Classification of homogeneous Fourier matrices

Modular data are commonly studied in mathematics and physics. A modular datum defines a finite-dimensional representation of the modular group SL₂(Z). In this paper, we show that there is a one-to-one correspondence between Fourier matrices associated to modular data and self-dual C-algebras that s...

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Zitieren:Classification of homogeneous Fourier matrices / G. Singh // Algebra and Discrete Mathematics. — 2019. — Vol. 27, № 1. — С. 75–84. — Бібліогр.: 7 назв. — англ.

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2023-02-28T19:14:51Z
2023-02-28T19:14:51Z
2019
Classification of homogeneous Fourier matrices / G. Singh // Algebra and Discrete Mathematics. — 2019. — Vol. 27, № 1. — С. 75–84. — Бібліогр.: 7 назв. — англ.
1726-3255
2010 MSC: Primary 05E30; Secondary 05E99, 81R05.
https://nasplib.isofts.kiev.ua/handle/123456789/188424
Modular data are commonly studied in mathematics and physics. A modular datum defines a finite-dimensional representation of the modular group SL₂(Z). In this paper, we show that there is a one-to-one correspondence between Fourier matrices associated to modular data and self-dual C-algebras that satisfy a certain condition. We prove that a homogenous C-algebra arising from a Fourier matrix has all the degrees equal to 1.
en
Інститут прикладної математики і механіки НАН України
Algebra and Discrete Mathematics
Classification of homogeneous Fourier matrices
Article
published earlier
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
title Classification of homogeneous Fourier matrices
spellingShingle Classification of homogeneous Fourier matrices
Singh, G.
title_short Classification of homogeneous Fourier matrices
title_full Classification of homogeneous Fourier matrices
title_fullStr Classification of homogeneous Fourier matrices
title_full_unstemmed Classification of homogeneous Fourier matrices
title_sort classification of homogeneous fourier matrices
author Singh, G.
author_facet Singh, G.
publishDate 2019
language English
container_title Algebra and Discrete Mathematics
publisher Інститут прикладної математики і механіки НАН України
format Article
description Modular data are commonly studied in mathematics and physics. A modular datum defines a finite-dimensional representation of the modular group SL₂(Z). In this paper, we show that there is a one-to-one correspondence between Fourier matrices associated to modular data and self-dual C-algebras that satisfy a certain condition. We prove that a homogenous C-algebra arising from a Fourier matrix has all the degrees equal to 1.
issn 1726-3255
url https://nasplib.isofts.kiev.ua/handle/123456789/188424
citation_txt Classification of homogeneous Fourier matrices / G. Singh // Algebra and Discrete Mathematics. — 2019. — Vol. 27, № 1. — С. 75–84. — Бібліогр.: 7 назв. — англ.
work_keys_str_mv AT singhg classificationofhomogeneousfouriermatrices
first_indexed 2025-11-25T20:37:34Z
last_indexed 2025-11-25T20:37:34Z
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fulltext “adm-n1” — 2019/3/22 — 12:03 — page 75 — #83 Algebra and Discrete Mathematics RESEARCH ARTICLE Volume 27 (2019). Number 1, pp. 75–84 c© Journal “Algebra and Discrete Mathematics” Classification of homogeneous Fourier matrices Gurmail Singh Communicated by V. V. Kirichenko Abstract. Modular data are commonly studied in mathe- matics and physics. A modular datum defines a finite-dimensional representation of the modular group SL2(Z). In this paper, we show that there is a one-to-one correspondence between Fourier matrices associated to modular data and self-dual C-algebras that satisfy a certain condition. We prove that a homogenous C-algebra arising from a Fourier matrix has all the degrees equal to 1. 