An n-class association scheme consists of a set X together with a partition S of X × X into n + 1 binary relations, R0, R1, ..., Rn which satisfy:
An association scheme is commutative if p i j k = p j i k {\displaystyle p_{ij}^{k}=p_{ji}^{k}} for all i {\displaystyle i} , j {\displaystyle j} and k {\displaystyle k} . Most authors assume this property. Note, however, that while the notion of an association scheme generalizes the notion of a group, the notion of a commutative association scheme only generalizes the notion of a commutative group.
A symmetric association scheme is one in which each R i {\displaystyle R_{i}} is a symmetric relation. That is:
Every symmetric association scheme is commutative.
Two points x and y are called i th associates if ( x , y ) ∈ R i {\displaystyle (x,y)\in R_{i}} . The definition states that if x and y are i th associates then so are y and x. Every pair of points are i th associates for exactly one i {\displaystyle i} . Each point is its own zeroth associate while distinct points are never zeroth associates. If x and y are k th associates then the number of points z {\displaystyle z} which are both i th associates of x {\displaystyle x} and j th associates of y {\displaystyle y} is a constant p i j k {\displaystyle p_{ij}^{k}} .
A symmetric association scheme can be visualized as a complete graph with labeled edges. The graph has v {\displaystyle v} vertices, one for each point of X {\displaystyle X} , and the edge joining vertices x {\displaystyle x} and y {\displaystyle y} is labeled i {\displaystyle i} if x {\displaystyle x} and y {\displaystyle y} are i {\displaystyle i} th associates. Each edge has a unique label, and the number of triangles with a fixed base labeled k {\displaystyle k} having the other edges labeled i {\displaystyle i} and j {\displaystyle j} is a constant p i j k {\displaystyle p_{ij}^{k}} , depending on i , j , k {\displaystyle i,j,k} but not on the choice of the base. In particular, each vertex is incident with exactly p i i 0 = v i {\displaystyle p_{ii}^{0}=v_{i}} edges labeled i {\displaystyle i} ; v i {\displaystyle v_{i}} is the valency of the relation R i {\displaystyle R_{i}} . There are also loops labeled 0 {\displaystyle 0} at each vertex x {\displaystyle x} , corresponding to R 0 {\displaystyle R_{0}} .
The relations are described by their adjacency matrices. A i {\displaystyle A_{i}} is the adjacency matrix of R i {\displaystyle R_{i}} for i = 0 , … , n {\displaystyle i=0,\ldots ,n} and is a v × v matrix with rows and columns labeled by the points of X {\displaystyle X} .
The definition of a symmetric association scheme is equivalent to saying that the A i {\displaystyle A_{i}} are v × v (0,1)-matrices which satisfy
The (x, y)-th entry of the left side of (IV) is the number of paths of length two between x and y with labels i and j in the graph. Note that the rows and columns of A i {\displaystyle A_{i}} contain v i {\displaystyle v_{i}} 1 {\displaystyle 1} 's:
The term association scheme is due to (Bose & Shimamoto 1952) but the concept is already inherent in (Bose & Nair 1939).9 These authors were studying what statisticians have called partially balanced incomplete block designs (PBIBDs). The subject became an object of algebraic interest with the publication of (Bose & Mesner 1959) and the introduction of the Bose–Mesner algebra. The most important contribution to the theory was the thesis of Ph. Delsarte (Delsarte 1973) who recognized and fully used the connections with coding theory and design theory.10
A generalization called coherent configurations has been studied by D. G. Higman.
The adjacency matrices A i {\displaystyle A_{i}} of the graphs ( X , R i ) {\displaystyle \left(X,R_{i}\right)} generate a commutative and associative algebra A {\displaystyle {\mathcal {A}}} (over the real or complex numbers) both for the matrix product and the pointwise product. This associative, commutative algebra is called the Bose–Mesner algebra of the association scheme.
