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Article

New Construction of Maximum Distance Separable (MDS) Self-Dual Codes over Finite Fields

Department of Mathematical Sciences, Xi’an University of Technology, Xi’an 710054, China
*
Author to whom correspondence should be addressed.
Entropy 2019, 21(2), 101; https://doi.org/10.3390/e21020101
Submission received: 24 December 2018 / Revised: 10 January 2019 / Accepted: 17 January 2019 / Published: 22 January 2019
(This article belongs to the Special Issue Information Theory Applications in Signal Processing)

Abstract

:
Maximum distance separable (MDS) self-dual codes have useful properties due to their optimality with respect to the Singleton bound and its self-duality. MDS self-dual codes are completely determined by the length n , so the problem of constructing q-ary MDS self-dual codes with various lengths is a very interesting topic. Recently X. Fang et al. using a method given in previous research, where several classes of new MDS self-dual codes were constructed through (extended) generalized Reed-Solomon codes, in this paper, based on the method given in we achieve several classes of MDS self-dual codes.

1. Introduction

Let F q be the finite field with q elements. A q-ary [ n , k , d ] linear code C is a k-dimensional subspace of F q n with minimum (Hamming) distance d . If the parameters [ n , k , d ] satisfy k + d = n + 1 , the code is called an MDS (maximum distance separable) code. A self-dual code is a linear code satisfying C = C . A linear complementary-dual code is a linear code satisfying C C = { 0 } .
The study of MDS self-dual codes has attracted a great deal of attention in recent years due to its theoretical and practical importance. The center of the study of MDS codes includes the existence of MDS codes [1], classification of MDS codes [2], balanced MDS codes [3], non-Reed-Solomon MDS codes [4], complementary-dual MDS codes [5,6], and lowest density MDS codes [7].
As the parameters of an MDS self-dual code are completely determined by the code’s length n, the main interest here is to determine the existence and give the construction of q-ary MDS self-dual codes for various lengths. The problem is completely solved for the case where q is even [8]. Many MDS self-dual codes over finite fields of odd characteristics were constructed [9,10,11,12,13,14].
In [11], Jin and Xing constructed several classes of MDS self-dual code from generalized Reed-Solomon code. Yan generalized Jin and Xing’s method and constructed several classes of MDS self-dual codes via generalized Reed-Solomon codes and extended generalized Reed-Solomon codes [14]. In [12], Ladad, Liu and Luo produced more classes of MDS self-dual codes based on [11] and [14]. In [9], based on the [11,12,14] more new parameter MDS self-dual codes were presented. Based on the method raised in [9], we present some classes of MDS self-dual codes.

