The tensor differential. Use homological grading, so each differential lowers degree by one. The tensor product of chain complexes has
for . This Koszul sign rule gives
Thus the graded tensor product is a chain complex.
The Hom differential. Write . For a degree- element of this graded Hom complex of chain complexes, use the prescribed differential
The next application uses degree , so
In degree zero, , so its kernel consists exactly of chain maps. A degree-one element has , which is exactly the change between two chain maps related by a chain homotopy. Consequently
This is natural: precomposition and postcomposition by chain maps preserve both degree-zero cycles and degree-zero boundaries.
The dual complex and the sign adjustment. Define the reversed dual chain complex
Here is a functional on , so it belongs to , and . The absence of an additional sign in is intentional.
Interpret finite generation of the free chain complexes as finiteness of their total graded free modules. Then only finitely many degrees occur, and the finite-free evaluation isomorphisms assemble into a graded isomorphism
where , , and this component is zero outside . The dual module construction and evaluation make natural. Finite rank is needed for evaluation to be an isomorphism; finite total support also makes the sums on the tensor side agree with the products on the Hom functor side.
Under , the Hom functor differential has the form
The usual tensor product of chain complexes instead has second coefficient . Set
This is integer-valued for every , including negative , and satisfies . Conjugating the usual tensor differential by leaves the first term unchanged and changes its second coefficient to . Hence , giving the sign conjugation for the tensor-Hom identification
This is an isomorphism of chain complexes, not merely of their homology. If one instead assumes only degreewise finite rank with unbounded grading, the ordinary tensor need not identify with the product defining ; the finite-total convention is essential to this last conclusion.
We use the James reduced product theorem and the Bott–Samelson theorem: if is a connected based CW complex with free integral homology, then is a weak equivalence, and its induced Pontryagin ring is
Here is the reduced suspension, is the tensor algebra, and the multiplication is induced by concatenating James words, hence by concatenating loops. Taking supplies a single generator of degree , so
is free, with one generator in every degree and zero in the other degrees.
The diagonal makes this a homology coalgebra. The generator is a primitive homology class:
There are no nontrivial lower positive degrees in which its reduced diagonal could land. Compatibility of the diagonal with loop multiplication gives
The degree of is even, so the two tensor factors commute without a Koszul sign rule.
The universal coefficient theorem for cohomology has no Ext terms here because homology is free. Let be the cohomology class dual to , with and . The cup product is dual to the diagonal, hence
Therefore the integral cohomology ring is the divided power algebra
Explicitly for , and all other cohomology groups vanish. In particular : over the integers this is not a polynomial ring on . This is the integral cohomology of an odd-sphere loop space.
For the requested homology multiplication, use the homology cross product followed by concatenation:
The constant loop gives the degree-zero unit. Loop concatenation is associative up to homotopy, which suffices for associativity on homology; Moore loops can make the space-level operation strictly associative. The Künneth theorem identifies the tensor-product homology because its groups are free abelian groups. The Bott–Samelson theorem identifies this product with word multiplication, so . The Pontryagin ring of an odd-sphere loop space has presentation
With only one generator the tensor algebra has the indicated polynomial presentation. The homology product and the divided-power cohomology product are different operations.