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The weight, and formulas for the tensor product crystal
Statement
Let be crystal bases of integrable modules as in The crystal basis of a tensor product and the two-case operator rule and let be the tensor product crystal of The tensor product crystal and its two-case convention with the two-case operators of that theorem. Then for all , and :
(a) ;
(b) ;
(c) ;
(d) the two cases are exactly the alternatives in the max formulas: acts on the first factor if and only if , and then (this equality also holds at the tie); it acts on the second factor if and only if , and then , and dually acts on the first factor if and only if ;
(e) partial-inverse property. For all and every , if and only if ; in particular the assignment of the non-strict comparison to and the strict comparison to is the one for which the two-case rule is internally consistent;
(f) along the -string, and for .
No choice principle is used.
Facts & Assumptions
Given: Crystal bases of integrable modules, the tensor product crystal of The tensor product crystal and its two-case convention with the operators of The crystal basis of a tensor product and the two-case operator rule, vertices , and ; write , , , .
The tensor product crystal (The tensor product crystal and its two-case convention): , and act on the factor selected by the strict/non-strict comparison of of the first factor with of the second, with value when the selected factor maps to .
The tensor rule theorem (The crystal basis of a tensor product and the two-case operator rule): the displayed two-case operators make a crystal basis of , they map into , and they satisfy the partial-inverse axiom for all .
Crystal graph invariants (The crystal graph, , and the weight function): for every in the crystal of an integrable module, and are finite and nonnegative, , the -string of has vertices, and along each existing edge one has and (dually for ).
Crystal lattice and basis axioms (Crystal lattices, crystal bases and their crystals) and the Kashiwara operators (The Kashiwara operators and of an integrable module) supplying the underlying finite strings and partial inverses of the two factors.
Proof
The two integer pairs and determine the strings and the pairings: and by [F3], the -string of has vertices and that of has vertices by [F3], and any -string contains a unique top (a vertex with ) and a unique bottom (a vertex with ).
One application of to . If , the non-strict comparison selects the first factor and (or if ), so the pair becomes in the first factor and is unchanged; if , the strict inequality selects the second factor, the pair becomes and is unchanged. Every application is a genuine existing edge of the corresponding factor precisely in the displayed case, by [F1] and the definition of in [F3].
Computation of . Case : by step 1.2 every -step acts on the first factor of the current pair, and the first factor offers exactly applicable steps before the next raising maps its top to ; each such step keeps the comparison true because only increases, so exactly steps are possible and . Case : the first steps act on the second factor, decreasing to (each needs , and throughout), after which the comparison is and the remaining steps act on the first factor; exactly steps are possible and because and by step 1.1. Hence in both cases , which is (b).
Computation of . If , every -step while the comparison stays strict acts on the first factor and lowers by one and raises by one, keeping fixed, so after steps the comparison is an equality; each of those steps is an existing edge because the current satisfies , so . From then on the non-strict comparison selects the second factor, which offers exactly steps before reaching its bottom. If , all -steps act on the second factor, steps in all. Hence because by , which is (c).
The branch and tie assertions (d). The step counts of steps 2.1 and 2.2 also identify the branch of the first application: for the first maximum entry is attained for , including equality, whereas the first application of uses the first factor only for ; the second entry is attained for and equals ; the first application of uses the first factor exactly for and of exactly for , as displayed in [F1]. In particular the maximal value alone does not determine the -branch, while the strict/non-strict split fixes it.
The partial-inverse property (e). Suppose and ; then by [F3], so the -rule selects the first factor at and . Suppose and ; then and by [F3], so the -rule selects the second factor and . The converse is the same computation read backwards, and at the tie the split non-strict, strict is exactly what makes both readings consistent; this is the partial-inverse axiom already established in [F2], verified here from the explicit two-case logic.
Iteration along the string and the choice audit. By [F3] each existing -edge raises by one and lowers by one, and by step 4.1 the displayed operators are a consistent partial-inverse structure on ; iterating, and for all , which is (f), and the maximal such is by [F3]. All steps were finite checks on the two integer pairs and and the two factor strings; no choice principle is used.
Depends on
- The tensor product crystal $B_1\otimes B_2$ and its two-case convention
- The crystal basis of a tensor product and the two-case operator rule
- The crystal graph, $\varepsilon_i$, $\varphi_i$ and the weight function
- Crystal lattices, crystal bases and their crystals
- The Kashiwara operators $\tilde e_i$ and $\tilde f_i$ of an integrable module
Used by
- Changing the equality case in the tensor rule breaks the partial-inverse axiom Counterexample
- Dual crystals reverse arrows and weights: two small computations Example
- Highest components in the A₂ tensor crystal B(λ₁)⊗ B(λ₁) Example
- The tensor crystal B(1)⊗ B(1) for sl₂ Example
- The dual crystal: reversed arrows, negated weights and swapped ε/φ Proposition
- Highest weight components in a tensor product crystal 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
- Sami Assaf, Anne Dranowski and Nicolle Gonzalez, Extremal tensor products of Demazure crystals, arXiv:2210.10236 (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)
- Mark Shimozono, Crystals for Dummies (lecture notes, 28 August 2005) (standard reference, not scraped)