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The bar involution and the contravariant anti-involution preserve
Statement
Let (the bar involution) and (the contravariant anti-involution) be the semilinear maps of The Chevalley involution, bar involution, and contravariant anti-involution preserve the Drinfeld–Jimbo ideal, so that , , , and , , , , with anti-multiplicative. Let and let be the Lusztig divided-power integral form with its generators , , and toral binomials (The Lusztig divided-power integral form ). Then and . Explicitly, on the generators,
In particular both maps restrict to bijections of : to a semilinear algebra involution of and to a semilinear anti-involution of , while keeps all coefficients in . These are the two involutions under which the bar lattice and the contravariant duality of the later constructions are taken; neither formula is the Chevalley involution , which changes signs, exchanges the two halves and is treated in The Chevalley involution, bar involution, and contravariant anti-involution preserve the Drinfeld–Jimbo ideal. No choice is used.
Facts & Assumptions
Given: The Drinfeld–Jimbo algebra (The Drinfeld-Jimbo quantized enveloping algebra by generators and relations), the involution lemma defining and their semilinearity (The Chevalley involution, bar involution, and contravariant anti-involution preserve the Drinfeld–Jimbo ideal), and the -algebra with its listed generators (The Lusztig divided-power integral form ).
is an involutive semilinear algebra automorphism and an involutive semilinear anti-automorphism of with the stated values on generators; both apply the field involution (The Chevalley involution, bar involution, and contravariant anti-involution preserve the Drinfeld–Jimbo ideal).
The field involution preserves , since ; and fixes and for every , because is invariant under (Quantum integers, factorials, Gaussian binomials and divided powers at ).
is the -subalgebra generated by the , , and ; its elements are finite -linear combinations of finite products of these generators (The Lusztig divided-power integral form ).
with the empty product (The Lusztig divided-power integral form ).
Proof
Proof technique: compute both (anti-)maps on each family of generators of and conclude by semilinearity and [F3].
For every one has and , since fixes and fixes the scalar by [F2]; on the torus . For the toral binomial, applying factor by factor and using , gives and ; the two signs cancel, so each factor and hence the product of [F4] is fixed: .
For , which is anti-multiplicative, by [F2], and symmetrically ; ; and on each factor of [F4], while , so fixes every factor; since the factors commute, as well.
Consequently each of sends every generator of into by steps 1.1 and 2.1, and sends scalars into by [F2]. From [F3], an element of is a finite sum with and generators ; applying the semilinear algebra map gives , and applying the semilinear anti-algebra map gives . Hence and ; since are involutions on by [F1], the reverse inclusions hold as well, so and and the restrictions are bijections of the stated (anti-)multiplicative types. No choice is used.
Depends on
- The Drinfeld-Jimbo quantized enveloping algebra by generators and relations
- The Lusztig divided-power integral form $U_A$
- Quantum integers, factorials, Gaussian binomials and divided powers at $q_i$
- The Chevalley involution, bar involution, and contravariant anti-involution preserve the Drinfeld–Jimbo ideal
Used by
- The bar lattice and the divided-power integral lattice of a based module Definition
- The lower global basis of U_q^- and of a highest weight module Definition
- Cartan projection constructs the Verma contravariant form and identifies its radical Lemma
- The Lusztig–Kashiwara form, parameter and coproduct dictionary Lemma
- Bar invariance, congruence and uniqueness of the lower global basis Theorem
- The KLR Cartan pairing is the Lusztig-normalized half form Theorem
- The KLR category categorifies the negative quantum half Theorem
- Upper and lower global bases are dual and crystal compatible Theorem
Dependency tree · two levels
15 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
- George Lusztig, Introduction to Quantum Groups (Progress in Mathematics 110, Birkhauser, 1993; second printing 1994; author-hosted scan) (standard reference, not scraped)
- Richard Borcherds, Mark Haiman, Theo Johnson-Freyd, Nicolai Reshetikhin and Vera Serganova, Berkeley Lectures on Lie Groups and Quantum Groups (book-length lecture notes, last updated 18 January 2024) (standard reference, not scraped)