Leonard pairs having specified end-entries

Abstract

Fix an algebraically closed field F and an integer d ≥ 3. Let V be a vector space over F with dimension d+1. A Leonard pair on V is an ordered pair of diagonalizable linear transformations A: V V and A* : V V, each acting in an irreducible tridiagonal fashion on an eigenbasis for the other one. Let \vi\i=0d (resp.\ \v*i\i=0d) be such an eigenbasis for A (resp.\ A*). For 0 ≤ i ≤ d define a linear transformation Ei : V V such that Ei vi=vi and Ei vj =0 if j ≠ i (0 ≤ j ≤ d). Define E*i : V V in a similar way. The sequence =(A, \Ei\i=0d, A*, \E*i\i=0d) is called a Leonard system on V with diameter d. With respect to the basis \vi\i=0d, let \i\i=0d (resp.\ \a*i\i=0d) be the diagonal entries of the matrix representing A (resp.\ A*). With respect to the basis \v*i\i=0d, let \θ*i\i=0d (resp.\ \ai\i=0d) be the diagonal entries of the matrix representing A* (resp.\ A). It is known that \θi\i=0d (resp. \*i\i=0d) are mutually distinct, and the expressions (θi-1-θi+2)/(θi-θi+1), (θ*i-1-θ*i+2)/(θ*i - θ*i+1) are equal and independent of i for 1 ≤ i ≤ d-2. Write this common value as β + 1. In the present paper we consider the "end-entries" θ0, θd, θ*0, θ*d, a0, ad, a*0, a*d. We prove that a Leonard system with diameter d is determined up to isomorphism by its end-entries and β if and only if either (i) β ≠ 2 and qd-1 ≠ -1, where β=q+q-1, or (ii) β = 2 and Char(F) ≠ 2.

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