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The rank-one tensor action of the two-strand Hecke algebra is not faithful

Statement refuted

For every N≥1 and n≥0, the normalized type-A Hecke algebra Hn(Q(q)) acts faithfully on VN⊗n through the ordered-basis Hecke operator.

Facts & Assumptions

Given: F=Q(q), the type-A Hecke algebra with quadratic relation (T1−q)(T1+q−1)=0, and the tensor-power action defined from the ordered-basis operator.

[F1]

The generic Hecke algebra has standard basis {Tw:w∈W}, and this basis remains a basis after base change (The standard basis of the generic Hecke algebra and base change).

[F2]

The type-A Hecke algebra is the specialization of the universal Coxeter Hecke presentation at common parameter q (Universal parameters, the generic Coxeter Hecke algebra and generator conjugacy).

[F3]

Sending Ti to the ordered-basis operator on positions i,i+1 defines an algebra action on every tensor power (The ordered-basis symmetry gives the normalized Hecke tensor action).

[F4]

On equal labels the ordered-basis operator is T(ea⊗ea)=q(ea⊗ea) (The ordered-basis Hecke operator and its normalization).

Counterexample

Given: Take N=1, n=2, V1=Fe1, and the Hecke action ρ2 on V1⊗2.

1.1givenF1F2F3F4algebra

In type A1 the Coxeter presentation has one generator s with s2=1, so every word reduces to 1 or s; the map s↦1ˉ to the two-element group is well-defined and nontrivial, so these are distinct and the Coxeter group has exactly two elements. Thus [F1]–[F2] give the F-basis 1,T1 of H2(F). By [F3]–[F4], T1 acts on the one-dimensional tensor square by ρ2(T1)(e1⊗e1)=q(e1⊗e1); hence T1−q1 lies in the kernel of ρ2.

2.1givenF1step 1.1algebra∎

In the basis 1,T1, the element T1−q1 has coefficients (−q,1), which are not both zero in F. Thus it is a nonzero element of H2(F) mapped to zero, so ρ2 is not injective and the universal faithfulness statement is false.

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