2. Preliminaries

In this section we introduce some basic notations of generalized Reed-Solomon codes and extended generalized Reed-Solomon codes. For more details, the reader is referred to [15].
Throughout this paper, q is a prime power, F q is the finite fields with q elements and let n be a positive integer with 1 < n q . For any x F q 2 , we denote by x ¯ the conjugation of x . Given an [ n , k , d ] linear code C , its Euclidean dual code (resp. Hermitian dual code) is denoted by C (resp. C H ). The codes C and C H are defined by
C = { x = ( x 1 , x 2 , , x n ) F q n : i = 1 n x i y i = 0 , y = ( y 1 , y 2 , , y n ) C } ,
C H = { x = ( x 1 , x 2 , , x n ) F q 2 n : i = 1 n x i y i ¯ = 0 , y = ( y 1 , y 2 , , y n ) C } ,
respectively. In this paper, we only consider the Euclidean inner product.
Let a = ( α 1 , α 2 , , α n ) , where α 1 , α 2 , , α n are n distinct elements of F q . Fix n nonzero elements v 1 , v 2 , , v n of F q ( v i are not necessarily distinct), put v = ( v 1 , v 2 , , v n ) . For 1 k n , the k-dimensional generalized Reed-Solomon code (GRS for short) of length n associated with a and v is defined to be
GRS k ( a , v ) = { ( v 1 f ( α 1 ) , v 2 f ( α 2 ) , , v n f ( α n ) ) : f ( x ) F q [ x ] , deg ( f ( x ) ) k 1 } .
It is well known that the code GRS k ( a , v ) is a q-ary [ n , k , n k + 1 ] MDS code and the dual of a GRS code is again a GRS MDS code; indeed
GRS k ( a , v ) = GRS n k ( a , v )
for some v = ( v 1 , v 2 , , v n ) with v i 0 for all 1 i n (e.g., see [15]).
Furthermore, the extended generalized Reed-Solomon code GRS k ( a , v , ) given by
GRS k ( a , v , ) = { ( v 1 f ( α 1 ) , v 2 f ( α 2 ) , , v n f ( α n ) , f k 1 ) : f ( x ) F q [ x ] , deg ( f ( x ) ) k 1 } ,
where f k 1 stands for the coefficient of x k 1 in f ( x ) . It is also well known that GRS k ( a , v , ) is a q-ary [ n + 1 , k , n k + 2 ] MDS code and the dual code is also a GRS MDS code (e.g., see [15]).
Put a = ( α 1 , α 2 , , α n ) and denote by A a the matrix
1 1 1 α 1 α 2 α n α 1 2 α 2 2 α n 2 α 1 n 2 α 2 n 2 α n n 2
Lemma 1
([11]). The solution space of the equation system A a X T = 0 has dimension 1 and { u = ( u 1 , u 2 , , u n ) } is a basis of this solution space, where u i = 1 j n , j i ( α i α j ) 1 . Furthermore, for any two polynomials f ( x ) , g ( x ) F q [ x ] with deg ( f ) k 1 and deg ( g ) n k 1 , one has i = 1 n f ( α i ) ( u i g ( α i ) ) = 0 .
We define
L a ( α i ) = 1 j n , j i ( α i α j ) .
The conclusion of the following lemma is straightforward. For completeness, we provide its proof.
Lemma 2
([11]). Let n be an even number, if there exists λ F q * such that λ L a ( α i ) is square element for all i = 1 , 2 , , n , then the code GRS n / 2 ( a , v ) defined in (1) is MDS self-dual code of length n.
Proof. 
Let f ( x ) , g ( x ) F q [ x ] with deg ( f ) n 2 1 and deg ( g ) n 2 1 . By Lemma 1, we have i = 1 n f ( α i ) ( u i g ( α i ) ) = 0 , where u i = 1 j n , j i ( α i α j ) 1 for i = 1 , 2 , , n . Hence,
0 = λ i = 1 n f ( α i ) ( u i g ( α i ) ) = i = 1 n f ( α i ) ( λ u i g ( α i ) ) = i = 1 n ( v i f ( α i ) ) ( v i g ( α i ) ) ( since λ u i = v i 2 ) .
This implies that GRS n / 2 ( a , v ) = GRS n / 2 ( a , v ) .  □
H. Yan [14] observed the following two results.
Lemma 3
([14]). Let n be an even integer and k = n 2 . If L a ( α i ) is square element for all i = 1 , 2 , , n 1 , then the code GRS k ( a , v , ) defined in (2) is MDS self-dual code of length n .
Lemma 4
([14]). Let m q 1 be a positive integer and let α F q be a primitive m-th root of unity. Then for any 1 i m , we have
1 j m , j i ( α i α j ) = m α i .