1. Introduction The set of columns of a Fourier matrix with entrywise multiplication and usual addition generate a fusion algebra over C, see [4]. But a two- step rescaling on Fourier matrices gives rise to the self-dual C-algebras. A C-algebra with all equal degrees except the trivial degree is called a homogeneous C-algebra and we call the associated Fourier matrix a homogenous Fourier matrix. We use the properties of self-dual C-algebras to classify homogeneous Fourier matrices, and to establish a one-to-one correspondence between Fourier matrices and the self-dual C-algebras. In Section 2, we collect the definitions and introduce a two-step rescal- ing of Fourier matrices to construct the C-algebras from Fourier matrices. In Section 3, we establish some properties of C-algebras that arise from Fourier matrices. Also, we show that there is a one-to-one correspondence between Fourier matrices and self-dual C-algebras that satisfy a certain 2010 MSC: Primary 05E30; Secondary 05E99, 81R05. Key words and phrases: modular data, Fourier matrices, fusion rings, C-algebras. “adm-n1” — 2019/3/22 — 12:03 — page 76 — #84 76 Homogeneous Fourier matrices integrality condition. In Section 4, we prove that every homogeneous C-algebra arising from a Fourier matrix has all the degrees equal to 1, and such a C-algebra with nonnegative structure constants is a group algebra. 2. C-algebras arising from Fourier matrices A scaling of the rows of a Fourier matrix gives the basis containing identity of a Fusion algebra. Here we introduce the two-step rescaling on Fourier matrices and construct C-algebras from them. Definition 1. Let A be a finite dimensional and commutative algebra over C with distinguished basis B = {b0 := 1A, b1, . . . , br−1}, and an R-linear and C-conjugate linear involution ∗ : A → A. Let δ : A → C be an algebra homomorphism. Then the triple (A,B, δ) is called a C-algebra if it satisfies the following properties: (i) for all bi ∈ B, (bi) ∗ = bi∗ ∈ B; (ii) for all bi, bj ∈ B, we have bibj = ∑ bk∈B λijkbk, for some λijk ∈ R; (iii) for all bi, bj ∈ B, λij0 6= 0 ⇐⇒ j = i∗; (iv) for all bi ∈ B, λii∗0 = λi∗i0 > 0; (v) for all bi ∈ B, δ(bi) = δ(bi∗) > 0. The algebra homomorphism δ is called a degree map, and δ(bi), for all bi ∈ B, are called the degrees. If δ(bi) = λii∗0, for all bi ∈ B, we say that B is a standard basis. The order of a C-algebra is denfined as n := δ(B+) = ∑r−1 i=0 δ(bi). A C-algebra is called symmetric if bi∗ = bi, for all i. A C-algebra with rational structure constants is called a rational C-algebra. The readers interested in C-algebras are directed to [1], [3] and [6]. To keep the generality, in the following definition of Modular data we assume the structure constants to be integers instead of nonnegative integers, see [4]. Definition 2. Let r ∈ Z+ and I an r × r identity matrix. A pair (S, T ) of r × r complex matrices is called a modular datum if (i) S is a unitary and symmetric matrix, that is, SS̄T = 1, S = ST , (ii) T is diagonal matrix and of finite multiplicative order, (iii) Si0 > 0, for 0 6 i 6 r− 1, where S is indexed by {0, 1, 2, . . . , r− 1}, (iv) (ST )3 = S2, (v) Nijk = ∑ l SliSljS̄lkS −1 l0 ∈ Z, for all 0 6 i, j, k 6 r − 1. Definition 3. A matrix S satisfying the axioms (i), (iii) and (v) of Definition 2 is called a Fourier matrix. “adm-n1” — 2019/3/22 — 12:03 — page 77 — #85 G. Singh 77 Let S be a Fourier matrix. Let s = [sij ] be the matrix with entries sij = Sij/Si0, for all i, j, and we call it an s-matrix associated to S (briefly, s-matrix). Since S is a unitary matrix, ss̄T = diag(d0, d1, . . . , dr−1) is a diagonal matrix, where di = ∑ j sij s̄ij . The numbers di are called norms of the s-matrix. The principal norm d0 (= S−2 00 ) is also known as the size of the modular datum, see [4, Definition 3.8]. The relation sij = Sij/Si0 implies the structure constants Nijk = ∑ l slisljslkd −1 l , for all i, j, k. Since the structure constants Nijk generated by the columns of S under entrywise multiplication are integers, the numbers Sij/Si0 are algebraic integers, see [4, Section 3]. Therefore, if S has only rational entries then the entries of s-matrix are rational integers, and such s-matrices are known as integral Fourier matrices, see [4, Definition 3.1]. Cuntz studied the integral Fourier matrices, see [4]. In this paper, we consider the broader class of s-matrices with algebraic