Article ID Journal Published Year Pages File Type
4604024 Linear Algebra and its Applications 2006 13 Pages PDF
Abstract

Let K denote a field, and let V denote a vector space over K with finite positive dimension. We consider a pair of linear transformations A : V → V and A∗ : V → V that satisfy (i) and (ii) below:(i)There exists a basis for V with respect to which the matrix representing A is irreducible tridiagonal and the matrix representing A∗ is diagonal.(ii)There exists a basis for V with respect to which the matrix representing A∗ is irreducible tridiagonal and the matrix representing A is diagonal.We call such a pair a Leonard pair on V. Let diag(θ0, θ1, … , θd) denote the diagonal matrix referred to in (ii) above and let denote the diagonal matrix referred to in (i) above. It is known that there exists a basis u0, u1, … , ud for V and there exist scalars ϕ1, ϕ2, … , ϕd in K such that Aui = θiui + ui+1 (0 ⩽ i ⩽ d − 1), Aud = θdud, , . The sequence ϕ1, ϕ2, … , ϕd is called the first split sequence of the Leonard pair. It is known that there exists a basis v0, v1, … , vd for V and there exist scalars ϕ1, ϕ2, … , ϕd in K such that Avi = θd−ivi + vi+1 (0 ⩽ i ⩽ d − 1),Avd = θ0vd, , . The sequence ϕ1, ϕ2, … , ϕd is called the second split sequence of the Leonard pair. We display some attractive formulae for the first and second split sequence that involve the trace function.

Related Topics
Physical Sciences and Engineering Mathematics Algebra and Number Theory