3. Main Result

Let q = r 2 , where r is odd prime power, F q be the finite fields with q elements. Suppose m q 1 , α is a primitive m-th root of unity and H = < β > is the cyclic group generated by β .
Theorem 1.
Let q = r 2 , where r is an odd prime power, r 1 ( mod 4 ) . Suppose that m ( q 1 ) and q 1 m is even, m 0 ( mod 4 ) . If 1 t 2 ( r + 1 ) g c d ( 2 ( r + 1 ) , m ) . Then there exists an [ n = t m , n 2 ] -MDS self-dual code.
Proof. 
Let α be a primitive m-th root of unity and H = < β > is the cyclic group of order 2 ( r + 1 ) . By the theorem of group homomorphism,
( H × α ) / α H / ( H α ) .
Let i 1 , i 2 , , i t be t distinct elements, such that 0 i 1 < i 2 < < i t < 2 ( r + 1 ) . Denote I = { i 1 , i 2 , , i t } , A = i 1 + i 2 + + i t and B = { β i 1 , β i 2 , , β i t } be a set of coset representatives of ( H × α ) / α . Let
a = ( α β i 1 , , α m β i 1 , α β i 2 , , α m β i 2 , , α β i t , , α m β i t ) .
Then the entries of a are distinct in F q * .
It is known that x m y m = j = 1 m ( x α j y ) . By the statement of Lemma 3, we get
L a ( β z α k ) = 1 j m , j k ( β z α k β z α j ) l I , l z j = 1 m ( β z α k β l α j ) = β z ( m 1 ) 1 j m , j k ( α k α j ) l I , l z [ ( β z α k ) m β l m ] = β z ( m 1 ) m α k l I , l z ( β z m β l m ) .
Let v = l I , l z ( β z m β l m ) , then
v r = l I , l z ( β z m r β l m r ) ( since β 2 ( r + 1 ) = 1 , β r = β 1 ) = l I , l z [ ( β 1 ) z m ( β 1 ) l m ] = l I , l z [ ( β 1 ) z m ( β 1 ) l m ] = l I , l z ( β 1 ) z m + l m ( β l m β z m ) = ( 1 ) t 1 β ( A + ( t 2 ) z ) m v
So v r 1 = ( 1 ) t 1 β ( A + ( t 2 ) z ) m .
Let g be a generator of F q * , then α = g q 1 m , β = g r 1 2 , 1 = g r 2 1 2 , v = g r + 1 2 ( t 1 ) ( A + ( t 2 ) z ) m 2 + i ( r + 1 ) . Note that β , m and α are square elements of F q * , we take λ = g r + 1 2 ( t 1 ) , then λ L a ( β z α k ) is a square element of F q * .
This implies there exists a q-ary [ n , n 2 ] MDS self-dual code. □
Example 1.
Let r = 173 , q = 173 2 , r 1 ( mod 4 ) , m = 4 × 43 , q 1 m = 174 is even. For 1 t 2 ( r + 1 ) g c d ( 2 ( r + 1 ) , m ) = 87 , we choose t = 81 . By Theorem 1, there exists the MDS self-dual code with length n = m t = 13,932.
Theorem 2.
Let q = r 2 , where r is an odd prime power. Suppose that m is odd, m ( q 1 ) and q 1 m is even. If 1 t m i n { r + 1 g c d ( 2 ( r + 1 ) , m ) , r + 1 2 } and t is odd, then there exists a q-ary [ n = t m + 1 , n 2 ] MDS self-dual code over F q .
Proof. 
Let α and β be the same as in Theorem 1, we choose t distinct even number i 1 , i 2 , , i t , 0 i 1 < i 2 < < i t < 2 ( r + 1 ) . Denote I = { i 1 , i 2 , , i t } , A = i 1 + i 2 + + i t . Suppose all i j 2 ( mod 4 ) , j = 1 , 2 , , t . The proof is as similar as in Theorem 1. We get
L a ( β z α k ) = β z ( m 1 ) m α k l I , l z ( β z m β l m ) .
Let v = l I , l z ( β z m β l m ) , then we get
v r 1 = ( 1 ) t 1 β ( A + ( t 2 ) z ) m , v = g r + 1 2 ( t 1 ) ( A + ( t 2 ) z ) m 2 + i ( r + 1 ) ,
since A + ( t 2 ) z 2 is even, it implies that v is a square element of F q * . So L a ( β z α k ) is square element of F q * . By Lemma 3, there exists a q-ary [ n , n 2 ] MDS self-dual code. □
Example 2.
Let r = 67 , q = 67 2 , m = 11 , q 1 m = 408 is even. Since 2 ( r + 1 ) = 136 = 4 × 34 , for 1 t r + 1 g c d ( 2 ( r + 1 ) , m ) = 68 , we choose t = 27 . By Theorem 2, there exists the MDS self-dual code with length n = m t + 1 = 298 .
Theorem 3.
Let q = r 2 , where r is an odd prime power, r 1 ( mod 4 ) . Suppose that m is odd, m ( q 1 ) and q 1 m is even. If 1 t m i n { r + 1 g c d ( 2 ( r + 1 ) , m ) , r + 1 2 } and t is odd, then there exists a q-ary [ n = t m + 1 , n 2 ] MDS self-dual code over F q .
Proof. 
Let α and β be the same as in Theorem 1, we choose t distinct even number i 1 , i 2 , , i t , 0 i 1 < i 2 < < i t < 2 ( r + 1 ) . Denote I = { i 1 , i 2 , , i t } , A = i 1 + i 2 + + i t , and i j 2 ( mod 4 ) , j = 1 , 2 , , t . We define the generalized Reed -Solomon code GRS k ( a , v ) with
a = ( 0 , α β i 1 , , α m β i 1 , α β i 2 , , α m β i 2 , , α β i t , , α m β i t ) .
For any z I and 1 k m , we get
L a ( β z α k ) = β z α k 1 j m , j k ( β z α k β z α j ) l I , l z j = 1 m ( β z α k β l α j ) = β z m m l I , l z ( β z m β l m )
and
L a ( 0 ) = l I j = 1 m ( 0 β l α j ) = ( 1 ) m t α m ( m + 1 ) 2 ( l I β l ) m .
