English

A factorization theorem for affine Kazhdan-Lusztig basis elements

Representation Theory 2009-08-05 v1

Abstract

The lowest two-sided cell of the extended affine Weyl group WeW_e is the set {wWe:w=xw0z,for somex,zWe}\{w \in W_e: w = x \cdot w_0 \cdot z, \text{for some} x,z \in W_e\}, denoted W(ν)W_{(\nu)}. We prove that for any wW(ν)w \in W_{(\nu)}, the canonical basis element \Cw\C_w can be expressed as 1[n]!χλ(\y)\Cv1w0\Cw0v2\frac{1}{[n]!} \chi_\lambda({\y}) \C_{v_1 w_0} \C_{w_0 v_2}, where χλ(\y)\chi_\lambda({\y}) is the character of the irreducible representation of highest weight λ\lambda in the Bernstein generators, and v1v_1 and v21v_2^{-1} are what we call primitive elements. Primitive elements are naturally in bijection with elements of the finite Weyl group WfWeW_f \subseteq W_e, thus this theorem gives an expression for any \Cw\C_w, wW(ν)w \in W_{(\nu)} in terms of only finitely many canonical basis elements. After completing this paper, we realized that this result was first proved by Xi in \cite{X}. The proof given here is significantly different and somewhat longer than Xi's, however our proof has the advantage of being mostly self-contained, while Xi's makes use of results of Lusztig from \cite{L Jantzen} and Cells in affine Weyl groups I-IV and the positivity of Kazhdan-Lusztig coefficients.

Keywords

Cite

@article{arxiv.0908.0340,
  title  = {A factorization theorem for affine Kazhdan-Lusztig basis elements},
  author = {Jonah Blasiak},
  journal= {arXiv preprint arXiv:0908.0340},
  year   = {2009}
}

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20 pages

R2 v1 2026-06-21T13:32:03.043Z