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The -string decomposition of the negative half
Statement
Let be the negative half of the Drinfeld–Jimbo algebra with its skew derivations (Kashiwara's skew derivations and on the negative half, Positive, negative and toral quantum subalgebras and their root gradings), fix , and write for the divided powers (Quantum integers, factorials, Gaussian binomials and divided powers at ). Then:
(i) is locally nilpotent on , and the endomorphism is well defined (each sum is finite on each element) and is the projection onto along . In particular , , , for , and
(ii) Every has a unique -string decomposition and the components are given by .
(iii) The Kashiwara operators on the negative half, defined on the string decomposition by are -linear endomorphisms of with ; if and only if ; is injective and . Both operators preserve the root grading and shift its degree by , that is and .
No choice principle is used. Here denotes the ordinary -fold power of the derivation, not its divided power. The same projector and every string coefficient preserve the divided-power lattice (The Lusztig divided-power integral form ), as proved by the integral skew-string supplier; this does not assert that lattice's freeness.
Facts & Assumptions
Given: The negative half , the skew derivations , a fixed , and the divided powers .
is graded by the positive root lattice, with and ; the grading is the restriction of the root grading of (Positive, negative and toral quantum subalgebras and their root gradings).
The maps are -linear, vanish on , satisfy , the Leibniz rule on homogeneous of actual weight , and similarly for with the opposite twist; they satisfy and decrease positive height by one, so (zero when ) and is locally nilpotent (Kashiwara's skew derivations and on the negative half).
for , , and with ; all displayed scalars are nonzero (Quantum integers, factorials, Gaussian binomials and divided powers at ).
Gaussian identity: for , equals for and for ; the Gaussian quotient is invariant under and the identity is the inversion of the Gauss product formula (The quantum Pascal recurrences, the Gauss product formula and Gaussian integrality, parts (iii)-(iv)).
Integral skew-string supplier: the operator of (i) is finite on each vector and projects onto along ; every has a unique finite expansion with and ; the projector and coefficients preserve , with no global basis or freeness assumed (Integral skew-string coefficients on the divided-power negative half).
Proof
The -boson relation. By [F2] with and , ; applying the Leibniz rule to and summing the geometric series gives , and dividing by yields for .
Iterated deletion. If , then induction on using step 1.1 gives for , while for .
Termination. By [F2] the derivation lowers positive height by one, so for homogeneous one has whenever ; hence on each only finitely many terms of the sum defining are nonzero, and is a well-defined -linear endomorphism of .
The projection. For and , steps 2.1 and [F3] give , which by the Gaussian identity [F4] equals for and for . Hence , fixes , and kills ; moreover by the cancellation of consecutive terms in using step 1.1, so and is the projection onto along , with because lies in the two subspaces.
Existence of the string decomposition. The algebra is spanned over by finite words in the , and each such word belongs to because . Thus write with and . Apply [F5] to each and use the -linearity of and to obtain , where . This sum is finite by step 2.2. The field-valued decomposition therefore follows from the integral one without assuming an integral basis or freeness.
Uniqueness and the coefficient formula. Suppose with and for large. Applying and then for fixed : by step 2.1, for and for , and by step 3.1, for while ; hence , that is . Thus the components of step 4.1 are determined by , giving uniqueness and the displayed coefficient formula.
The Kashiwara operators. Given the unique decomposition of steps 4.1-5.1, the prescriptions and are well-defined -linear maps by uniqueness; shifting the index shows , so .
Kernel, injectivity and value at . For one has exactly when for every , that is ; hence . If , then is a decomposition with all top coefficients in , so uniqueness in step 5.1 forces for all , that is ; hence is injective. Finally has decomposition , so .
Root grading. Let be homogeneous. Since raises the degree by , the components of steps 4.1-5.1 may be taken homogeneous of degree (decompose and each into finitely many homogeneous pieces and compare degrees), so has degree and has degree ; hence and .
Integrality and choice. By [F5] the projector and every coefficient preserve the divided-power lattice , and the shifts of step 6.1 preserve it as well; no freeness of is asserted. All constructions used unique decompositions, finite sums and the explicit operator ; no choice principle is used.
Depends on
- Kashiwara's skew derivations $e_i'$ and $e_i''$ on the negative half
- Positive, negative and toral quantum subalgebras and their root gradings
- Quantum integers, factorials, Gaussian binomials and divided powers at $q_i$
- The Lusztig divided-power integral form $U_A$
- The quantum Pascal recurrences, the Gauss product formula and Gaussian integrality
- Integral skew-string coefficients on the divided-power negative half
Used by
- Crystal lattices, crystal bases and their crystals Definition
- The crystal graph, εᵢ, φᵢ and the weight function Definition
- The Kashiwara lattices L(λ) and L(∞) and their generating sets Definition
- The Kashiwara operators ẽᵢ and f̃ᵢ of an integrable module Definition
- Matching the canonical and lower global normalizations in rank one and A₂ Example
- The projection from B(∞) to a highest weight crystal for sl₂ Example
- Canonical elementary crystal extraction and highest-weight survivors Lemma
- Integrality of the string decomposition and the divided-power string ideals Lemma
- Projection from L(∞) to L(λ) and its compatibility with the Kashiwara operators Lemma
- The crystal basis B(∞) of the negative half Theorem
- The grand loop: existence of the highest weight crystal bases Theorem
Dependency tree · two levels
16 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 Math. J. 63 (1991), no. 2, 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)
- 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)