Since r 1 ( mod 4 ) , q 1 m is even, so α , β , m , 1 are square elements of F q * , we only need to consider v = l I , l z ( β z m β l m ) . As the calculation in the proof of Theorem 1, v = g r + 1 2 ( t 1 ) ( A + ( t 2 ) z ) m 2 + i ( r + 1 ) . Since all i j 2 ( mod 4 ) and t is odd, so ( A + ( t 2 ) z ) m 2 is even. L a ( β z α k ) , L a ( 0 ) are square elements of F q * . By Lemma 2, there exists a q-ary [ n , n 2 ] MDS self-dual code. □
Example 3.
Let r = 101 , r 1 ( mod 4 ) , q = 101 2 , m = 75 , q 1 m = 136 is even. Since 2 ( r + 1 ) = 204 = 4 × 51 , for 1 t r + 1 g c d ( 2 ( r + 1 ) , m ) = 34 , we choose t = 33 . By Theorem 2, there exists the MDS self-dual code with length n = m t + 1 = 2476 .
Theorem 4.
Let q = r 2 , where r is an odd prime power. Suppose that m ( q 1 ) , q 1 m is even. If 1 t 2 ( r + 1 ) g c d ( 2 ( r + 1 ) , m ) and t m is even, then there exists a q-ary [ n = t m + 2 , n 2 ] MDS self-dual code over F q .
Proof. 
Let α and β be the same as in Theorem 1. We define the extended generalized Reed -Solomon code GRS k ( a , v , ) with
a = ( 0 , α β i 1 , , α m β i 1 , α β i 2 , , α m β i 2 , , α β i t , , α m β i t ) .
For any z I and 1 k m , we get
L a ( β z α k ) = β z α k 1 j m , j k ( β z α k β z α j ) l I , l z j = 1 m ( β z α k β l α j ) = β z m m l I , l z ( β z m β l m )
and
L a ( 0 ) = l I j = 1 m ( 0 β l α j ) = ( 1 ) m t α m ( m + 1 ) 2 ( l I β l ) m .
Case 1: If m is even, t is odd.
β z m , m and L a ( 0 ) are square elements of F q * . Let v = l I , l z ( β z m β l m ) , as the calculation in Theorem 1, v = g r + 1 2 ( t 1 ) ( A + ( t 2 ) z ) m 2 + i ( r + 1 ) . So we only need to consider the parity of ( A + ( t 2 ) z ) m 2 .
  • i 1 , i 2 , , i t are even number, so A + ( t 2 ) z 0 ( mod 2 ) , v is a square element of F q * .
  • i 1 , i 2 , , i t are odd number, so A + ( t 2 ) z 0 ( mod 2 ) , v is a square element of F q * .
Case 2: If m and t are even, r 3 ( mod 4 ) , we assume A is an even integer. It follows that r + 1 2 ( t 1 ) ( A + ( t 2 ) z ) m 2 is an even integer.
Case 3: If m is odd, t is even.
  • t 0 ( mod 4 )
    (1)
    If r 1 ( mod 4 ) , all i 1 , i 2 , , i t are odd, and A 0 ( mod 4 ) , then then ( r + 1 ) ( t 1 ) ( A + ( t 2 ) z ) m 0 ( mod 4 ) , v is a square element of F q * .
    (2)
    If r 3 ( mod 4 ) , all i 1 , i 2 , , i t are even, and A 2 ( mod 4 ) , then ( r + 1 ) ( t 1 ) ( A + ( t 2 ) z ) m 0 ( mod 4 ) , v is a square element of F q * .
  • t 2 ( mod 4 ) .
    (1)
    If r 1 ( mod 4 ) , A 2 ( mod 4 ) , then ( r + 1 ) ( t 1 ) ( A + ( t 2 ) z ) m 0 ( mod 4 ) , v is square of F q * .
    (2)
    If r 3 ( mod 4 ) , A 0 ( mod 4 ) , then ( r + 1 ) ( t 1 ) ( A + ( t 2 ) z ) m 0 ( mod 4 ) , v is square of F q * .
 □
We can extend the Theorem 1 to a more general case.
Theorem 5.
Let q = r 2 , where r is an odd prime power. Suppose that m ( q 1 ) , q 1 m is even, s m , s r 1 and r 1 s is even. If 1 t s ( r + 1 ) g c d ( s ( r + 1 ) , m ) , then there exists a q-ary [ n = t m , n 2 ] MDS self-dual code over F q .
Proof. 
Let α be a primitive m-th root of unity and H = < β > is the cyclic group of order s ( r + 1 ) . By the theorem of group homomorphism,
( H × α ) / α H / ( H α ) ,
Let i 1 , i 2 , , i t be t distinct elements, such that 0 i 1 < i 2 < < i t < 2 ( r + 1 ) . Denote I = { i 1 , i 2 , , i t } , A = i 1 + i 2 + + i t and B = { β i 1 , β i 2 , , β i t } be a set of coset representatives of H × α . Let
a = ( α β i 1 , , α m β i 1 , α β i 2 , , α m β i 2 , , α β i t , , α m β i t ) .
Similar with Theorem 1, we get
L a ( β z α k ) = 1 j m , j k ( β z α k β z α j ) l I , l z j = 1 m ( β z α k β l α j ) = β z ( m 1 ) · m · α k l I , l z ( β z m β l m . )
Since β s ( r + 1 ) = 1 , then β r + 1 = ξ s , where ξ s is s-th primitive root of unity. So β r = ξ s β 1 . Let v = l I , l z ( β z m β l m ) . Since s m , then
v r = l I , l z ( ( β 1 ) z m ( β 1 ) l m ) = l I , l z β ( l + z ) m ( β l m β z m ) = ( 1 ) t 1 β ( A + ( t 2 ) z ) m v .
So v r 1 = ( 1 ) t 1 β ( A + ( t 2 ) z ) m .
Let g be a generator of F q * . It follows that β = g r 1 s and 1 = g r 2 1 2 . So
v = g ( r + 1 ) 2 ( t 1 ) [ A + ( t 2 ) z ] m s .
Case 1: If m odd and t even, we can take λ = g ( r + 1 ) 2 ( t 1 ) A · m s . Hence, we have λ L a ( β z α k ) is square element of F q * .
Case 2: If m even and 2 m s , we can take λ = g ( r + 1 ) 2 ( t 1 ) . Hence, we have λ L a ( β z α k ) is square element of F q * .
So there exists a q-ary MDS self-dual code with length n .  □

