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.
The Lusztig divided-power integral form
Definition
Let be a symmetrizable Cartan datum for a quantum group with for all (Symmetrizable Cartan data for quantum groups), let be its Drinfeld–Jimbo algebra (The Drinfeld-Jimbo quantized enveloping algebra by generators and relations) with and , and set
the image of the Laurent polynomial ring of The Laurent polynomial ring as the principal localisation of Z[t] at t under the unital ring homomorphism sending to the indeterminate ; this homomorphism is injective and is a subring of (Verification, step 1.1). We work over this commutative domain inside the field .
For , and define the toral quantum binomial
the empty product being . Each factor is defined in because for (Quantum integers, factorials, Gaussian binomials and divided powers at ), so is a polynomial in with coefficients in ; in particular all commute with the and with one another (Verification, step 2.1).
The Lusztig divided-power integral form is the -subalgebra
where are the divided powers of Quantum integers, factorials, Gaussian binomials and divided powers at . Write for the -subalgebras generated by the and by the , and for the one generated by the and the .
Then:
(i) contains , and all ;
(ii) is a root-graded -subalgebra of the root-graded -algebra (Positive, negative and toral quantum subalgebras and their root gradings): with one has , each is an -submodule, and are graded in the same way;
(iii) canonically, i.e. the -span of is all of .
The shifted binomials with are included because the divided-power reordering identity of Divided-power multiplication, toral binomials and the reordering identity has coefficients with a nonconstant index; the specializations at of these elements are computed in The q=1 toral specialization identifies the classical Cartan generators, and the integral triangular decomposition and the specialization are treated only after this definition.
No freeness of or of its parts over , no independence of the listed generators, and no triangularity of the products of the three parts is asserted here. In particular is not a principal ideal domain (Verification, step 7.1), so no torsion-free-to-free inference over is permitted anywhere on this page.
Facts & Assumptions
Given: A symmetrizable Cartan datum with ; the algebra with its root grading and subalgebras ; the Laurent polynomial ring and the indeterminate over ; and the divided powers of Quantum integers, factorials, Gaussian binomials and divided powers at .
() has the universal property: for every ring with unit and every unit there is a unique unital ring homomorphism with ; every element of has a unique finite expansion with ; and the sum-of-coefficients map is a unital ring homomorphism (The Laurent polynomial ring as the principal localisation of Z[t] at t).
is an indeterminate over : is the fraction field of , and no nonzero polynomial over vanishes at ; with (Symmetrizable Cartan data for quantum groups).
is graded by with , , , and is a direct sum; is a quotient of the commutative group algebra , so is commutative and , ; and is a -subspace for every (The Drinfeld-Jimbo quantized enveloping algebra by generators and relations, Positive, negative and toral quantum subalgebras and their root gradings).
for every , and , and (Quantum integers, factorials, Gaussian binomials and divided powers at ).
The subalgebras are generated by the , the , and the respectively, and these elements together generate as a -algebra; the rank-one subalgebra generated by is described by Divided-power commutation and the simple string modules (used only as the published divided-power convention reference) (Positive, negative and toral quantum subalgebras and their root gradings, The Drinfeld-Jimbo quantized enveloping algebra by generators and relations).
A subring of a field is a domain; if is an -submodule of a -vector space and , then identifies with its image modulo the evident relation, and the canonical map , , is injective: writing with and , the relation follows from the vanishing of by multiplying by (The Laurent polynomial ring as the principal localisation of Z[t] at t for the coefficient calculus).
Verification
The assignment defines a unital ring homomorphism by the universal property of [F1], since is a unit of the field . It is injective: if with finitely many , choose so that every ; then the polynomial vanishes at the indeterminate , so by [F2] it is the zero polynomial and all . Hence its image is a subring of , and in particular is a commutative domain.
Each factor is a -linear combination of the toral elements and , and the denominator is nonzero for : would make the indeterminate a root of the nonzero polynomial by [F2]. Hence every factor, and therefore , is a well-defined element of ; expanding the product and using and of [F3], each is a finite -linear combination of the toral elements (), that is, a polynomial in . Since is commutative by [F3], all commute with every and with one another.
The listed generators are homogeneous for the root grading of [F3]: has degree because and the grading is multiplicative with by [F4]; likewise has degree ; and and, by step 2.1, have degree .
