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Crystal lattices, crystal bases and their crystals
Definition
Let be the local ring of The local ring of rational functions regular at and let be an integrable weight module with its Kashiwara operators (The Kashiwara operators and of an integrable module, Quantum weight modules, weights in , and integrability).
A crystal lattice of is a free -submodule such that
(i) generates over , i.e. the canonical map is an isomorphism;
(ii) with , and each is again a free -module;
(iii) and for all .
Because is a principal ideal domain, each graded piece has a well-defined rank , and (ii) says that is the sum of the ranks of the .
A crystal basis of is a pair consisting of a crystal lattice and a -basis of the crystal limit (The local ring of rational functions regular at ) such that
(iv) , where ;
(v) and for all ;
(vi) for all and all : if and only if ; here denote the operators induced on .
The crystal graph of is the coloured directed graph with vertex set and an arrow whenever (by (vi) this is equivalent to ). The crystal of is this graph, together with the weight function for . For every one has .
A crystal basis of the negative half is defined by the same data with in place of : a free -submodule with and (The -string decomposition of the negative half), together with a -basis of satisfying (v) and (vi) for the operators on the negative half. Here the root grading replaces the weight grading, and the lattice and residue basis are required to respect that root grading. In the negative half, implies ; this refinement is specific to its infinite strings. No choice principle is used in these definitions.
Facts & Assumptions
Given: The local ring with residue field , an integrable chosen -graded type-1 module with Kashiwara operators, and a crystal lattice with as in (ii).
are -linear endomorphisms of shifting the label weight by and ; on a string they move to or , with the top of an -string and the bottom of an -string mapped to (The Kashiwara operators and of an integrable module).
with the toral action and gradings of Quantum weight modules, weights in , and integrability.
For a free -module the canonical map is an isomorphism, and is a -vector space of dimension equal to the rank of ; has dimension equal to the rank of over (The local ring of rational functions regular at ).
On the negative half, , and the operators shift the root degree by (The -string decomposition of the negative half, part (iii)).
Verification
Induced operators. By (iii) the operators preserve and commute with multiplication by , so they descend to -linear endomorphisms of , which is canonically by [F3]; by [F1] they shift the label weight by , so they map to and to , and axiom (v) says that they map into .
Rank decomposition. Since with every free by (ii), , and applying gives with each summand of dimension by [F3]. The isomorphism of (i) is weight graded, because and the target is the direct sum of the ; hence for every .
Residue counts. The crystal limit isomorphism of [F3] is compatible with the grading, and ; by (iv) each is contained in and is a -basis of , so is a -basis of . Hence , which is the displayed equality, and the weight function of the crystal is well defined by (iv).
The graph and the partial-inverse property. By (vi) the arrow relation is symmetric under exchanging and , so the crystal graph has no ambiguity: an arrow exists exactly when , equivalently . In a finite-dimensional piece a string may end at a bottom, where ; by (v) this is allowed and no vertex is added.
The negative half. For the same discussion applies with the root grading in place of the weight grading. By [F4] the induced endomorphisms of satisfy , so is injective and no element of is mapped to by ; with (v) this gives , the infinite-string refinement.
Choice. The definitions select no bases, no complements and no representatives; the lattice, its grading and the residue basis are given data, and all statements above are computations with them, so no choice principle is used.
Depends on
Used by
- A free A₀-lattice generating the module that is not a crystal lattice Counterexample
- Bar invariance and the congruence modulo q do not imply balancedness Counterexample
- Changing the equality case in the tensor rule breaks the partial-inverse axiom Counterexample
- The crystal graph, εᵢ, φᵢ and the weight function Definition
- The Kashiwara lattices L(λ) and L(∞) and their generating sets Definition
- The tensor product crystal B₁⊗ B₂ and its two-case convention Definition
- Kashiwara strings in the three-dimensional sl₂-module Example
- The crystal graph of the quantum symmetric square of the standard A₂-module Example
- The projection from B(∞) to a highest weight crystal for sl₂ Example
- Crystal lattice polarizations are perfect at q=0 Lemma
- Fixed-residue node cubes realize the actual Fock strings Lemma
- Projection from L(∞) to L(λ) and its compatibility with the Kashiwara operators Lemma
- Tensor products of integrable weight modules and of their crystal lattices Lemma
- The i-string components of a lattice vector and the single surviving component modulo q Lemma
- The vector representation has a perfect crystal of level one and a lower global basis Lemma
- The weight, εᵢ and φᵢ formulas for the tensor product crystal Lemma
- The dual crystal: reversed arrows, negated weights and swapped ε/φ Proposition
- The canonical crystal B(λ) is a highest weight crystal of highest weight λ Theorem
- The column monomial basis of the higher-level Fock module Theorem
- The crystal basis B(∞) of the negative half Theorem
- The crystal basis of a tensor product and the two-case operator rule Theorem
- The crystal of the level-one Fock space is the good-node partition graph Theorem
- The grand loop: existence of the highest weight crystal bases Theorem
- Uniqueness: crystal bases of integrable modules decompose into highest weight crystals Theorem
Dependency tree · two levels
26 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)