Down᎐up algebras which originated in the study of differential posets were recently defined and studied by Benkart and Roby. Benkart posed an open problem in her paper: to determine the centers of all down᎐up algebras. Here in this paper we completely solve this problem. As an application we also ge
Down–Up Algebras
✍ Scribed by Georgia Benkart; Tom Roby
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 403 KB
- Volume
- 209
- Category
- Article
- ISSN
- 0021-8693
No coin nor oath required. For personal study only.
✦ Synopsis
The algebra generated by the down and up operators on a differential or Ž . uniform partially ordered set poset encodes essential enumerative and structural properties of the poset. Motivated by the algebras generated by the down and up operators on posets, we introduce here a family of infinite-dimensional associative algebras called down᎐up algebras. We show that down᎐up algebras exhibit many Ž . of the important features of the universal enveloping algebra U ᒐ l of the Lie 2 algebra ᒐ ᒉ including a Poincare᎐BirkhoffᎏWitt type basis and a well-behaved 2 representation theory. We investigate the structure and representations of down᎐up algebras and focus especially on Verma modules, highest weight representations, and category O O modules for them. We calculate the exact expressions for all the weights, since that information has proven to be particularly useful in determining structural results about posets.
📜 SIMILAR VOLUMES
A class of algebras called down-up algebras was introduced by G. Benkart and T. Roby (1998, J. Algebra 209, 305-344). We classify the finite dimensional simple modules over Noetherian down-up algebras and show that in some cases every finite dimensional module is semisimple. We also study the questi
lie in a certain class of iterated skew polynomial rings, called ambiskew polynomial rings, in two indeterminates x and y over a commutative ring B. In such rings, commutation of the indeterminates with elements of B involve the same endomorphism σ of B, but from different sides, that is, yb = σ b y
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