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The canonical and quasi-canonical bases need not coincide
Statement refuted
In the four-dimensional model of The four Fock bases in a small two-factor tensor space the canonical and quasi-canonical Fock families coincide on every label.
Facts & Assumptions
Given: The rank-one Fock model with monomials , the source families of The dual-canonical, canonical and quasi-canonical Fock bases, and the computed bar matrix and vectors of The four Fock bases in a small two-factor tensor space.
Bar and families (The tensor-product bar on the Fock module and its truncation compatibility, The dual-canonical, canonical and quasi-canonical Fock bases): is triangular with and fixes the other monomials; the canonical family is the -chart and the quasi-canonical family is defined by the inverse transition matrix.
Highest constituent (The highest weight Fock submodule carries the quantum-group global bases, Standard tableau monomials form a basis of the highest weight Fock submodule, The four Fock bases in a small two-factor tensor space): the projection , the rectified highest label , and the rescaling on the highest constituent with .
Counterexample
Take , , , and retain the mixed order and the notation of The dual-canonical, canonical and quasi-canonical Fock bases and The four Fock bases in a small two-factor tensor space. There because ; but over . Hence the canonical and quasi-canonical families are different, and so are the dual-canonical and monomial families. The highest-component label rectification is with , which exhibits the genuine power and label distinction: the coincidence happens on the rectified highest label, not by an identity of the two index sets. At the highest-submodule vectors and agree after rectification, but the full canonical and quasi-canonical families are still not interchangeable. This is no claim that every corresponding label differs at .
Proof technique: direct.
The two families at label . In the mixed order the bar fixes and sends to . A vector is fixed exactly when . The positive chart gives and the negative chart gives ; uniqueness follows because a bar-fixed polynomial in either or is zero. Thus , and . Inverting the chart gives , so the transposed inverse chart is and . Linear independence of the two monomials proves .
The rectified highest-label coincidence. At label the same computations give , so the two families do meet at the rectified highest label with the power of [F2]; this is an identity between specific vectors, not an identification of the two labelled families.
Conclusion. Since , the canonical and quasi-canonical families are different over ; the dual-canonical and monomial families differ too, because . The highest-submodule coincidence is exactly the rectified normalization of [F2], and at it does not make the whole families interchangeable.
Depends on
- The dual-canonical, canonical and quasi-canonical Fock bases
- The higher-level wedge-tensor Fock module
- The column monomial basis of the higher-level Fock module
- Parabolic Kazhdan-Lusztig polynomials give the dual-canonical transition matrix
- The highest weight Fock submodule carries the quantum-group global bases
- The lower global basis of $U_q^-$ and of a highest weight module
- The upper (form-dual) global basis and the required perfectness of the integral pairing
- The four Fock bases in a small two-factor tensor space
- Standard tableau monomials form a basis of the highest weight Fock submodule
- The tensor-product bar on the Fock module and its truncation compatibility
Used by
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Sources
- Jonathan Brundan and Alexander Kleshchev, The degenerate analogue of Ariki's categorification theorem, Math. Z. 266 (2010) 877-919 (complete 44-page arXiv article) (standard reference, not scraped)
- Jonathan Brundan, Dual canonical bases and Kazhdan-Lusztig polynomials, J. Algebra 306 (2006) 17-46 (complete 29-page arXiv v2 article) (standard reference, not scraped)