For the generic n×nn\times n matrix A=(aij)A=(a_{ij}) over the free field, Gelfand–Krob–Lascoux–Leclerc–Retakh–Thibon (1995) proved a noncommutative Cayley–Hamilton theorem ∑j(−1)jLj(A)An−j=0\sum_j(-1)^jL_j(A)A^{n-j}=0, where Lj(A)L_j(A) is a diagonal matrix whose entries Lj(i)(A)L_j^{(i)}(A) are the coefficients of the nn pseudo-characteristic polynomials Qi(t)Q_i(t) obtained from the rationality of the series ∣I−tA∣ii−1|I-tA|_{ii}^{-1}. Generically these coefficients are complicated rational expressions involving inverses of the entries, and they depend on the row index ii. The paper poses the problem of investigating two classes of specializations of the generic matrix: (1) matrices for which all Lj(i)(A)L_j^{(i)}(A) are polynomials in the entries, and (2) matrices for which Lj(i)(A)L_j^{(i)}(A) is independent of ii, so that the characteristic polynomial is essentially scalar. The matrix EnE_n of standard generators of U(gln)U(gl_n) lies in both classes (its pseudo-determinants equal the Capelli determinant), while the quantum matrix AqA_q of GLq(n)GL_q(n) lies in the first only. Three decades of later work have produced many further example families — quantum matrix algebras of orthogonal, symplectic and super type, reflection-equation algebras, Manin and qq-Manin matrices — together with neighbouring universal-identity frameworks, but no necessary-and-sufficient characterization of either class is known. The problem of systematically characterizing these two classes remains open.

Background

The classical Cayley–Hamilton theorem states that a square matrix over a commutative ring is annihilated by its own characteristic polynomial. When the entries of a matrix do not commute, there is no single determinant and the theorem has no obvious analogue. A systematic noncommutative linear algebra was built from the quasi-determinant: for a matrix A=(aij)A=(a_{ij}) with noncommuting invertible entries, the (i,j)(i,j)-quasi-determinant ∣A∣ij|A|_{ij} is the inverse of the (j,i)(j,i)-entry of A−1A^{-1}, and it behaves as a noncommutative analogue of a ratio of two determinants (Gelfand–Retakh, Selecta Math. 3 (1997) 517–546). Rational expressions in noncommuting variables live naturally in the free field, the universal skew field of fractions of the free algebra K⟨aij⟩K\langle a_{ij}\rangle, which plays the role of the field of rational functions.

Gelfand, Krob, Lascoux, Leclerc, Retakh and Thibon developed the theory of noncommutative symmetric functions — the free graded algebra Sym⁡=K⟨Λ1,Λ2,…⟩\operatorname{Sym}=K\langle\Lambda_1,\Lambda_2,\ldots\rangle on noncommuting elementary symmetric functions — and, in Section 8.6 of their 1995 paper, applied it to the characteristic polynomial of the generic matrix. For the generic n×nn\times n matrix A=(aij)A=(a_{ij}) (the entries are free generators over a field KK of characteristic zero) and a diagonal index ii, set

σ(t,αi)=∑k≥0Sk(αi)tk=∣I−tA∣ii−1,\sigma(t,\alpha_i)=\sum_{k\ge0}S_k(\alpha_i)t^k=|I-tA|_{ii}^{-1},

where the complete symmetric functions Sk(αi)S_k(\alpha_i) of the formal alphabet αi\alpha_i attached to the diagonal index ii are defined by this generating series. It is a noncommutative analogue of the ratio det⁡(I−tAi^)/det⁡(I−tA)\det(I-tA_{\hat i})/\det(I-tA), where Ai^A_{\hat i} is obtained from AA by deleting row and column ii. This series is rational over the free field: one has σ(t,αi)=Qi(t)−1Pi(t)\sigma(t,\alpha_i)=Q_i(t)^{-1}P_i(t) with Qi,PiQ_i,P_i of degrees nn and n−1n-1, normalized by Qi(0)=Pi(0)=1Q_i(0)=P_i(0)=1. Writing

