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Eckmann–Hilton duality

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An example is given by currying, which tells us that for any object X, a map X×I→Y is the same as a map X→YI, where YI is the exponential object, given by all maps from I to Y. In the case of topological spaces, if we take I to be the unit interval, this leads to a duality between X×I and YI, which then gives a duality between the reduced suspension ΣX, which is a quotient of X×I, and the loop space ΩY, which is a subspace of YI. This then leads to the adjoint relation ⟨ΣX,Y⟩=⟨X,ΩY⟩, which allows the study of spectra, which give rise to cohomology theories.

We can also directly relate fibrations and cofibrations: a fibration p:E→B is defined by having the homotopy lifting property, represented by the following diagram

and a cofibration i:A→X is defined by having the dual homotopy extension property, represented by dualising the previous diagram:

The above considerations also apply when looking at the sequences associated to a fibration or a cofibration, as given a fibration F→E→B we get the sequence

⋯→Ω2B→ΩF→ΩE→ΩB→F→E→B

and given a cofibration A→X→X/A we get the sequence

A→X→X/A→ΣA→ΣX→Σ(X/A)→Σ2A→⋯.

and more generally, the duality between the exact and coexact Puppe sequences.

This also allows us to relate homotopy and cohomology: we know that homotopy groups are homotopy classes of maps from the n-sphere to our space, written πn(X,p)≅⟨Sn,X⟩, and we know that the sphere has a single nonzero (reduced) cohomology group. On the other hand, cohomology groups are homotopy classes of maps to spaces with a single nonzero homotopy group. This is given by the Eilenberg–MacLane spaces K(G,n) and the relation

Hn(X;G)≅⟨X,K(G,n)⟩.

A formalization of the above informal relationships is given by Fuks duality.

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