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The link-state Gram form is symmetric and invariant

Statement

Let R, δ, n, t and Wn,t(R,δ) be as in Temperley–Lieb link-state standard modules by defect number. For link states x,y, let x∗ denote reflection across a horizontal line. The diagram y∘x∗:t→t is either δc1t for some c≥0 or has fewer than t propagating components. Define ϕn,t(x,y)=δc in the first case and 0 in the second, and extend R-bilinearly. Then ϕn,t is symmetric and satisfies

ϕn,t(x⋅a,y)=ϕn,t(x,y⋅a∗)

for all x,y∈Wn,t(R,δ) and a∈TLn(R,δ). Here a∗ is reflection across a horizontal line. The matrix of ϕn,t in the link-state basis is the Gram matrix obtained by reflecting and capping two link states, with one factor δ for each closed loop.

Facts & Assumptions

Given: A commutative ring R with unit, δ∈R, n≥0, an allowed t, and link-state representatives in MR(n,t).

[F1]

The link states are the basis cosets of diagrams with t propagating components, and the right action is x⋅a=[x∘a] (Temperley–Lieb link-state standard modules by defect number, The link-state quotient is a right Temperley–Lieb module).

[F2]

Diagram composition is associative and each closed component contributes one factor δ (Temperley–Lieb planar diagram data and endomorphism modules, Stacking is associative and horizontal juxtaposition is strict monoidal).

Proof

technique · direct
1.1F1F2givenconstruct

For basis link states x and y, the composite y∘x∗ is a diagram from t to t. If all t boundary points propagate, planarity forces them to connect in their order, so after removing c closed loops the result is δc1t for a unique c. Otherwise it has fewer than t propagating components. Thus the stated value is determined by the matching and loop count, and it extends uniquely to an R-bilinear form on the free link-state basis [F1, F2].

2.1F1F2step 1.1

Reflection reverses the order of stacking, fixes each scalar δ, and sends y∘x∗ to x∘y∗. Hence y∘x∗=δc1t exactly when x∘y∗=δc1t with the same c; the lower-propagating case is also preserved. Therefore ϕn,t(x,y)=ϕn,t(y,x) on basis states and, by bilinearity, on all module elements.

3.1F1F2step 1.1step 2.1∎

For basis states x,y and a basis diagram a∈TLn, reflection gives (x∘a)∗=a∗∘x∗. Both form values are therefore the coefficient of 1t in the same associative composite y∘(x∘a)∗=y∘a∗∘x∗=(y∘a∗)∘x∗. They have the same exterior matching and number of removed loops, so their coefficients of 1t agree. If an intermediate term has fewer than t propagating components, it remains lower-propagating after further stacking and contributes zero on both sides. This proves the invariance identity for basis states and basis diagrams; bilinearity proves it for all x,y,a.

Depends on

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