In this paper we explore the close and interesting relationship of a three-dimensional Euclidean Jordan algebra to the adjacency matrix of a strongly regular graph. According to [1] , the Jordan algebras were formally introduced in 1934 by Pascual Jordan, John von Neumann and Eugene Wigner in [2] . There, the authors attempted to deduce some of the Hermitian matrix properties and they came across a structure lately called a Jordan algebra. Euclidean Jordan algebras were born by adding an inner product with a certain property to a Jordan algebra. It is remarkable that Euclidean Jordan algebras turned out to have such a wide range of applications. For instance, we may cite the application of this theory to statistics [3] , interior point methods [4] [5] and combinatorics [6] . More detailed literature on Euclidean Jordan algebras can be found in Koecher’s lecture notes [7] and in the monograph by Faraut and Korányi [8] .

Along this paper, we consider only simple graphs, i.e., graphs without loops and parallel edges, herein called graphs. Considering a graph X, we denote its vertex set by and its edge set by―an edge whose endpoints are the vertices x and y is denoted by xy. In such case, the vertices x and y are adjacent or neighbors. The number of vertices of X, , is called the order of X.

A graph in which all pairs of vertices are adjacent (non-adjacent) is called a complete (null) graph. The number of neighbors of a vertex v in is called the degree of v. If all vertices of a graph X have degree k, for some natural number k, then X is k-regular.

We associate to X an n by n matrix, where each, if, otherwise, called the adjacency matrix of X. The eigenvalues of A are simply called the eigenvalues of X.

A non-null and not complete graph X is -strongly regular; if it is k-regular, each pair of adjacent vertices has a common neighbors and each pair of non-adjacent vertices has c common neighbors. The parameters of a -strongly regular graph are not independent and are related by the equality

It is also well known (see, for instance, [9] ) that the eigenvalues of a -strongly regular graph X are k, and, where and are given by

Therefore, the usually called restricted eigenvalues and are such that the former is positive and the latter is negative. Their multiplicities can be obtained as follows (see, for instance, [10] ):

Taking into account the above eigenvalues and their multiplicities, the following additional conditions are widely used as feasible conditions for parameters sets of strongly regular graphs; that is, if is a parameter set of a strongly regular graph, then the equality (1) and each one of the following inequalities holds:

・ The nontrivial Krein conditions obtained in [11] :

・ The Seidel’s absolute bounds qre (see [12] ):

With these conditions, many of the parameter sets are discarded as possible parameters sets of strongly regular graphs. To decide whether a set of parameters is the parameter set of a strongly regular graph is one of the main problems on the study of strongly regular graphs. It is worth noticing that these Krein conditions and the Seidel’s absolute bounds are special cases of general inequalities obtained for association schemes.

An association scheme with classes is a finite set S together with relations defined on S satisfying the following conditions.

1) The set of relations is a partition of the Cartesian product of.

2).

3) If, then also, and for.

4) For each the number of elements such that and depends only from, and.

The numbers are called the intersection numbers of the association scheme. Some authors call this type of association schemes symmetric association schemes. The relations of the association scheme can be re-

presented by their adjacency matrices of order defined by We may

say that is the adjacency matrix of the graph, with and. The Bose-Mesner algebra of the association scheme (introduced in [13] ) is defined, using these matrices, by the following conditions, which are equivalent to the conditions 1) - 4) of the association scheme:

1),

2),

3),

4),

where is the matrix of order n whose entries are equal to one and is the identity matrix of order. From 1) we may conclude that the matrices are linearly independent, and from 2) - 4) it follows that they generate a commutative -dimensional algebra of symmetric matrices with constant diagonal. The matrices commute and then, they can be diagonalized simultaneously, i.e., there exists a matrix such that, is a diagonal matrix. Thus, the algebra is semisimple and has a unique complete system of

orthogonal idempotents. Therefore, and, where

This paper is organized as follows. In Section 2, a short introduction on Euclidean Jordan algebras with the fundamental concepts is presented. In order to obtain new feasible conditions for the existence of a strongly regular graph, in Section 3, we define the generalized Krein parameters of a strongly regular graph. In Section 4, we establish some relations between the Krein parameters and the generalized Krein parameters, and present some properties of the generalized Krein parameters. Finally, since the generalized Krein parameters are nonnegative we establish new admissibility conditions, for the parameters of a strongly regular graph that give different information from that given by the Krein conditions 6) - 7).

In this section the main concepts of Euclidean Jordan Algebras that can be seen for instance in [8] , are shortly surveyed.

