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A Deligne kernel need not be one external tensor factor

Statement refuted

Under the identification Aop⊠B≃(B,A)-bimod of The opposite Deligne product is the category of finite bimodules, not every object is one external tensor factor aˉ⊠b. Witness: for the upper triangular k-algebra A0 with basis e1,e2,u, unit 1=e1+e2, e12=e1, e22=e2, e1u=u=ue2 and all other basis products zero (Algebras over a commutative ring, central structure maps, and algebra homomorphisms, Vector space over a field, Finite-dimensional vector space, and its dimension dim⁡FV; infinite-dimensional means having no finite basis), the regular bimodule A0 has dimension 3, and it is not isomorphic to b⊗ka∗ for any finite-dimensional left A0-modules a,b: if it were, one of dim⁡kb,dim⁡ka would be 1, and a one-dimensional left or right A0-module has u acting as zero (Simple module: a nonzero module with no proper nonzero submodule), forcing the left (if dim⁡kb=1) or right (if dim⁡ka=1) multiplication by u on b⊗ka∗ to vanish; on the regular bimodule left multiplication by u sends e2 to u≠0 and right multiplication by u sends e1 to u≠0 ((S,R)-bimodules and commuting left and right scalar actions, Unital left and right modules over a ring; unqualified module means left module, Linear map between vector spaces over the same field), a contradiction in either case.

Facts & Assumptions

Given: A field k and the k-algebra A0 with k-basis e1,e2,u, unit 1=e1+e2, e12=e1, e22=e2, e1u=u=ue2 and all remaining products of basis elements zero; the regular bimodule A0(A0)A0; and finite-dimensional left A0-modules a,b.

[F1]

A left A0-module is an abelian group with a scalar action satisfying r(m+n)=rm+rn, (r+s)m=rm+sm, (rs)m=r(sm) and 1m=m, and dually on the right (Unital left and right modules over a ring; unqualified module means left module); on a one-dimensional module the action is a k-linear map into scalars, so all products and sums of actions are computed by the corresponding relations in A0 (Linear map between vector spaces over the same field, Vector space over a field); a one-dimensional module has no nonzero proper submodule, hence is simple (Simple module: a nonzero module with no proper nonzero submodule).

[F2]

For finite-dimensional k-vector spaces the dimension is the cardinality of a basis, and the products xi⊗λj of bases (xi) of b and (λj) of a∗ form a basis of b⊗ka∗ by the universal property of the tensor product; hence dim⁡k(b⊗ka∗)=dim⁡kb⋅dim⁡ka∗, and dim⁡ka∗=dim⁡ka for a∗=Hom⁡k(a,k) (Finite-dimensional vector space, and its dimension dim⁡FV; infinite-dimensional means having no finite basis, Generated submodule, cyclic and finitely generated modules, module basis and free module, Universal property of the tensor product for balanced maps into abelian groups, Linear functionals and the algebraic dual V∗=L(V,F)).

[F3]

An isomorphism of (A0,A0)-bimodules is a bijection that is linear over k and intertwines both actions, so it preserves k-dimensions and the vanishing of the two multiplications ((S,R)-bimodules and commuting left and right scalar actions); the external objects aˉ⊠b in the identified category correspond to the bimodules b⊗ka∗ (The opposite Deligne product is the category of finite bimodules).

Counterexample

1.1givenF1F2

The specified algebra is the upper triangular 2×2 matrix algebra under e1↦E11, e2↦E22, u↦E12, so the products are associative and define a unital algebra. In A0 the relations e1+e2=1, e1e2=e2e1=0 and e1u=u=ue2 hold with e1,e2,u a k-basis of the regular bimodule, so left multiplication by u sends e2 to ue2=u≠0 and right multiplication by u sends e1 to e1u=u≠0, while A0 has k-dimension 3 [F1, F2].

2.1step 1.1F1

On a one-dimensional left or right module, the action of u is multiplication by a scalar c∈k. Since u2=0, the module law gives c2=0, hence c=0 because k is a field. Thus u acts as zero on every one-dimensional module on either side.

3.1step 2.1F2F3∎

Suppose the regular bimodule A0 were isomorphic to b⊗ka∗. By [F3] the two sides have the same k-dimension and the same vanishing pattern of the two multiplications, and by [F2] 3=dim⁡kA0=dim⁡kb⋅dim⁡ka∗=dim⁡kb⋅dim⁡ka, so one of the two factors is one-dimensional. If dim⁡kb=1, then left multiplication by u is zero on b by step 2.1, hence zero on b⊗ka∗ because u⋅(x⊗λ)=(ux)⊗λ=0, contradicting step 1.1, where left multiplication by u sends e2 to u≠0. If dim⁡ka=1, then u acts as zero on a, so (λ⋅u)(x)=λ(ux)=0 for every λ∈a∗, and right multiplication by u is zero on b⊗ka∗ because (y⊗λ)⋅u=y⊗(λ⋅u)=0, contradicting step 1.1, where right multiplication by u sends e1 to u≠0. Both alternatives contradict the assumed bimodule isomorphism, so the regular bimodule A0 is not isomorphic to any external tensor factor b⊗ka∗.

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