4) be the generator polynomials ofCi¯ for1i6, respectively. Then,C=κ1p1(z)+κ2p2(z)++κ6p6(z) is a Λ-constacyclic code with length35 overR5. LetN2GL6(F5), as given in Example 2, thenN2N2T=4I6 and the Gray image(C) has the parameters[210,199,3]. Moreover,(z35Λi)0mod(pi(z)pi*(z)) for1i6; thus, by Theorem 8, we find that C is a dual-containing code; so, by Theorem 9 we have an improved QECC[[210,188,3]]5 against the existing code[[210,186,3]]5 [14]. Here, we can see that the distance of(C)dH(Ci¯) for1i6.
    Example 9.
    LetR5 be a non-chain ring, as in Example 7. Suppose thatΛ=4+w2(2+w1)(2+w2) is a unit element inR5. Then,Λ1=1=Λ2=Λ3 andΛ4=1=Λ5=Λ6. Thus, inF5[z], we have
    z451=(z+4)5(z2+z+1)5(z6+z3+1)5z45+1=(z+1)5(z2+4z+1)5(z6+4z3+1)5.
    Letp1(z)=(z6+4z3+1),p2(z)=(z+1),p3(z)=(z+1)2,p4(z)=1, andp5(z)=p6(z)=(z+4) be the generator polynomials ofCi¯ for1i6, respectively. Then,C=κ1p1(z)+κ2p2(z)++κ6p6(z) is a(4+w2(2+w1)(2+w2))-constacyclic code with length45 overR5. LetN2GL6(F5), as given in Example 2, thenN2N2T=4I6 and the Gray image(C) has the parameters[270,259,3]. Moreover,(z45Λi)0mod(pi(z)pi*(z)) for1i6; thus, by Theorem 8, we find that C is a dual-containing code; thus, by Theorem 9 we have an improved QECC with parameters[[270,248,3]]5 against the existing code[[270,246,3]]5 [28]. Here, we can see that the distance of(C)dH(Ci¯) for1i6.
    Example 10.
    LetR7=F7[w1,w2]w121,w23w2,w1w2w2w1 be a non-chain ring. Suppose thatΛ=2w221 is a unit element inR7. Then,Λ1=1=Λ2 andΛ3=Λ4=1=Λ5=Λ6. Thus, inF7[z], we have
    z91=(z+3)(z+5)(z+6)(z3+3)(z3+5)z9+1=(z+1)(z+2)(z+4)(z3+2)(z3+4).
    Letp1(z)=(z3+2),p2(z)=1, andp3(z)=p4(z)=(z+3)=p5(z)=p6(z) be the generator polynomials ofCi¯ for1i6, respectively. Then,C=κ1p1(z)+κ2p2(z)++κ6p6(z) is a(2w221)-constacyclic code of length9 overR7. LetN3GL6(F7) such that
    N3=322222232222223222222322222232222223,
    thenN3N3T=I6 and the Gray image(C) has the parameters[54,47,3]. Moreover,(z9Λi)0mod(pi(z)pi*(z)) for1i6; thus, by Theorem 8, we find that C is a dual-containing code; so, by Theorem 9, we have a new QECC with parameters[[54,40,3]]7. Here, one can see that the distance of(C)dH(Ci¯) for1i6.
    Note: InTable 1,q,n, andΛ represent the order of the field, the length of the code defined overR, and the unit element inR, respectively.pi(z) is a generator polynomial ofCi fori{1,2,,6},N1,N2,N3 are the invertible matrices overF3,F5,F7, respectively, used to define the Gray map ∇. The parameters of the corresponding Gray image (dual-containing code) are denoted by(C).[[n,k,d]] and[[n,k,d]] represent the parameters of the new QECC and existing QECC, respectively.

    5. Conclusions

    This article focuses on the exploration of constacyclic codes in the context of non-chain ringsR=Fp[u,v]w12α2,w23β2w2,w1w2w2w1, whereα,βFp{0} for a primep. From this investigation, numerous new and improved quantum codes have been derived. Substantial potential exists for discovering additional quantum codes within the finite fieldFp by considering prime powers instead of primes. Applying the Gray map ∇ harnesses this potential. In a more general context, substituting the ringR with alternative commutative finite rings offers the prospect of developing many fresh quantum code constructions.

    Author Contributions

    Conceptualization, M.A.R. and P.S.; methodology, N.u.R., A.A. and M.F.A.; investigation, M.A.R., M.F.A., A.A. and M.K.G.; writing—original draft preparation, M.A.R., M.F.A., N.u.R., A.A. and A.N.K.; writing—review and editing, M.A.R., M.F.A., H.S., W.B. and N.u.R.; supervision, M.A.R. and A.A.; project administration, M.A.R., W.B., M.K.G., A.N.K., H.S. and P.S.; funding acquisition, M.A.R. and A.N.K. All authors have read and agreed to the published version of the manuscript.