Since the matrices in A {\displaystyle {\mathcal {A}}} are symmetric and commute with each other, they can be diagonalized simultaneously. Therefore, A {\displaystyle {\mathcal {A}}} is semi-simple and has a unique basis of primitive idempotents J 0 , … , J n {\displaystyle J_{0},\ldots ,J_{n}} .
There is another algebra of ( n + 1 ) × ( n + 1 ) {\displaystyle (n+1)\times (n+1)} matrices which is isomorphic to A {\displaystyle {\mathcal {A}}} , and is often easier to work with.
The Hamming scheme and the Johnson scheme are of major significance in classical coding theory.
In coding theory, association scheme theory is mainly concerned with the distance of a code. The linear programming method produces upper bounds for the size of a code with given minimum distance, and lower bounds for the size of a design with a given strength. The most specific results are obtained in the case where the underlying association scheme satisfies certain polynomial properties; this leads one into the realm of orthogonal polynomials. In particular, some universal bounds are derived for codes and designs in polynomial-type association schemes.
In classical coding theory, dealing with codes in a Hamming scheme, the MacWilliams transform involves a family of orthogonal polynomials known as the Krawtchouk polynomials. These polynomials give the eigenvalues of the distance relation matrices of the Hamming scheme.
Bailey 2004, pg. 387 - Bailey, Rosemary A. (2004), Association Schemes: Designed Experiments, Algebra and Combinatorics, Cambridge University Press, ISBN 978-0-521-82446-0, MR 2047311 http://www.maths.qmul.ac.uk/~rab/Asbook ↩
Bose & Mesner 1959 - Bose, R. C.; Mesner, D. M. (1959), "On linear associative algebras corresponding to association schemes of partially balanced designs", Annals of Mathematical Statistics, 30 (1): 21–38, doi:10.1214/aoms/1177706356, JSTOR 2237117, MR 0102157 http://projecteuclid.org/euclid.aoms/1177706356 ↩
Bose & Nair 1939 - Bose, R. C.; Nair, K. R. (1939), "Partially balanced incomplete block designs", Sankhyā, 4 (3): 337–372, JSTOR 40383923 https://www.jstor.org/stable/40383923 ↩
Bannai & Ito 1984 - Bannai, Eiichi; Ito, Tatsuro (1984), Algebraic combinatorics I: Association schemes, Menlo Park, CA: Benjamin/Cummings, ISBN 0-8053-0490-8, MR 0882540 https://mathscinet.ams.org/mathscinet-getitem?mr=0882540 ↩
Godsil 1993 - Godsil, C. D. (1993), Algebraic Combinatorics, New York: Chapman and Hall, ISBN 0-412-04131-6, MR 1220704 https://mathscinet.ams.org/mathscinet-getitem?mr=1220704 ↩
Zieschang 2005b - Zieschang, Paul-Hermann (2005b), Theory of association schemes, Springer, ISBN 3-540-26136-2 ↩
Zieschang 2005a - Zieschang, Paul-Hermann (2005a), "Association Schemes: Designed Experiments, Algebra and Combinatorics by Rosemary A. Bailey, Review" (PDF), Bulletin of the American Mathematical Society, 43 (2): 249–253, doi:10.1090/S0273-0979-05-01077-3 https://www.ams.org/bull/2006-43-02/S0273-0979-05-01077-3/S0273-0979-05-01077-3.pdf ↩
Dembowski 1968, pg. 281, footnote 1 - Dembowski, P. (1968), Finite Geometries, Springer, ISBN 978-3-540-61786-0 https://books.google.com/books?id=NJy_iTT_wGMC ↩
Bannai & Ito 1984, pg. vii - Bannai, Eiichi; Ito, Tatsuro (1984), Algebraic combinatorics I: Association schemes, Menlo Park, CA: Benjamin/Cummings, ISBN 0-8053-0490-8, MR 0882540 https://mathscinet.ams.org/mathscinet-getitem?mr=0882540 ↩
Street & Street 1987, pg. 238 - Street, Anne Penfold; Street, Deborah J. (1987), Combinatorics of Experimental Design, Oxford U. P. [Clarendon], ISBN 0-19-853256-3 ↩