integer entries. Note that an s-matrix satisfies all the axioms of the definition of an integral Fourier matrix except the entries may not be integers. For example, the first eigenmatrix (character table) of every group algebra of a group of prime order is an s-matrix but not an integral Fourier matrix. There is an interesting row-and-column operation (two-step rescaling) procedure that can be applied to a Fourier matrix S that results in the first eigenmatrix, the character table, of a C-algebra, see Theorem 1. The steps of the procedure are reversed to obtain the Fourier matrix S from the first eigenmatrix. The explanation of the procedure is as follows. Let S = [Sij ] be a Fourier matrix indexed with {0, 1, . . . , r−1}. We divide each row of S with its first entry and obtain the s-matrix. The multiplication of each column of the s-matrix with its first entry gives the P -matrix associated to S (briefly, P -matrix), the first eigenmatrix of the C-algebra. That is, sij = SijS −1 i0 and pij = sijs0j , for all i, j, where pij denotes the (i, j)-entry of the P -matrix. Conversely, to obtain the s-matrix from a P -matrix, divide each column of the P -matrix with the squareroot of its first entry. Further, the Fourier matrix S is obtained from the s-matrix by dividing the ith row of s-matrix by √ di, where di = ∑ j |sij |2. That is, sij = pij/ √ p0j , and Sij = sij/ √ di, ∀ i, j. Since the entries of an s-matrix are algebraic integers, the entries of P -matrix are also algebraic integers. Remark 1. Throughout this paper, unless mentioned explicitly, the set of the columns of P -matrix and s-matrix are denoted by B = {b0, b1, . . ., br−1} and B̃ = {b̃0, b̃1, . . . , b̃r−1}, respectively. The structure constants generated by the columns, with the entrywise multiplication, of P -matrix “adm-n1” — 2019/3/22 — 12:03 — page 78 — #86 78 Homogeneous Fourier matrices and s-matrix are denoted by λijk and Nijk, respectively. MT denotes the transpose of a matrix M . The columns of a Fourier matrix gives rise to a fusion algebra, see [4]. In the next theorem we show that corresponding to every Fourier matrix there exists a C-algebra. Theorem 1. Let S be a Fourier matrix. Then the vector space A := CB is a C-algebra of order d0, B is the standard basis of A, and P -matrix is the first eigenmatrix of A. Proof. The C-conjugate linear involution ∗ on columns of S is given by the involution on elements of S, defined as (Sij) ∗ = Sij∗ = S̄ij for all i, j. Therefore, if Sj denotes the jth column of a Fourier matrix S then the involution on Sj is given by (Sj) ∗ = Sj∗ = [S0j∗ , S1j∗ , . . . , S(r−1),j∗ ] T . Since bi = s0ib̃i, the structure constants generated by the basis B are given by λijk = Nijks0is0js −1 0k , for all i, j, k. As S is a unitary matrix, therefore, Nij0 = ∑ l SliSljS̄l0S −1 l0 6= 0 ⇐⇒ j = i∗ and Nii∗0 = 1 > 0, for all i, j. Hence, λij0 6= 0 ⇐⇒ j = i∗ and λii∗0 > 0, for all i, j. Define a C-conjugate linear map δ : A −→ C as δ( ∑ i aib̃i) = ∑ i āis0i. Thus δ(bi) = δ(s0ib̃i) = s20i, hence δ is positive valued. The map δ is an algebra homomorphism, to see: δ(bibj) = s0is0j ∑ k Nijkδ(b̃k) = s0is0j [ s0is0j d0 r−1 ∑ k=0 s̄0ks0k] + s0is0j [ r−1 ∑ l=1 slislj dl r−1 ∑ k=0 s̄lks0k] = s0is0j [ s0is0j d0 d0] + s0is0j [0] = s20is 2 0j = δ(bi)δ(bj). In the third last equality we use the fact that n ∑ k=1 s0ks̄0k = d0 and the rows of s-matrix are orthogonal. Since bi∗ = s̄0ib̃i∗ = s0ib̃i∗ , (bibi∗)0 = s0is0i(b̃ib̃i∗)0 = s20i = δ(bi). Therefore, δ is the positive degree map and B is the standard basis. The value of a basis element bj under an irreducible character (linear character) is given by pij , for all i, j. By Theorem 1, every Fourier matrix gives rise to a C-algebra. The algebra A in the above theorem is denoted by (A,B, δ), and we say (A,B, δ) is arising from a Fourier matrix S. A C-algebra arising from a Fourier matrix S of rank r is a symmetric C-algebra if and only if S ∈ Rr×r. “adm-n1” — 2019/3/22 — 12:03 — page 79 — #87 G. Singh 79 3. General results on C-algebras arising from Fourier matrices Let s be an integral Fourier matrix. Then √ djsij = √ disji, for all i, j. Therefore, d0 = diδ(bi) for all i, that is, the degrees and norms divide d0. This can be generalized to s-matrices under a certain condition. In the following proposition we prove that not only the list of the degrees of a C-algebra arising from a Fourier matrix matches with list of multiplicities but their indices also match. Also, we prove that a C-algebra arising from an integral Fourier matrix has perfect square integral degrees and rational structure constants. Proposition 1. Let (A,B, δ) be a C-algebra arising from a Fourier ma- trix S. Let mj be the multiplicity of A corresponding to the irreducible character χj. (i) The degrees of A exactly match with the multiplicities of A, that is, mj = δ(bj), for all j. (ii) If degrees of A are rational numbers then the degrees and norms are integers, and both the degrees and norms divide the order of A. (iii) If the associated s-matrix has integral entries then degrees of A are perfect square integers, and A is a rational C-algebra. (iv) If A is a rational C-algebra the degrees of A are integers. (v) A has unique degree if and only if s-matrix has unique norm. Proof. (i). The multiplicities, mj = δ(B+)/ r−1 ∑ i=0 |χj(bi∗ )| 2 λii∗0 , see [2, Corol- lary 5.6]. Therefore, mj = d0/ r−1 ∑ i=0 |sji|2 = d0/dj , for all j. Since S is a symmetric matrix, di|sji|2 = dj |sij |2. Thus d0/dj = s20j , for all j. Hence mj = d0/dj = s20j = δ(bj), for all j. (ii). The fact that the P -matrix has algebraic entries implies that the degrees of the algebra A are integers, consequently d0 is an integer. By the above part (i), dj = d0δ(bj) −1, for all j. Therefore, dj are rational numbers. The entries of s-matrix are algebraic integers, thus the norms dj are rational integers. Hence both the degrees and norms divide the order of A, because d0 = djδ(bj), for all j. (iii). The entries of s-matrix are integers and √ δ(bj) = s0j imply √ δ(bj) ∈ Z, for all j. By the proof of Theorem 1, λijk = (Nijk √ δ(bi) √ δ(bj))/ √ δ(bk), for all i, j, k. Hence λijk ∈ Q, for all i, j, k. (iv). Since A is a rational algebra, λijk ∈ Q. Therefore, δ(bi)=λii∗0∈Q, because B is a standard basis. But the entries of P -matrix are algebraic “adm-n1” — 2019/3/22 — 12:03 — page 80 — #88 80 Homogeneous Fourier matrices integers and δ(bi) = p0i, for all i. Therefore, δ(bi) are integers. (Though we remark that rationality of all the structure constants is not required.) (v). The result follows from the fact that d0 = diδ(bi), for all i. By Proposition 1 (i), a C-algebra arising from a Fourier matrix S is a self-dual C-algebra. But every self-dual C-algebra not necessarily arise from a Fourier matrix, see Example 1. Therefore, in general, the converse is not true. In the next theorem we prove that the converse is also true under a certain integrality condition. Theorem 2. Let (A,B, δ) be a C-algebra with standard basis B = {b0, b1, . . . , br−1}. Let λijk be the structure constants generated by the basis B. Then A is self-dual and λijk √ δ(bk)/ √ δ(bi)δ(bj) ∈ Z if and only if A arises from a Fourier matrix S. Proof. Suppose (A,B, δ) is a self-dual C-algebra and λijk √ δ(bk)/( √ δ(bi) √ δ(bj)) ∈ Z, for all i, j, k. Let P be the first eigenmatrix of A and I an identity matrix. Therefore, without loss of generality, assume PP̄ = d0I and mj = δ(bj), where mj is the multiplicity of an irreducible character χj . By [2, Theorem 5.5 (i)], pji/δ(bi) = pij/mj , implies pji/δ(bi) = pij/δ(bj), for all i, j. Let L = diag(1/ √ δ(b0), 1/ √ δ(b1), . . . , 1/ √ δ(br−1), and s = PL. Therefore, ss̄T = diag(d0/δ(b0), d0/δ(b1), . . . , d0/δ(br−1)) = diag(d0, d1, . . . , dr−1), where d0 = diδ(bi), di = ∑ j |sij |2 and sij = pij/ √ δ(bj), for all i, j. Also, sij √ dj = sij √ di, because pji/δ(bi) = pij/δ(bj), for all i, j.. Hence s is an s-matrix associated to a Fourier matrix S = [Sij ], where Sij = sij/ √ di, for all i, j. Since Nijk ∈ Z, the other direction follows from the Proposition 1(i). Remark 2. By Pontryagin duality, every group algebra of a finite abelian group is self-dual. A group algebra of a finite abelian group also satisfies