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Tor one of R modulo I and M is not always the I-torsion submodule of M

Statement

False claim: for every ideal I◃R, Tor⁡1R(R/I,M) equals {m∈M:Im=0}.

Even for a commutative ring this fails: for any field k, take R=k[x,y], I=(x,y) and M=k=R/I. Then the Tor group is k2, whereas the annihilator submodule is k, so they are not isomorphic as R-modules. Assume DC only for the resolution-independent balanced Tor interpretation; the explicit finite-resolution computation below is choice-free.

Refutation

1.1givenalgebra

Every element of R=k[x][y] is uniquely a finite sum ∑a,b≥0cabxayb. Constant-term evaluation ϵ:R→k is onto and has kernel I: every nonconstant monomial is divisible by x or by y. Multiplication by x in R, and by y in k[y], is injective because it shifts the corresponding coefficient indices.

2.1step 1.1algebra

Consider 0→R→d2R2→d1R→ϵk→0, where d2(c)=(−yc,xc) and d1(a,b)=xa+yb. Its composites are zero; d2 is injective by step 1.1, and im⁡d1=I=ker⁡ϵ. If xa+yb=0, setting x=0 gives yb(0,y)=0, hence b(0,y)=0. Coefficient uniqueness gives b=xc for some c, and then x(a+yc)=0 implies a=−yc. Thus ker⁡d1=im⁡d2 and the displayed augmented complex is exact.

3.1step 2.1algebra

The finite free modules in step 2.1 are projective by the lifting definition Projective modules and the lifting property: lift the images of their one or two specified basis vectors through a surjection, and extend linearly. Only finitely many choices are made; no choice axiom is needed. Commutativity gives the same lifting property on the right, so step 2.1 is a supplied right projective resolution of R/I=k.

4.1step 2.1step 3.1algebra

For r=1,2, the mutually inverse maps Rr⊗Rk→kr, (aj)⊗t↦(ϵ(aj)t), and (tj)↦∑jej⊗tj are well-defined by Universal property of the tensor product for balanced maps into abelian groups. Tensoring the resolution with k therefore gives 0→k→0k2→0k→0, since x,y act by zero. Its degree-one homology is k2, which is the right-resolution Tor group by Tor from a projective resolution of the right module and represents balanced Tor under DC.

5.1step 1.1step 4.1algebra

The cotangent calculation also holds explicitly: I2 consists exactly of polynomials all of whose monomials have total degree at least two. Products of two elements of I have this property, and every such monomial is divisible by one of x2,xy,y2. Consequently every class in I/I2 is uniquely ax+by modulo I2, for a,b∈k, and the classes of x,y are a basis. The isomorphism I⊗Rk→I/I2 sends a⊗t to ta+I2 (view t as a constant); its inverse sends a+I2 to a⊗1. For u,v∈I, (uv)⊗1=u⊗ϵ(v)=0, so the inverse is well-defined. Balancing and the inverse composites follow on the generating tensors.

6.1step 4.1contradiction∎

Because I annihilates k, its annihilator submodule is all of k. There is no k-linear isomorphism k2→k: if the images of its standard vectors are a,b, then for (a,b)≠(0,0) the nonzero vector (−b,a) lies in the kernel, and for (a,b)=(0,0) the entire map is zero. Every R-linear map between these modules is k-linear by the constant scalars. Thus the k2 in step 4.1 cannot be the asserted annihilator module.

Remarks

The refutation retains the two-dimensional polynomial-ring example and proves its entire finite resolution and cotangent calculation locally. It does not invoke a Tor long exact sequence or a later Koszul-complex theorem. The nonisomorphism assertion is about R-modules (equivalently here k-vector spaces), not about abstract additive groups for an arbitrary infinite field.

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