    Funding

    This research work was funded by the Institutional Fund Projects of Saudi Arabia under grant number IFPRC-167-130-2020. Therefore, the authors gratefully acknowledge technical and financial support from the Ministry of Education and King Abdulaziz University, Jeddah, Saudi Arabia.

    Data Availability Statement

    This article required no data set.

    Acknowledgments

    We appreciate the constructive feedback provided by the reviewers, which has greatly improved the quality of our work.

    Conflicts of Interest

    The authors declare no conflicts of interest.

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    Table 1. Some new and improved QECCs overFp from constacyclic codes overRp for(p=3,5,7).
    Table 1. Some new and improved QECCs overFp from constacyclic codes overRp for(p=3,5,7).
    qnΛp1(z)p2(z)p3(z)=p4(z)p5(x)=p6(x)N(C)[[n,k,d]][[n,k,d]]
    39w1+w22+w1w22111211N1[54,52,2][[54,50,2]]3[[54,46,2]]3 [12]
    392w2211101111011121N1[54,44,4][[54,34,4]]3New QECC
    311w1+w22+w1w2210222111021221N1[66,51,3][[66,36,3]]3New QECC
    311w1+w22+w1w221022211021221021221N1[66,46,4][[66,26,4]]3New QECC
    311w1+w22+w1w2210222111021221022122N1[66,41,5][[66,16,5]]3New QECC
    3132w2211021102111021N1[78,66,4][[78,54,4]]3New QECC
    31811101111011121N1[108,98,3][[108,88,3]]3New QECC
    561134131212N2[36,29,4][[36,22,4]]5New QECC
    51811003004131212N2[108,97,4][[108,86,4]]5New QECC
    51911103323434110332343411033234341N2[114,69,6][[114,24,6]]5New QECC
    51911033234341103323434110332343411033234341N2[114,60,7][[114,6,7]]5New QECC
    520w1+w22+w1w2210404111111N2[120,111,3][[120,102,3]]5[[120,96,3]]5 [14]
    522w1w22+w1w2211121211312N2[132,123,4][[132,114,4]]5[[132,110,4]]5 [21]
    52512w22140004111111N2[150,140,3][[150,130,3]]5New QECC
    52512w2214000000001411111N2[150,135,4][[150,120,4]]5New QECC
    54011234211213N2[240,232,3][[240,224,3]]5New QECC
    7712w22143611111N3[42,35,4][[42,28,4]]7New QECC
    792w2211002121313N3[54,46,4][[54,38,4]]7New QECC
    714w1+w22+w1w221020113311111N3[84,73,4][[84,62,4]]7New QECC
    71512w2215335611214N3[90,81,4][[90,72,4]]7New QECC
    718w1+w22+w1w22102130261212N3[108,98,4][[108,88,4]]7New QECC
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    © 2024 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).

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    MDPI and ACS Style

    Raza, M.A.; Ahmad, M.F.; Alahmadi, A.; Basaffar, W.; Gupta, M.K.; Rehman, N.u.; Khan, A.N.; Shoaib, H.; Sole, P. Quantum Codes as an Application of Constacyclic Codes.Axioms2024,13, 697. https://doi.org/10.3390/axioms13100697

    AMA Style

    Raza MA, Ahmad MF, Alahmadi A, Basaffar W, Gupta MK, Rehman Nu, Khan AN, Shoaib H, Sole P. Quantum Codes as an Application of Constacyclic Codes.Axioms. 2024; 13(10):697. https://doi.org/10.3390/axioms13100697

    Chicago/Turabian Style

    Raza, Mohd Arif, Mohammad Fareed Ahmad, Adel Alahmadi, Widyan Basaffar, Manish K. Gupta, Nadeem ur Rehman, Abdul Nadim Khan, Hatoon Shoaib, and Patrick Sole. 2024. "Quantum Codes as an Application of Constacyclic Codes"Axioms 13, no. 10: 697. https://doi.org/10.3390/axioms13100697

    APA Style

    Raza, M. A., Ahmad, M. F., Alahmadi, A., Basaffar, W., Gupta, M. K., Rehman, N. u., Khan, A. N., Shoaib, H., & Sole, P. (2024). Quantum Codes as an Application of Constacyclic Codes.Axioms,13(10), 697. https://doi.org/10.3390/axioms13100697

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