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Bar invariance, congruence and uniqueness of the lower global basis
Statement
For the divided-power integral form of The Lusztig divided-power integral form and for every dominant , let be or , let be or with bar lattice , and let be or . Then there is a unique lower global family with the property that the residue class of in is for every , namely the family of The lower global basis of and of a highest weight module. It is bar invariant, a genuine basis of , and a basis of both rational chart lattices and over and ; its -span is the simultaneous balanced intersection and its field span is the whole module. It is adapted to every divided string-image ideal in the exact sense of the integral balanced theorem, and the same family is obtained with residue over either chart. No word family is assumed to be a basis, no unitriangular characterization is used, and no lower lattice self-duality is asserted.
Facts & Assumptions
Given: The balanced triple over of Balanced triples over the two charts of and the globalization map, the string-image ideals of Integrality of the string decomposition and the divided-power string ideals, the lower global definition of The lower global basis of and of a highest weight module, and the bar involution with its stability of and the divided-power form (The bar involution and the contravariant anti-involution preserve ).
Integral balanced theorem (The highest weight and negative half integral crystal triples are balanced): the triples and are integrally balanced componentwise; the balanced -intersection maps isomorphically onto , after rational extension onto the full rational crystal space; there are bar-invariant global lifts forming an -basis of , spanning over and over , adapted to every string-image ideal and with the displayed free decompositions.
Balancedness and its kernel (Balanced triples over the two charts of and the globalization map): the canonical map is an isomorphism exactly when the triple is balanced, so in the balanced case an element of lies in only if it is .
Bar transport (The bar involution and the contravariant anti-involution preserve , The bar lattice and the divided-power integral lattice of a based module): preserves , commutes with the projection , and exchanges and , so the balanced intersection is stable under and transports the zero-chart residue map to the infinity-chart residue map; the bar-fixed global lifts and their corresponding residue labels are supplied by [F1], not by an action of on the zero-chart quotient.
Proof
Existence. Apply [F1] degree by degree, and note that the residue target is the free -span of in each finite root or label component. The lift of residue exists in , is bar invariant by [F1], and the direct sums over degrees give a family with the asserted spanning properties over , and ; adaptedness to the string ideals is the corresponding clause of [F1].
Uniqueness. Let have the same residue class in . Then lies in the kernel of the canonical map of [F2], which is injective in the balanced case; hence . Applied to and an arbitrary lift of , this is exactly the uniqueness used by later consumers, and it identifies the family defined over either chart.
Conclusion. Steps 1.1 and 2.1 give existence, the residue normalization, bar invariance, the two chart-basis assertions, the balanced-intersection and field-span descriptions and uniqueness; no word family, unitriangular condition or lower self-duality enters, since the construction is the inverse of the integral globalization map of [F2].
Depends on
- Balanced triples over the two charts of $\mathbb P^1$ and the globalization map
- The lower global basis of $U_q^-$ and of a highest weight module
- The bar lattice and the divided-power integral lattice of a based module
- Integrality of the string decomposition and the divided-power string ideals
- The bar involution and the contravariant anti-involution preserve $U_A$
- The highest weight and negative half integral crystal triples are balanced
Used by
- Bar invariance and the congruence modulo q do not imply balancedness Counterexample
- The dual-canonical, canonical and quasi-canonical Fock bases Definition
- The upper (form-dual) global basis and the required perfectness of the integral pairing Definition
- Lower and upper global bases in a small highest weight module Example
- Matching the canonical and lower global normalizations in rank one and A₂ Example
- The balanced triple and global basis for the two-dimensional U_q(sl₂)-module Example
- Canonical elementary crystal extraction and highest-weight survivors Lemma
- Divided-power integrality of the quasi-R action on based lattices Lemma
- Self-dual KLR projectives have positive first-block divided-string leading terms Lemma
- Specialization of the global bases and the root-of-unity boundary Proposition
- Finitely generated free integral weight lattices and deformation of the classical weight character Theorem
- Integral triangular decomposition and freeness of the Lusztig form Theorem
- Lusztig's canonical basis and Kashiwara's lower global basis agree in symmetric finite ADE type Theorem
- Self-dual indecomposable KLR projectives give the lower global basis (symmetric type) Theorem
- Standard tableau monomials form a basis of the highest weight Fock submodule Theorem
- The based quotient: projection of the lower global basis to a highest weight module Theorem
- The basic representation global basis is unitriangular in the partition basis Theorem
- The highest weight Fock submodule carries the quantum-group global bases Theorem
- Upper and lower global bases are dual and crystal compatible Theorem
Dependency tree · two levels
31 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
- Masaki Kashiwara, On crystal bases of the q-analogue of universal enveloping algebras, Duke Mathematical Journal 63 (1991), 465–516 (standard reference, not scraped)
- Kyeonghoon Jeong, Seok-Jin Kang and Masaki Kashiwara, Crystal Bases for Quantum Generalized Kac-Moody Algebras, arXiv:math/0305390 (standard reference, not scraped)
- George Lusztig, Introduction to Quantum Groups (Progress in Mathematics 110, Birkhauser, 1993; second printing 1994; author-hosted scan) (standard reference, not scraped)