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The structure of a tridiagonal 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 K-linear transformations A:VV and A:VV that satisfy the following conditions: (i) each of A,A is diagonalizable; (ii) there exists an ordering View the MathML source of the eigenspaces of A such that AViVi-1+Vi+Vi+1 for 0?i?d, where V-1=0 and Vd+1=0; (iii) there exists an ordering View the MathML source of the eigenspaces of A such that View the MathML source for 0?i?δ, where View the MathML source and View the MathML source; (iv) there is no subspace W of V such that AWW,AWW,W≠0,WV.We call such a pair a tridiagonal pair on V. It is known that d=δ and for 0?i?d the dimensions of View the MathML source coincide.In this paper we show that the following (i)-(iv) hold provided that K is algebraically closed: (i) Each of View the MathML source has dimension 1.(ii) There exists a nondegenerate symmetric bilinear form 〈,〉 on V such that 〈Au,v〉=〈u,Av〉 and 〈Au,v〉=〈u,Av〉 for all u,vV.(iii) There exists a unique anti-automorphism of End(V) that fixes each of A,A.(iv) The pair A,A is determined up to isomorphism by the data View the MathML source, where θi (resp.View the MathML source) is the eigenvalue of A (resp.A) on Vi (resp.View the MathML source), andView the MathML source is the split sequence of A,A corresponding to View the MathML source and View the MathML source.
Keywords:05E35  05E30  33C45  33D45
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