Let be a real vector space with finite dimension and a bilinear mapping from to, that satisfies,. Then, is called a real power associative algebra. If contains an element, e, such that for all u in, , then e is called the unit element of. Considering a bilinear mapping, if for all and in we have and , with, then is called a Jordan algebra. If is a Jordan algebra with unit element, then is power associative (cf. [8] ). Given a Jordan algebra with unit element, if there is an inner product that verifies the equality, for any u, v, w in, then is called an Euclidean Jordan algebra. An element in an Euclidean Jordan algebra, with unit element, is an idempotent if. Two idempotents and are orthogonal if. We call the set a complete system of orthogonal idempotents if (i),; (ii), and (iii).

Let be an Euclidean Jordan algebra with unit element e. Then, for every u in, there are unique distinct real numbers, and an unique complete system of orthogonal idempotents such that

with, (see [8] , Theorem III 1.1). These’s are the eigenvalues of u and (9) is called the first spectral decomposition of u.

The rank of an element u in is the least natural number k, such that the set is linear dependent (where), and we write. This concept is expanded by defining the rank of the algebra as the natural number. The elements of with rank equal to the rank of are the regular elements of. This set of regular elements is open and dense in. If u is a regular element of, with, then the set is linearly dependent and the set is linearly independent. Thus we may conclude that there exist unique real numbers, such that, where 0 is the null vector of. Therefore, with the necessary adjustments, we obtain the following polynomial in: This polynomial is called the characteristic polynomial of u, where each coefficient is a homogeneous polynomial of degree in the coordinates of in a fixed basis of. Although we defined the characteristic polynomial for a regular element of, we can extend this definition to all the elements in, because each polynomial is homogeneous and, as above referred, the set of regular elements of is dense in. The roots of the characteristic polynomial of, are called the eigenvalues of. Furthermore, the coefficients and in the characteristic polynomial of u, are called the trace and the determinant of, respectively.

From now on, we consider the Euclidean Jordan algebra of real symmetric matrices of order, , such that, , where is the usual product of matrices. Furthermore, the inner product of is defined as, where is the classical trace of matrices, that is the sum of its eigenvalues.

Let be a -strongly regular graph such that, and let be the adjacency matrix of. Then has three distinct eigenvalues, namely the degree of regularity, and the restricted eigenvalues and, given in (2) and (3). Now we consider the Euclidean Jordan subalgebra of, , spanned by the identity matrix of order, , and the powers of. Since has three distinct eigenvalues, then is a three dimensional Euclidean Jordan algebra with and is a basis of.

Let be the unique complete system of orthogonal idempotents of associated to. Then

where is the matrix whose entries are all equal to 1. Since is an Euclidean Jordan algebra that is closed for the Hadamard product of matrices, denoted by and is a basis of, then there exist real numbers and, , , , such that

The real numbers, defined in (11), (whose notation will be clarified later) and, , , , are called the “classical” Krein parameters of the graph (cf. [10] ). Since and, the “classical” Krein admissibility conditions, and (presented in [9] , Theorem 21.3) can be deduced.

Herein the generalized Krein parameters of a -strongly regular graph are defined and then, necessary conditions for the existence of a -strongly regular graph are deduced. These conditions are generalizations of the Krein conditions (see Theorem 21.3 in [9] ). Throughout this paper we use a slight different notation from classical books like [9] [14] , because, in this way, the connections between the “classical’’ and the generalized parameters are better understood. Now we generalize the Krein parameters in order to obtain new generalized admissibility conditions on the parameters of strongly regular graphs. Firstly, considering defined like in (10) in the Basis, and rewriting the idempotents under the new basis of we obtain

Consider the natural number and denote by the set of square matrices of order with real entries. Then for, we denote by and the Hadamard power of order of B and the Kronecker power of order of, respectively, with and.

Now, we introduce the following compact notation for the Hadamard and the Kronecker powers of the elements of S. Let x, y, z, , and be natural numbers such that, and. Then we define

Again, since the Euclidean Jordan algebra is closed under the Hadamard product and is a basis of, then there exist real numbers, , and, such that

We call the parameters and defined in (13) the generalized Krein parameters of the strongly re- gular graph. Notice that and are precisely the Krein parameters of already presented. With this notation, the Greek letters are used as idempotent indices and the Latin letters are used as exponents of Hadamard (Kronecker) powers.

In this section we prove that the generalized Krein parameters can be expressed in function of the Krein parameters. Before that, it is worth to mention that the previously introduced generalizations are straightforward extended to the Krein parameters of symmetric association schemes with classes, see [9] . Notice that the algebra spanned by the matrices of a symmetric association scheme with d classes is an Euclidean Jordan

Algebra with rank and with the Jordan product where is the usual product of

matrices. Furthermore, the inner product of is defined as where is the classical trace of matrices, that is, the sum of its eigenvalues. Let us consider the matrices and of the Bose-Mesner algebra of an association scheme with classes as defined in [14] . However, for convenience, we denote this

matrix such as defined in [14] by. Therefore, we can say that, see [14] . Hence, we can say

that the matrices and satisfy,

The matrices and are usually called the eigenmatrix and the dual eigenmatrix of the association scheme, respectively.

