Description
For any \([n,k]_q\) linear code \(C\), the dual code is the set of \(q\)-ary strings that are orthogonal to the codewords of \(C\) under a particular inner product.
The dual code is a linear code defined by \begin{align} C^\perp = \{ y\in GF(q)^{n} ~|~ x\cdot y=0 \forall x\in C\}, \tag*{(1)}\end{align} where the ordinary, standard, Euclidean, or symmetric inner product is \(x\cdot y = \sum_{i=1}^n x_i y_i\) for coordinates \(x_i,y_i\).
A code that is contained in its dual, \(C \subseteq C^\perp\), is called self-orthogonal, weakly self-dual, or null. A self-orthogonal code is called maximal if it is not contained in the dual of any other code. A code that contains its dual, \(C^\perp \subseteq C\), is called dual-containing. A code that is equal to its dual, \(C^\perp = C\), is called self-dual. A code that is equivalent to its dual is called iso-dual. A code admits a complementary dual if \(C\) and \(C^{\perp}\) do not share any codewords; such codes are called LCD codes. The dual of a dual code is the original code. A code is dual-containing iff its dual is self-orthogonal.
The dual code \(C^\perp\) is the row space of the parity check matrix of \(C\). The dual code is the kernel of the encoding map for \(C\), and \(\dim C^\perp = n-k\). The automorphism group of a linear binary code and its dual are the same [1; pg. 230].
An alternative definition of dual substitutes the Euclidean inner product for the Hermitian inner product, \begin{align} x\cdot y \to x\cdot \bar{y} = \sum_{i=1}^n x_i y^{p}_i~. \tag*{(2)}\end{align} Self-dual codes with respect to the above product are called Hermitian self-dual; similar definitions hold for self-orthogonal and dual-containing.
More general inner products can also be considered [2].
Protection
The dual of an \([n,k,d] \) code is an \([n,n-k,d^{\perp}]\) code, where the dual distance \(d^{\perp}\) is not always related to \(d\). The generator matrix of \(C^\perp\) is the parity check matrix of \(C\), and visa versa.
The generator matrix of the Hermitian dual of a code with generator matrix \(G = [I_k~~A]\) is \([-\bar{A}^T~~I_{n-k}]\), where \(\bar{A}\) contains matrix elements of \(A\) raised to the \(p\)th power. A code is Hermitian self-dual if and only if \(A \bar{A}^{T} = -I_{n/2}\).
Cousins
- Dual lattice— Dual lattices are lattice analogues of dual codes.
- Combinatorial design— Linear codes and their duals are related to combinatorial designs via the Assmus-Mattson theorem [3,4] (see [5; Sec. 5.4]).
- \([23, 12, 7]\) Golay code— The dual of the Golay code is its \([23,11,8]\) even-weight subcode [6,7].
- \([2^m-1,m,2^{m-1}]\) simplex code— Hamming and simplex codes are dual to each other.
- \([2^r,2^r-r-1,4]\) Extended Hamming code— Extended Hamming and first-order RM codes are dual to each other.
- \([7,4,3]\) Hamming code— The \([7,3,4]\) simplex code is the dual of the Hamming code and also its even-weight subcode [6,7].
- Hergert code— Hergert codes are duals of DG codes in that their distance distribution is equal to the MacWilliams transform of the distance distribution of DG codes [8]. However, the two codes are images of a pair of mutually dual linear codes over \(\mathbb{Z}_4\) under the Gray map [9–11].
- \([n,n-1,2]\) Single parity-check (SPC) code— Binary SPCs and repetition codes are dual to each other.
- Reed-Muller (RM) code— The codes RM\((r,m)\) and RM\((m-r-1,m)\) are dual to each other, with the case \(m = 2r+1\) being self dual.
- Hsu-Anastasopoulos LDPC (HA-LDPC) code— HA-LDPC and MN-LDPC codes are dual to each other [12].
- Maximum distance separable (MDS) code— A linear binary or \(q\)-ary \([n,k,n-k+1]\) code is MDS if and only if its dual \([n,n-k,k+1]\) is MDS [13; Thm. 1.9.13].
- Dual additive code— Different inner products are typically used to define duals of linear and additive codes.
- \(q\)-ary simplex code— \(q\)-ary Hamming and \(q\)-ary simplex codes are dual to each other.
- Dual linear code over \(R\)
- Majorana stabilizer code— Classical self-orthogonal codes can be used to construct Majorana stabilizer codes [14]. The direct relationship between the two codes follows from expressing the Majorana strings as binary vectors – akin to the symplectic representation – and observing that the binary stabilizer matrix \(S\) for such a Majorana stabilizer code satisfies \(S\cdot S^T=0\) because it has commuting stabilizers, which is precisely the condition \(G\cdot G^T=0\) on the generator matrix \(G\) of a self-orthogonal classical code. A self-orthogonal classical code \(C\) with parameters \([2N,k,d]\) yields a Majorana stabilizer code with parameters \([[N,N-k,d^\perp]]_f\), where \(d^\perp\) is the code distance of the dual code \(C^\perp\).
- Hermitian qubit code— Hermitian qubit codes are constructed from Hermitian self-orthogonal linear codes over \(GF(4)\) via the \(GF(4)\) representation.
- Qubit CSS code— CSS codes for which \(C_X=C_Z \equiv C\) are called self-orthogonal or homogeneous [15] since \(C^{\perp} \subseteq C\). The stabilizer group of such codes is invariant under the Hadamard gate exchanging \(X\) and \(Z\).
- Qubit stabilizer code— Qubit stabilizer codes are in one-to-one correspondence with symplectic self-orthogonal binary linear codes of length \(2n\) via the symplectic representation.
- Hermitian Galois-qudit code— Hermitian codes are constructed from Hermitian self-orthogonal linear codes over \(GF(q^2)\) via the \(GF(q^2)\) representation.
Member of code lists
Primary Hierarchy
References
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- A. R. Hammons Jr., P. V. Kumar, A. R. Calderbank, N. J. A. Sloane, and P. Solé, “The Z_4-Linearity of Kerdock, Preparata, Goethals and Related Codes”, (2002) arXiv:math/0207208
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- Z. X. Wan, Quaternary Codes (WORLD SCIENTIFIC, 1997) DOI
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- K. KASAI and K. SAKANIWA, “Spatially-Coupled MacKay-Neal Codes and Hsu-Anastasopoulos Codes”, IEICE Transactions on Fundamentals of Electronics, Communications and Computer Sciences E94-A, 2161 (2011) arXiv:1102.4612 DOI
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- W. C. Huffman, J.-L. Kim, and P. Solé, "Basics of coding theory." Concise Encyclopedia of Coding Theory (Chapman and Hall/CRC, 2021) DOI
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- S. Vijay and L. Fu, “Quantum Error Correction for Complex and Majorana Fermion Qubits”, (2017) arXiv:1703.00459
- [15]
- Y.-J. Wang, Z.-Y. Xiao, Y. Zhang, X.-Y. Xiong, and S. Shi, “Construction of Multiple-Rate Quantum LDPC Codes Sharing One Scalable Stabilizer Circuit”, IEEE Transactions on Communications 71, 1071 (2023) DOI
Page edit log
- Victor V. Albert (2022-07-22) — most recent
- Micah Shaw (2022-06-28)
- Victor V. Albert (2021-12-18)
- Dhruv Devulapalli (2021-12-17)
Cite as:
“Dual linear code”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2022. https://errorcorrectionzoo.org/c/dual