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The four Fock bases in a small two-factor tensor space

Example

Take I={0}, I+={0,1} and Λ=2Λ0 in the conventions of The higher-level wedge-tensor Fock module, so that F=V⊗V has the four monomials M00,M01,M10,M11 in the source normalization of The dual-canonical, canonical and quasi-canonical Fock bases.

In the mixed order (M01,M10), the ordinary bar matrix is Bψ=(1s−1−s01), and both source monomial Gram matrices equal S=Bψ−1, i.e. S=(1s−s−101). All unchanged labels satisfy L=T=M. The remaining vectors are L10=M10−s M01,T10=M10+s−1M01,P01=M01+s M10,P10=M10, and the reverse family has L~01=M~01−s M~10.

The transition and pairing matrices satisfy P‾ tS L=I,L~ tS T=I on the four-dimensional space, the four whole families are pairwise different over Q(s), and both L and T are ordinary-bar fixed, unlike the general quasi-canonical family.

At t=s−1 the highest-module form rescaling is B8(T10,T10)=1+t2,D01=T10s+s−1,Gup=s D01.

Facts & Assumptions

Given: The rank-one Fock model I+={0,1}, Λ=2Λ0, its four monomials in the mixed order (M01,M10), the source bar ψ and families L,T,P of The dual-canonical, canonical and quasi-canonical Fock bases, the forms ⟨−,−⟩, C, C0 and B8, and the projection π of Standard tableau monomials form a basis of the highest weight Fock submodule.

[F1]

Source bar and families (The dual-canonical, canonical and quasi-canonical Fock bases, The higher-level wedge-tensor Fock module): the monomial basis and its weights; the triangular charts d,p; the delta pairings ⟨PA,LB⟩=δAB, C(L~A,TB)=δAB.

[F2]

The normalized quasi-R supplier Existence and uniqueness of the weightwise quasi-R intertwiner gives Θα0=(t−t−1)E0⊗F0; the tensor bar is supplied by The tensor-product bar on the Fock module and its truncation compatibility, with t=s−1. Its fixed-vector equation is c=Bψcˉ.

[F3]

Highest constituent and rescaling (Standard tableau monomials form a basis of the highest weight Fock submodule, The highest weight Fock submodule carries the quantum-group global bases): the projection π, the source dual-canonical basis on StdΛ, and the weight rescaling B8=s−aC0 with Gup(A)=saDA.

Verification

technique · direct
1.1F2algebra

The bar matrix. Each natural-factor bar fixes its two coordinate vectors. The only nonconstant quasi-R term acting on this tensor square is (s−1−s)E0⊗F0; it takes M10 to (s−1−s)M01 and kills the other three monomials. Higher terms vanish because E02=F02=0 on a natural factor. This gives the displayed Bψ in the mixed order (M01,M10).

2.1F1step 1.1algebra

The four families. A vector M10+cM01 is bar fixed exactly when c−cˉ=s−1−s. The two triangular charts give c=−s for the sZ[s]-chart and c=s−1 for the s−1Z[s−1]-chart, that is L10=M10−sM01 and T10=M10+s−1M01. The quasi-canonical family is defined by the inverse transition matrix, giving P01=M01+sM10 and P10=M10; the reverse reading gives L~01=M~01−sM~10. Since the off-diagonal entries are −s, s−1 and s, the four families are pairwise different over Q(s).

3.1F1step 2.1algebra

The Gram matrices and delta identities. The defining forms have labelled monomial Gram matrices equal to the inverse ordinary-bar matrix, so S=Bψ−1=(1s−s−101) for both forms, as displayed. Substituting the coefficient matrices of step 2.1 and multiplying the resulting 4×4 matrices (which are the identity on the 00- and 11-labelled directions) gives P‾ tSL=I and L~ tST=I exactly; these are the delta identities ⟨PA,LB⟩=δAB and C(L~A,TB)=δAB of [F1].

3.2F3step 2.1algebra

The form rescaling. The mixed-weight vector in the highest constituent is T10=F0M00; its norm under the normalized bilinear form C0 is [2]s=s+s−1, and by [F3] the library polarization gives B8(T10,T10)=s−1[2]s=1+t2 at t=s−1. The projected dual-canonical vector is D01=πL01=T10/(s+s−1), and the library form-dual upper vector is its rescaled Gup=sD01, which checks the exact rescaling of [F3] without asserting that the source D-family itself is the library upper family.

4.1step 1.1step 2.1step 3.1step 3.2∎

Conclusion. In this four-dimensional model the ordinary bar matrix is Bψ, both Gram matrices are S=Bψ−1, the displayed L,T,P,L~ vectors are the four distinct source families with the stated delta pairings, and the highest-component rescaling checks B8(T10,T10)=1+t2, D01=T10/(s+s−1) and Gup=sD01.

Depends on

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