Theorem 1. Let be a -strongly regular graph such that whose adjacency matrix is and has the eigenvalues and and whose eigenmatrix and dual eigenmatrix matrix are respectively and If and are natural numbers such that then

Proof. Consider that is the of idempotents defined in (12) and the following notation, and

For since and, it follows that

Therefore and since implies we obtain

Finally, from (19) the result follows.

Theorem 2. Let be a -strongly regular graph such that whose adjacency matrix is and has the eigenvalues and and whose eigenmatrix and dual eigenmatrix matrix are respectively and Let and be natural numbers such that Then

Proof. Taking into account that and by the equalities (21) and (22)

we conclude that Therefore and since by (22)

we obtain. Hence

As an application of the Theorem 2 we may conclude that considering a strongly regular graph the generalized Krein parameters can be expressed in function of the classical Krein parameters as follows:

The expression (23) is obtained using (14) and (20). Summarizing, we have the following corollary.

Corollary 1. Let be a -strongly regular graph such that Then for all natural numbers and such that

Theorem 3. Let be a -strongly regular graph such that Then for all natural numbers and such that

Proof. We have Since from (21) then

. Hence we obtain

Therefore, the equality (25) follows.

Recurring to (14) and (25), we may conclude the Corollary 2.

Corollary 2. Let be a -strongly regular graph such that Then for all natural numbers and such that,

Theorem 4. Let be a -strongly regular graph such that Then and

Proof. We prove by induction on n. For the inequality (26) holds, since the classical Krein parameters are nonnegative and Now assuming that the inequality (26) holds for, we prove that (26) also holds for Consider the sum Then from (14), we obtain

Since for the inequality (26) is verified and the summands are nonnegative, we may conclude that

Recurring to the Theorem 4 we are conducted to the Corollaries 3 and 4.

Corollary 3. Let G be a -strongly regular graph such that Then for all natural numbers and such that the generalized Krein parameters are nonnegative.

Corollary 4. Let be a -strongly regular graph such that Then for all natural numbers and s such that the generalized Krein parameters are nonnegative.

Theorem 5. Let G be a strongly regular graph and let i, s and m be natural numbers such that Then

Proof. Recurring to the inequalities (14)-(17) we have:

Theorem 6. Let G be a -strongly regular graph such that. Let and s be natural numbers such that and Then the generalized Krein parameter satisfy

Proof. Similar to the Proof done in Theorem 5.

Let G be a -strongly regular graph such that Since the generalized Krein parameters and are nonnegative then we can establish new admissibility conditions distinct from the Krein conditions (6) and (7). For instance, the generalized Krein condition allows us to establish a new theorem on strongly regular graphs after some algebraic manipulation of its expressions. Analyzing the generalized Krein parameter of a strongly regular graph with one in its spectra we deduce the following theorem (7).

Theorem 7. Let be a -strongly regular graph such that whose adjacency matrix is and has the eigenvalues and If then

Proof. Since then we have

From the inequality (28) and after some simplifications we conclude that

Therefore if then

Finally we have

Dividing both members of (29) by we are supposing that we obtain

¹We must note that the equation as the roots and the root Since implies that and finally this implies that therefore

Now from the inequality (30) we conclude that if is a -strongly regular graph with one in his

spectra1 then implies that

We now present in Table 1 some examples of parameter sets that do not verify the inequality (27) of Theorem 7. We consider the parameter sets, , , and. For each example we present the respective eigen-

values, and the value of defined by

In this paper, we have generalized the Krein parameters of a strongly regular graph and obtained some relations

between the classical Krein parameters and the generalized Krein parameters (see Corollaries 1 and 2). We also establish that these generalize Krein parameters are always positive and less than one (see Corollaries 3 and 4, and Theorems 5 and 6). Let and s be natural numbers such that The generalized Krein admissibility conditions with and with allow us to establish new admissibility conditions; they permit us to establish new inequalities on the parameters of a strongly regular graph. For instance the generalized Krein parameter condition after some algebraic manipulation allows us to establish the inequality (27) in Theorem 7. Finally, we conclude that we can extend the definition of generalized Krein parameters to a symmetric association scheme with classes.

1) Luís Almeida Vieira was supported by the European Regional Development Fund through the program COMPETE and by the Portuguese Government through the FCT―Fundação para a Ciência e a Tecnologia under the project PEst―C/MAT/UI0144/2013.

2) Vasco Moço Mano was partially supported by Portuguese Funds trough CIDMA―Center for Research and development in Mathematics and Applications, Department of Mathematics, University of Aveiro, 3810-193, Aveiro, Portugal and the Portuguese Foundation for Science and Technology (FCT-Fundação para a Ciência e Tecnologia), within Project PEst-OE/MAT/UI4106/2014.

3) The authors would like to thank the anonymous referee for his/her careful revision and relevant comments that improved our paper.