Leonard pairs having specified end-entries

preprint2014arXivOpen access

Abstract

Fix an algebraically closed field F\mathbb{F} and an integer d≥3d \geq 3. Let VV be a vector space over F\mathbb{F} with dimension d+1d+1. A Leonard pair on VV is an ordered pair of diagonalizable linear transformations A:V→VA: V \to V and A∗:V→VA^* : V \to V, each acting in an irreducible tridiagonal fashion on an eigenbasis for the other one. Let {vi}i=0d\{v_i\}_{i=0}^d (resp.\ {vi∗}i=0d\{v^*_i\}_{i=0}^d) be such an eigenbasis for AA (resp.\ A∗A^*). For 0≤i≤d0 \leq i \leq d define a linear transformation Ei:V→VE_i : V \to V such that Eivi=viE_i v_i=v_i and Eivj=0E_i v_j =0 if j≠ij \neq i (0≤j≤d)(0 \leq j \leq d). Define Ei∗:V→VE^*_i : V \to V in a similar way. The sequence Φ=(A,{Ei}i=0d,A∗,{Ei∗}i=0d)Φ=(A, \{E_i\}_{i=0}^d, A^*, \{E^*_i\}_{i=0}^d) is called a Leonard system on VV with diameter dd. With respect to the basis {vi}i=0d\{v_i\}_{i=0}^d, let {þi}i=0d\{þ_i\}_{i=0}^d (resp.\ {ai∗}i=0d\{a^*_i\}_{i=0}^d) be the diagonal entries of the matrix representing AA (resp.\ A∗A^*). With respect to the basis {vi∗}i=0d\{v^*_i\}_{i=0}^d, let {θi∗}i=0d\{θ^*_i\}_{i=0}^d (resp.\ {ai}i=0d\{a_i\}_{i=0}^d) be the diagonal entries of the matrix representing A∗A^* (resp.\ AA). It is known that {θi}i=0d\{θ_i\}_{i=0}^d (resp. {þi∗}i=0d\{þ^*_i\}_{i=0}^d) are mutually distinct, and the expressions (θi−1−θi+2)/(θi−θi+1)(θ_{i-1}-θ_{i+2})/(θ_i-θ_{i+1}), (θi−1∗−θi+2∗)/(θi∗−θi+1∗)(θ^*_{i-1}-θ^*_{i+2})/(θ^*_i - θ^*_{i+1}) are equal and independent of ii for 1≤i≤d−21 \leq i \leq d-2. Write this common value as β+1β+ 1. In the present paper we consider the "end-entries" θ0θ_0, θdθ_d, θ0∗θ^*_0, θd∗θ^*_d, a0a_0, ada_d, a0∗a^*_0, ad∗a^*_d. We prove that a Leonard system with diameter dd is determined up to isomorphism by its end-entries and ββ if and only if either (i) β≠±2β\neq \pm 2 and qd−1≠−1q^{d-1} \neq -1, where β=q+q−1β=q+q^{-1}, or (ii) β=±2β= \pm 2 and Char(F)≠2\text{Char}(\mathbb{F}) \neq 2.

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