How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Bruhat intervals and the -coefficients
Definition
Let and . The Bruhat interval is finite, with Bruhat order as in Basic properties of the Bruhat order on and The Bruhat order on by rank inequalities. The rank-order definition uses the zero-based model of , while uses the one-based model; throughout, identify them by the order-preserving shift on inputs and values.
The -coefficients are the unique coefficients in the standard-basis expansion where the bar is the involution from The Hecke bar involution is well defined and is the standard basis of The normalized type-A Hecke algebra and its bar involution. The sum has finite support because is finite. In rank one, , so .
The support, diagonal, and parity properties of these coefficients are stated and proved in The -coefficient recursion, support, degree bounds and inversion. This page uses the coefficient normalization given by the displayed bar expansion.
Depends on
Used by
Dependency tree · two levels
11 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- G. Lusztig, Hecke Algebras with Unequal Parameters (revised book version, arXiv:math/0208154v2) — the split case $L\equiv1$ read as the source for the bar operator, the R-coefficients, the new basis, its multiplication properties and cells; translated to the normalization of this page by $v_L=v^{-1}$ (so $v_L^{L(w)-L(y)}=v^{-(\ell(w)-\ell(y))}$) (standard reference, not scraped)
- Ben Elias and Geordie Williamson, The Hodge theory of Soergel bimodules, arXiv:1212.0791 (45 pp.) — §3.2 (printed pp. 15–16): the Hecke algebra in the normalization $H_xH_s=H_{xs}$ or $(v^{-1}-v)H_x+H_{xs}$, the bar involution $\overline{H_x}=H_{x^{-1}}^{-1}$, the Kazhdan–Lusztig basis $\{\underline H_x\}$ characterized by bar-invariance and $\underline H_x\in H_x+\sum_{y<x}v\mathbb Z[v]H_y$, the example $\underline H_s=H_s+vH_{\mathrm{id}}$, and Remark 3.2: $v=q^{-1/2}$, $H_x=v^{\ell(x)}T_x$, $\underline H_x=C'_x$, $h_{y,x}=v^{\ell(x)-\ell(y)}P_{y,x}(v^{-2})$ (standard reference, not scraped)
- Susumu Ariki, Robinson–Schensted correspondence and left cells, arXiv:math/9910117 (18 pp.) — the direct proof of the Kazhdan–Lusztig cell classification in type A via Knuth relations and transported Kazhdan–Lusztig graph edges (standard reference, not scraped)