By definition consists of the finite -linear combinations of finite products of the listed generators, the empty product included. Every finite product of homogeneous elements is homogeneous of the sum of their degrees (the grading of [F3] is multiplicative), so every element of is a finite sum of homogeneous elements of . Since is a direct sum, this decomposition is unique, so with ; the same argument applies to the generated -subalgebras (generators of degrees ) and (degree- generators), which are therefore graded in the same way. Each , being the intersection of the -submodule with a -subspace, is an -submodule.
Since , by [F4] and the are among the listed generators, contains , and ; consequently its -span contains all generators of , so by [F5] the -span of is all of .
The canonical multiplication map , is surjective by step 5.1. It is injective by the argument of [F6]: given with , , , one has , and forces in the -vector space because ; hence . Thus is an isomorphism, which is claim (iii).
Finally, is not a principal ideal domain: the ideal is proper, since a relation would give under the ring homomorphism with of [F1], in which contributes an even integer. If were principal, then from and the domain one gets , and reducing modulo the ring homomorphism , (again [F1]) gives ; if then reduces to , a contradiction, so and hence , that is, for some . Then and therefore because is a domain with , so is a unit and , contradicting the properness of . Hence no principal ideal equals . This is why no freeness, independence or triangularity statement is attached to in this definition; those are separate theorems with their own hypotheses.
Depends on
- The Drinfeld-Jimbo quantized enveloping algebra by generators and relations
- Positive, negative and toral quantum subalgebras and their root gradings
- Quantum integers, factorials, Gaussian binomials and divided powers at $q_i$
- Symmetrizable Cartan data for quantum groups
- The Laurent polynomial ring as the principal localisation of Z[t] at t
- Divided-power commutation and the simple $U_{q_i}(\mathfrak{sl}_2)$ string modules
Used by
- Direct q=1 substitution in quantum denominators Counterexample
- The bar lattice and the divided-power integral lattice of a based module Definition
- The Drinfeld pairing between the positive and negative quantum halves Definition
- The Fock-space convention dictionary for finite type-A quantum modules Definition
- The integral residue lattices L_A(∞) and L_A(λ) Definition
- Divided powers and the Lusztig form in quantized sl2 Example
- Specializing a quantum highest weight lattice at q=1 Example
- Cartan projection constructs the Verma contravariant form and identifies its radical Lemma
- Distinct cyclotomic shears give integrable based quantum sl-two chains Lemma
- Divided-power integrality of the quasi-R action on based lattices Lemma
- Divided-power multiplication, toral binomials and the Eᵢ⁽ᵃ⁾Fᵢ⁽ᵇ⁾ reordering identity Lemma
- Integral skew-string coefficients on the divided-power negative half Lemma
- Integrality of the string decomposition and the divided-power string ideals Lemma
- Local q=1 deformation proves integrable highest weight universality Lemma
- Rational-local quantum halves and torus specialize at q=1 Lemma
- Reversal preserves the negative-half integral and crystal lattices Lemma
- The bar involution and the contravariant anti-involution preserve U_A Lemma
- The Drinfeld pairing is nondegenerate in each root degree and matches the shuffle pairing Lemma
- The q=1 toral specialization identifies the classical Cartan generators Lemma
- The unmodified integral torus has a quantum-binomial basis Lemma
- Two cyclotomic shears give a periodic integrable based quantum sl-two chain Lemma
- Specialization at q=1 recovers the classical enveloping relations Proposition
- Integral triangular decomposition and freeness of the Lusztig form Theorem
- The cyclotomic projective K₀ is the integral highest-weight module Theorem
- The highest weight and negative half integral crystal triples are balanced Theorem
- The i-string decomposition of the negative half Theorem
- The KLR Cartan pairing is the Lusztig-normalized half form Theorem
- The KLR category categorifies the negative quantum half Theorem
- The KLR Grothendieck ring satisfies the divided-power quantum Serre relations Theorem
- The negative-half bilinear form is symmetric, nondegenerate and integral Theorem
Dependency tree · two levels
30 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)
- Math 263C Quantum Groups (Stanford, 2022), lecture slides 'Lusztig's quantum group. Tilting modules.' (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)