the integrality condition of the above theorem. On the other hand, a self- dual C-algebra with a unique degree and nonnegative structure constants is a group algebra, see Theorem 3. Hence a self-dual C-algebra with nonnegative structure constants has a unique degree if and only if it is a group algebra of a finite abelian group. In the next example, we show that the condition λijk √ δ(bk)/( √ δ(bi) √ δ(bj)) ∈ Z cannot be removed. “adm-n1” — 2019/3/22 — 12:03 — page 81 — #89 G. Singh 81 Example 1. Since the row sum of a character table is zero, the character table of a C-algebra of rank 2 with basis B = {b0, bi} is given by P = [ 1 n 1 −1 ] , and the structure constants are given by b21 = nb0 + (n− 1)b1. (Note that, for n ∈ Z+, P is the first eigenmatrix of an association scheme of order n+ 1 and rank 2.) Apply the two-step scaling on the matrix P , we obtain S = 1√ n+ 1 [ 1 √ n√ n −1 ] . But for 1 6= n ∈ R+, the condition λijk √ δ(bk)/ √ δ(bi)δ(bj) ∈ Z is not satisfied, because λ111/ √ n 6∈ Z, and the matrix S is not a unitary matrix. Cuntz proved that the size of every integral Fourier matrix with odd rank is a square integer, [4, Lemma 3.7]. In the following lemma we generalize the Cuntz’s result. Lemma 1. Let (A,B, δ) be a C-algebra arising from a Fourier matrix S with rank r. Let r be an odd integer. If determinant of the P -matrix is an integer then the order of A is a square integer. Proof. Let det(P ) denote the determinant of P -matrix. A is a self dual C-algebra, thus PP̄ = nI implies (det(P ))2 = nr, where n is the order of A. Since r is an odd integer, √ n is an integer. 4. Homogeneous C-algebras arising from Fourier matrices In this section we show that every homogenous C-algebra arising from a Fourier matrix has unique degree, and such a C-algebra under a certain condition is a group algebra. In the following lemma we prove that if a degree of a C-algebra arising from a Fourier matrix divides the all nontrivial degrees then that degree might be equal to 1. Lemma 2. Let (A,B, δ) be a C-algebra arising from a Fourier matrix S such that the degrees δ(bi) ∈ Z, for all i. If for a given j, δ(bj) divides δ(bi) for all i > 1, then δ(bj) = 1, for all j. Proof. The degrees δ(bi) are integers, therefore, by Proposition 1(ii), dj are integers. Since d0 = 1+ r−1 ∑ i=1 δ(bi), (1 + r−1 ∑ i=1 δ(bi))δ(bj) −1 = δ(bj) −1+α ∈ Z, where α ∈ Z. Hence δ(bj) = 1, for all j. “adm-n1” — 2019/3/22 — 12:03 — page 82 — #90 82 Homogeneous Fourier matrices Note that, the above lemma is true for any self-dual C-algebra with integral norms and degrees. We can apply this lemma to recognize some C- algebras not arising from s-matrices just by looking at the degree pattern (or the first row of the character table) of a C-algebra. For example, the character tables of the association schemes as5(2), as9(2), as9(3), as9(8) and as9(9) violate the above result so they are not the character tables of the adjacency algebras arising from Fourier matrices. For the character tables of the association schemes see [5]. Definition 4. Let (A,B, δ) be a C-algebra arising from a Fourier matrix S. Let t ∈ R+ and δ(bi) = t, for all 1 6 i 6 r − 1. Then A is called a homogenous C-algebra with homogeneity degree t, and the associated Fourier matrix S is called a homogeneous Fourier matrix. In the next proposition, we prove that if a C-algebra arising from a Fourier matrix S is either homogeneous, or of prime order with integral degrees then each degree of the algebra is equal to 1. Proposition 2. Let (A,B, δ) be a C-algebra arising from a Fourier ma- trix S. (i) If A is a homogenous C-algebra then A has unique degree, that is, δ(bi) = 1, for all i. (ii) If the order of A is a prime number and δ(bi) ∈ Z+, for all i, then δ(bi) = 1, for all i. Proof. (i). Let t be the homogeneity degree of A. If the rank of A is 2 then the result holds trivially, see Example 1. Suppose t ∈ R+\Q+. Let bi, bj be two nonidentity elements of B such that bj 6= bi∗ . Therefore, the support of b̃ib̃j does not contain the identity element, because λij0 = 0 implies Nij0 = 0. Note that the first entry of the