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Some trace formulae involving the split sequences of a Leonard pair
Authors:Kazumasa Nomura  Paul Terwilliger
Institution:a College of Liberal Arts and Sciences, Tokyo Medical and Dental University, Kohnodai, Ichikawa 272-0827, Japan
b Department of Mathematics, University of Wisconsin, 480 Lincoln Drive, Madison, WI 53706, USA
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(θ0θ1, … , θd) denote the diagonal matrix referred to in (ii) above and let View the MathML source denote the diagonal matrix referred to in (i) above. It is known that there exists a basis u0u1, … , ud for V and there exist scalars ?1?2, … , ?d in K such that Aui = θiui + ui+1 (0 ? i ? d − 1), Aud = θdud, View the MathML source, View the MathML source. The sequence ?1?2, … , ?d is called the first split sequence of the Leonard pair. It is known that there exists a basis v0v1, … , vd for V and there exist scalars ?1?2, … , ?d in K such that Avi = θdivi + vi+1 (0 ? i ? d − 1),Avd = θ0vd, View the MathML source, View the MathML source. The sequence ?1?2, … , ?d 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.
Keywords:05E30  05E35  33C45  33D45
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