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The normalized Hecke generator requires inverting v plus one

Example

Over D=C[v,v−1,(v+1)−1], the Jones idempotent generator ei=(Ti+1)/(v+1) is defined. The specialization v=−1 is not a ring map from D to C, because it sends the inverted element v+1 to zero. Moreover, in the specialized two-strand Hecke algebra the element T1+1 is a nonzero square-zero element, so no scalar multiple of it is an idempotent generator.

Facts & Assumptions

Given: The rank-two Hecke quadratic relation and the normalized generator definition.

[F1]

Ti2=(v−1)Ti+v and 1,Ti are distinct standard-basis elements (The generic type-A Hecke algebra).

[F2]

The element ei=(Ti+1)/(v+1) is defined in the localization where v+1 is a unit (The Temperley-Lieb quotient and the Jones specialization).

Verification

technique · direct calculation
1.1F2givenalgebra

A unital map from D to C specializing v to −1 would have to send the unit (v+1)−1 to an inverse of (−1)+1=0. No element of C is an inverse of zero, so the localization has no such specialization. Thus the formula in [F2] does not define ei at v=−1.

2.1F1F2step 1.1algebra∎

In the specialized Hecke algebra, put x=T1+1. The quadratic relation at v=−1 gives T12=−2T1−1, hence x2=T12+2T1+1=0. The standard basis in [F1] shows x≠0 because 1 and T1 are linearly independent. If c∈C and cx were idempotent, then (cx)2=cx would force 0=cx; for c≠0 this contradicts x≠0. Therefore a scalar multiple cannot supply a normalized idempotent at this specialization.

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