column vector b̃ib̃j is t. To obtain t from the linear combinations of the nonidentity elements of B̃ the structure constants Nijk must involve √ t, because the first entry of each column of s-matrix is √ t except the first column. Therefore, the structure constants Nijk cannot be integers, a contradiction. Thus t ∈ Q+. The entries of the P -matrix are algebraic integers, thus t must be an integer. Therefore, t divides δ(bi) for all i > 0. Hence by Lemma 2, t = 1, that is, δ(bi) = 1, for all i. (ii). By Proposition 1 (ii), δ(bi) divides d0, for all i. But d0 is a prime number, therefore, δ(bi) = 1, for all i. Michael Cuntz made a conjecture that is a generalization to his result, see [4, Lemma 3.11]. The conjecture states that if s is an integral Fourier “adm-n1” — 2019/3/22 — 12:03 — page 83 — #91 G. Singh 83 matrix with unique norm, then s ∈ {±1}r×r, see [4, Conjecture 3.10]. The conjecture cannot be extended to non-real s-matrices, the trivial contradiction is the character tables of cyclic groups of prime order. Note that if all the structure constants are nonnegative then |pij | 6 p0j (or equivalently, |sij | 6 s0j) for all j, see [7, Proposition 4.1]. The next theorem completely classify the s-matrices under the conditions of Proposition 2 and |pij | 6 p0j , for all j. It also shows that even for real s-matrices it is not necessary to pre-assume the uniqueness of the norm to get all entries of s-matrices equal to ±1. Theorem 3. Let (A,B, δ) be a C-algebra arising from a Fourier matrix S. Suppose A is either a homogeneous C-algebra, or A has prime order and integral degrees. Let |sij | 6 s0j, for all i, j. (i) The modulus of each entry of the s-matrix is 1, that is, |sij | = 1, for all i, j. (ii) The columns of the s-matrix form an abelian group under entrywise multiplication. (iii) If s-matrix is a real matrix then the columns of s-matrix form an elementary abelian group. Proof. (i). By Theorem 2, δ(bj) = 1, for all j. Therefore, dj = d0, for all j. Since |sij | 6 1, |sij | = 1, for all i, j. (ii). Let si be the i-th column of s-matrix and let sisj be the entrywise multiplication of si and sj . For a column sk of s, each entry of sisjsk has modulus value 1, and the sum of the entries of sisjsk cannot be −r because s0l = 1, for all l. But the structure constants Nijk = 1 r ∑ l slisljslk are integers. Therefore, Nijk are either 0 or r. Since sisj is a nonzero vector, it cannot be orthogonal to all the columns of s-matrix. Thus sisj = sk for some column sk of s. Therefore, the columns of s-matrix are closed under entrywise multiplication. The first column of s-matrix serves as an identity of the group of columns of s-matrix under entrywise multiplication. (iii). Let s be a real matrix. Since |sij | = 1, sij = ±1. Thus, by Part (ii), s is a group. Hence s is a character table of an elementary abelian group of order r. If an s-matrix of rank r has unique norm then the Fourier matrix S = r−1/2s. Thus the above theorem also classifies the homogeneous Fourier matrices under the same condition. References [1] Z. Arad, E. Fisman, and M. Muzychuk, Generalized table algebras, Israel J. Math., 114, 1999, 29-60. “adm-n1” — 2019/3/22 — 12:03 — page 84 — #92 84 Homogeneous Fourier matrices [2] E. Bannai and T. Ito, Algebraic Combinatorics I: Association Schemes, Ben- jamin/Cummings, Menlo Park, CA, 1984. [3] Harvey I. Blau, Table algebras, European J. Combin., 30(6), 2009, 1426-1455. [4] Michael Cuntz, Integral modular data and congruences, J Algebr Comb., 29, 2009, 357-387. [5] A. Hanaki and I. Miyamoto, Classification of Small Association Schemes. (http://math.shinshu-u.ac.jp/ hanaki/as/) [6] D. G. Higman, Coherent algebras, Linear Algebra Appl., 93, 1987, 209-239. [7] Bangteng Xu, Characters of table algebras and applications to association schemes, Journal of Combinatorial Theory, Series A 115, 2008, 1358-1373. Contact information G. Singh Department of Mathematics and Statistics, University of Regina, Regina, Saskatchewan, Canada, S4S 0A2 E-Mail(s): Gurmail.Singh@uregina.ca Received by the editors: 14.04.2017 and in final form 19.02.2018.