Qi(t)=∑0≤j≤n(−1)jLj(i)(A) tj,Q_i(t)=\sum_{0\le j\le n}(-1)^jL_j^{(i)}(A)\,t^j,

the coefficients Lj(i)(A)L_j^{(i)}(A) — expressible by Hankel-type quasi-determinants in the Sk(αi)S_k(\alpha_i) and also by a noncommutative Krylov formula in the entries of the powers of AA — satisfy the noncommutative Cayley–Hamilton theorem

∑0≤j≤n(−1)jLj(A) An−j=0,\sum_{0\le j\le n}(-1)^jL_j(A)\,A^{n-j}=0,

where Lj(A)=diag⁡(Lj(1)(A),…,Lj(n)(A))L_j(A)=\operatorname{diag}(L_j^{(1)}(A),\ldots,L_j^{(n)}(A)). The leading coefficients det⁡i(A)=Ln(i)(A)\det_i(A)=L_n^{(i)}(A) are the nn pseudo-determinants of AA, exact noncommutative analogues of the determinant. Already for n=2n=2,

Q1(t)=1−(a11+a12a22a12−1)t+(a12a22a12−1a11−a12a21)t2,Q_1(t)=1-(a_{11}+a_{12}a_{22}a_{12}^{-1})t+(a_{12}a_{22}a_{12}^{-1}a_{11}-a_{12}a_{21})t^2,

so the coefficients are genuine rational expressions involving inverses of entries, and they depend on the index ii: the characteristic polynomial has diagonal-matrix rather than scalar coefficients.

Two specializations behave much better. If En=(eij)E_n=(e_{ij}) is the matrix of standard generators of the universal enveloping algebra U(gln)U(gl_n) of the general linear Lie algebra (the associative algebra generated by the matrix units eije_{ij} subject to the commutation relations of glngl_n), then all Qi(t)Q_i(t) coincide with det⁡(I−t(En+(n−1)I))\det(I-t(E_n+(n-1)I)); their coefficients lie in the center of U(gln)U(gl_n), the pseudo-determinants reduce to the classical Capelli determinant (a central element of U(gln)U(gl_n) constructed by Capelli), and one recovers the characteristic identities satisfied by the generators on highest-weight modules (the standard class of glngl_n-modules classified by a maximal weight). If Aq=(aij)A_q=(a_{ij}) is the matrix of generators of the quantum group GLq(n)GL_q(n) (the qq-deformed analogue of the algebra of polynomial functions on the general linear group), whose entries satisfy quadratic qq-commutation relations, then the pseudo-determinants are all equal, up to powers of qq, to the quantum determinant (the central determinant-like element of that algebra), every coefficient of every Qi(t)Q_i(t) is a polynomial in the aija_{ij}, and one recovers the quantum Cayley–Hamilton theorem; the lower coefficients still differ by powers of qq from one diagonal position to another. In view of these examples the authors pose the problem stated below.

Problem Statement

As posed at the end of Section 8.6 of the paper of Gelfand, Krob, Lascoux, Leclerc, Retakh and Thibon (1995), systematically characterize the following two classes of n×nn\times n matrices with noncommutative entries — that is, of specializations of the generic matrix, where the coefficients Lj(i)(A)L_j^{(i)}(A) of the pseudo-characteristic polynomials Qi(t)Q_i(t) are computed in the skew field generated by the entries via the rationality of σ(t,αi)=∣I−tA∣ii−1\sigma(t,\alpha_i)=|I-tA|_{ii}^{-1}:

  1. Matrices AA for which every coefficient Lj(i)(A)L_j^{(i)}(A), 0≤j≤n0\le j\le n and 1≤i≤n1\le i\le n, is a polynomial in the entries aija_{ij}, so that no inverses of entries survive in the pseudo-characteristic polynomial.

  2. Matrices AA for which the coefficients Lj(i)(A)L_j^{(i)}(A) do not depend on ii, so that the coefficients of the noncommutative characteristic polynomial are scalars rather than diagonal matrices.

Characterizing the two classes means determining necessary and sufficient conditions for membership in each class. Investigating the classes includes clarifying how the two classes relate to one another and to the known example families (enveloping algebras, quantum groups, and Manin-type matrices, that is, matrices whose entries satisfy Manin's quadratic cross-commutation relations), and what obstruction makes the generic matrix fail both properties.

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