4. Conclusions

In this paper, based on the method from [9], we construct several classes of MDS self-dual code over finite fields with odd characteristics via the generalized Reed-Solomon code and extend the generalized Reed-Solomon code.

Author Contributions

Original ideas, writing, original draft preparation, A.Z.; review, Z.J.; funding acquisition, A.Z.

Funding

This research was funded by the National Natural Science Foundation of China under Grants 11401468.

Conflicts of Interest

The authors declare no conflict of interest.

References

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MDPI and ACS Style

Zhang, A.; Ji, Z. New Construction of Maximum Distance Separable (MDS) Self-Dual Codes over Finite Fields. Entropy 2019, 21, 101. https://doi.org/10.3390/e21020101

AMA Style

Zhang A, Ji Z. New Construction of Maximum Distance Separable (MDS) Self-Dual Codes over Finite Fields. Entropy. 2019; 21(2):101. https://doi.org/10.3390/e21020101

Chicago/Turabian Style

Zhang, Aixian, and Zhe Ji. 2019. "New Construction of Maximum Distance Separable (MDS) Self-Dual Codes over Finite Fields" Entropy 21, no. 2: 101. https://doi.org/10.3390/e21020101

APA Style

Zhang, A., & Ji, Z. (2019). New Construction of Maximum Distance Separable (MDS) Self-Dual Codes over Finite Fields. Entropy, 21(2), 101. https://doi.org/10.3390/e21020101

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