A direct and simple proof of Jacobi identities for determinants

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  • Title: A direct and simple proof of Jacobi identities for determinants
  • ArXiv ID: 0712.1932
  • Date: 2007-12-13
  • Authors: – 저자 정보가 제공되지 않았습니다.

📝 Abstract

The Jacobi identities play an important role in constructing the explicit exact solutions of a broad class of integrable systems in soliton theory. In the paper, a direct and simple proof of the Jacobi identities for determinants is presented by employing the Pl$\ddot{u}$cker relations.

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Let A = a ij n×n be a n-order matrix. Denoted by M ij R ij ≡ (-1) i+j M ij the cofactor (algebraic cofactor) of the matrix entry a ij . The cofactor (algebraic cofactor) of the minor determinant a ij a il a kj a kl is denoted by M i j k l R i j k l ≡ (-1) k+l+i+j M i j k l , then the following Jacobi identities [1,2] M ii M jj -M ij M ji = M i j i j det A, 1 ≤ i, j ≤ n, (1) are valid. Though the Jacobi identities have been proved in [1], as the author in [2] said, looking at the proof of the general case, it is difficult to understand the Jacobi identities immediately and the author himself came to understand the result by checking the formulae using computer algebra, looking for an alternative proof and applying it to actual problems. Here we will present a direct proof for the Jacobi identities using the famous Plücker relations for determinants.

In this section, let’s state the Plücker relations for determinants.

where

On the other hand, by the classical Laplace expansion for determinants, it can be obtained that

Comparing the above two equations, we have

where

Corollary 2.2. Let M be a n×(n-2) matrix and a, b, c and d four n-order column vectors , then

Remark 2.3. The above equation (5) is the simplest case of the Plücker relations [2] which plays an important role in nonlinear dynamics and soliton theory due to Sato’s theorem [3,4]. It shows that many of the differential and difference equations in mathematical physics are merely disguised versions of the Plücker relations. For example, Sato [3,4] first discovered that the KP equation in bilinear form

was nothing but a Plücker relation, where the Hirota’s bilinear operators D t , D x and D y are defined by

Remark 2.4. The other forms of Plücker relations have been widely applied to algebraic geometry. For example, a projective embedding of the Grassmann variety Gr(p, n) can be defined by the quadratic polynomial equations called “the Plücker relations” (to see [5] and its references).

Remark 2.5. The Plücker relations are also exactly relational to the Maya diagrams and Young diagrams [2]. It makes them play a primary role in Combinatorics, Lie theory and Representation Theory (to see [6,7] and their references).

Theorem 3.1. Let A = a ij n×n be a n-order matrix. Denoted by M i j k l the cofactor of the minor determinant a ik a il a jk a jl , then

Proof. It is no less of generality to consider the case of i < j and k < l < s < r. Denoted by M the (n -2) × (n -4) submatrix obtained by eliminating the i-th and j-th rows and the k-th, l-th, s-th and r-th columns from A. The four (n -2)-order column vectors obtained by eliminating the i-th and j-th components from the k-th, l-th, s-th and r-th column vectors in A are denoted by a, b, c and d respectively. Then it is easy to see that

) k+r M a d ; M i j l s = (-1) l+s M b c . Consequently, by employing the Plücker relation (5), one has

Remark 3.2. Note that only the indices are important in the equation (7), so it can also be expressed as

which is nothing but a Plücker relation.

Theorem 3.3. Let A = a ij n×n be a n-order matrix. Denoted by

the cofactor of the minor determinant

. Choosing r rows and 2r columns from A, the according row and column indices are denoted by

where

Proof. It is completely similar to the proof of the above theorem 3.1 by employing the equation (2). So here we omit it.

Theorem 3.4. (Jacobi identity [1,2]) Let A = a ij n×n be a n-order matrix. Denoted by M ij the cofactor of the matrix entry a ij in A. The cofactor of the minor determinant a ij a il a kj a kl is denoted by M i j k l , then

Proof. It is no less generality to condider the special case with i = 1 and j = 2. Firstly, it is easy to see that

Then

On the other hand, by the equation ( 7), it can be obtained that

Therefore, by employing the Laplace expasion for determinants, one has

Remark 3.5. The Jacobi identities play an important role in soliton theory.

For example [2], if the solutions to the KP equation or the Toda lattice equation are expressed as Grammian determinants, their bilinear equations are nothing but the Jacobi identities.

Corollary 3.6. Let A = a ij 2n×2n be a 2n-order antisymmetric matrix, then det A is equal to a perfect square of a polynomial of its matrix entries

Proof. Following the above symbols, it is obvious that M 11 = M 22 = 0 and M 12 = -M 21 . Hence using the Jacobi identities, it can be obtained that

Note that det A = a 2

12 when n = 1, and M 1 2 1 2 is the determinant of a 2(n-1)-order antisymmetric matrix. Therefore, it can be deduced that det A is a perfect square of a polynomial of a ij (1 ≤ i, j ≤ n) by the recurrence relation (10). Remark 3.7. Recalling the definition of a Pfaffian, the square of a n-order Pfaffian is equal to the determinant of a 2n-order antisymmetric matrix. The above corollary in a sense ensures that a Pfaffian is well defined. On the other hand, by the Pfaffian expression for determinants, the terms of Jacobi identities (9) can be express

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