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Divided-power multiplication, toral binomials and the reordering identity
Statement
Let and let be the toral quantum binomials of The Lusztig divided-power integral form (, , , ), inside the Drinfeld–Jimbo algebra of The Drinfeld-Jimbo quantized enveloping algebra by generators and relations with and its parts as in that definition. Write , , , for the divided powers of Quantum integers, factorials, Gaussian binomials and divided powers at and put inside the displayed formulas.
(i) Divided-power multiplication. For all ,
(ii) Toral recursion and commutation. For , Each is a Laurent polynomial in with coefficients in ; the toral elements commute with one another and with all . For all and all one has if , while , , , for all . In particular , , and : the toral factor can be moved to the middle at the cost of a shift of the binomial index.
(iii) Reordering identity. For all , with every coefficient a toral quantum binomial in . In particular and . For , and commute; the same-half divided powers (and likewise ) commute whenever , and for no commutation is asserted.
(iv) Triangular spanning. Every element of is an -linear combination of products with , and ; equivalently as an -module. No independence of the spanning family is asserted.
Facts & Assumptions
Given: The Cartan datum, the algebra , the toral binomials , and the divided powers .
, because and for all (Quantum integers, factorials, Gaussian binomials and divided powers at ).
The defining relations: ; for ; when ; and the general same-half relations are the quantum Serre relations (The Drinfeld-Jimbo quantized enveloping algebra by generators and relations).
Toral conjugation and shifts: and , so for every Laurent polynomial one has and (Positive, negative and toral quantum subalgebras and their root gradings).
The published rank-one formula: for , , equivalently , and for one has (Divided-power commutation and the simple string modules (ii) and The Lusztig divided-power integral form for the identification of the coefficient with ).
For use in this proof, extend the quantum integer to every by , agreeing with Quantum integers, factorials, Gaussian binomials and divided powers at for and giving . Direct expansion of the numerators gives ; replacing by gives the other version. Thus for all integers , without extending factorials or Gaussian binomials to negative indices.
is the -algebra generated by the ; its elements are finite -linear combinations of finite products of these generators, and , , (The Lusztig divided-power integral form ).
Verification
Part (i): by [F1], and likewise for .
Auxiliary product identity. Fix integers and , put and let , so that with ; we prove . Factoring and putting , so that and , the relevant factors become , , and , where . Multiplying the target identity by , using and , and factoring out the common factor , the two sides become and ; comparing the coefficients of and gives the identities and , both instances of [F5] with .
Part (ii): unrolling the product definition, equals the factor times ; since both are Laurent polynomials in (The Lusztig divided-power integral form , Verification) they commute and the recursion follows. The commutativity statements are those of that step. For the shifts, [F3] gives and ; applying this to the -fold product , the first factor of is multiplied by (first term) and (second term), which is the same as replacing by ; hence (for , ), and likewise . Rewriting gives and .
Reordering by induction on for fixed . At the identity is . Multiply the formula for on the left by . For a target index put . The no-contraction term from index contributes to the coefficient of , after shifting through the toral factor. The contraction term from index contributes by [F4]. Their sum is by step 1.2, so division by the nonzero gives the target coefficient. When the absent no-contraction term is represented by ; the term is just . A contraction from is absent because , so no target exceeds . These account for every term and prove the induction, including the stated special cases.
The remaining clauses of (iii): for the relation of [F2] gives after dividing by the nonzero factorials [F1]; if then and by [F2], hence and for all . No commutation is asserted when , where the quantum Serre relation is the only comparison used later.
Part (iv): every element of is a finite -linear combination of finite products of generators by [F6]. Move every and every to the middle: commutes with the toral generators and crosses at the cost of the scalar by [F3]; crosses at the cost of an index shift by step 2.1. These operations do not change the relative order of the positive and negative generators, so after finitely many of them we obtain a finite sum of terms with and products of divided powers of a single sign, except that a product may still contain an -factor to the left of an -factor. Define the measure of such a product as the pair (total height = sum of the exponents of all its divided powers, number of ordered pairs (positive factor, negative factor) in which the positive factor precedes the negative one), ordered lexicographically. An adjacent sign inversion, after moving toral factors aside, has the form with . If , step 3.2 swaps the factors, keeping and decreasing . If , step 3.1 rewrites it as : the terms with strictly decrease , while the term keeps but strictly decreases (that inversion disappears and no other inversion is created, as toral factors are ignored by ). By induction on the rewriting terminates, producing the asserted span by triangular products in .
Depends on
- The Drinfeld-Jimbo quantized enveloping algebra by generators and relations
- The Lusztig divided-power integral form $U_A$
- Positive, negative and toral quantum subalgebras and their root gradings
- Quantum integers, factorials, Gaussian binomials and divided powers at $q_i$
- The quantum Pascal recurrences, the Gauss product formula and Gaussian integrality
- Divided-power commutation and the simple $U_{q_i}(\mathfrak{sl}_2)$ string modules
Used by
- The integral residue lattices L_A(∞) and L_A(λ) Definition
- Divided powers and the Lusztig form in quantized sl2 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
- Integral quantum highest modules are the normalized q-Schur Weyl cells Lemma
- Local q=1 deformation proves integrable highest weight universality Lemma
- Periodic cyclotomic shear tensor corrections escape every finite cut Lemma
- Polynomial quantum highest vectors satisfy every divided-power highest relation Lemma
- Polynomial quantum Schur first levels: Weyl filtration and the actual Hecke corner Lemma
- Rational-local quantum halves and torus specialize at q=1 Lemma
- The dominant quantum Serre quotient is nonzero and integrable 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
- Integral triangular decomposition and freeness of the Lusztig form Theorem
Dependency tree · two levels
18 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
- Math 263C Quantum Groups (Stanford, 2022), lecture slides 'Lusztig's quantum group. Tilting modules. The Fusion Category in Action' (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)
- Kyeonghoon Jeong, Seok-Jin Kang and Masaki Kashiwara, Crystal Bases for Quantum Generalized Kac-Moody Algebras, arXiv:math/0305390 (standard reference, not scraped)