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.
Generic quantum Schur–Weyl mutual centralizers over Q(q)
Statement
Let , , , , and let be the images of the quantum and normalized Hecke tensor actions defined above. Then These are equalities for the two matrix-algebra images. If , no faithfulness of the abstract Hecke algebra is asserted. If , the abstract Hecke action is faithful. The theorem is only over the rational function field and asserts no equality at a root of unity, at an arbitrary specialized parameter, or over a field of positive characteristic.
Facts & Assumptions
Given: , integers , the local commuting inclusion, the rank bounds, and the abstract Hecke standard basis.
The two images commute: and (The quantum and Hecke tensor actions commute).
For , the two generic image lower bounds and commutant upper bounds are those of Classical commutants bound the two generic tensor images.
The abstract type-A Hecke algebra has basis over , obtained by base change from the universal standard-basis theorem (The standard basis of the generic Hecke algebra and base change, Universal parameters, the generic Coxeter Hecke algebra and generator conjugacy).
A nonzero minor of a matrix with entries regular at remains nonzero over (Finite matrix rank bounds under regular specialization).
Proof
Given: The data in [F1]–[F4].
Suppose first and . By [F2] and the commuting inclusions [F1], , so every inequality is equality and because the included finite-dimensional subspaces have equal dimension. The other sandwich is , which gives by the same inclusion-and-dimension argument. This establishes both mutual centralizer equalities without generic semisimplicity or a character formula.
Assume . On , the orbit vectors have entries regular at ; their specializations are the distinct tensors obtained by permuting the distinct basis labels. Their vectorized column matrix therefore has an minor equal to at , which remains nonzero over by [F4]. Thus the orbit vectors are linearly independent over . If lies in the kernel, the standard basis [F3] gives this expansion and forces every . Hence the abstract action is faithful.
If , then and both unital images and both commutants are ; the unique unital map from the abstract algebra is the identity, so this action is faithful. If , is one-dimensional; the quantum image contains the scalars and every Hecke generator acts by , so both images and both commutants are again . These direct cases cover the parameters excluded from step 1.1.
In the range the equalities in step 1.1 remain image equalities and do not identify with the abstract Hecke algebra. The distinction is real: for , the abstract algebra has basis by [F3], while its one-dimensional tensor-space action sends to ; the nonzero element is in the kernel. No claim of faithfulness in the full range is used in either centralizer equality.
Depends on
- Classical commutants bound the two generic tensor images
- The quantum and Hecke tensor actions commute
- Finite matrix rank bounds under regular specialization
- The ordered-basis symmetry gives the normalized Hecke tensor action
- The standard basis of the generic Hecke algebra and base change
- Universal parameters, the generic Coxeter Hecke algebra and generator conjugacy
Used by
Nothing in the library uses this result yet.
Dependency tree · two levels
27 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
- Pavel Etingof et al., Introduction to representation theory (standard reference, not scraped)
- Alexei Davydov and Alexander Molev, A categorical approach to classical and quantum Schur–Weyl duality (standard reference, not scraped)