Christian Marks

Ecumenical dispatches from the London Library

A co-topological category

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This post describes a nearly useless category that reminds me of the topologies associated with categories of coalgebras for a set endofunctor.

Let {X, Y} be topological spaces. A not-necessarily continuous map {f:X\rightarrow Y} is open if for every open set {U\subset X}, {f[U]} is open in {Y}. The category {\mathbf{Opt}} of topological spaces and open maps has the same isomorphism types as the category {\mathbf{Top}} of topological spaces and continuous maps.

Proof: A map is an isomorphism in {\mathbf{Opt}} if and only if it is a homeomorphism in {\mathbf{Top}}. \Box

Coproducts exist in {\mathbf{Opt}}. In general, products do not exist in {\mathbf{Opt}}. However, something analogous to powers of a single space exist.

For a topological space {X}, {\square X} (“the square of {X}“) denotes the topological space with underlying set {X\times X} and topology generated by the basis

\displaystyle  \{ U\times V, \Delta_X[U] : U,V\,\mathrm{open}\,\mathrm{in}\,X\}

where {\Delta_X:X\rightarrow X\times X} is the diagonal. This topology is the smallest topology on {X\times X} making the diagonal map open (and continuous).

The {\square} construction defines an endofunctor {\square} on {\mathbf{Opt}} together with a natural transformation {\delta_X:X\rightarrow\square X} (the same underlying map as {\Delta_X}) from the identity functor {1_\mathbf{Opt}} to {\square}. There is a one-to-one correspondence between maps {f:X\rightarrow Y} and maps {g:X\rightarrow\square Y} such that {\pi_1 g= \pi_2 g} for {i=1,2}, where {\pi_i:\square Y\rightarrow Y} is the projection (projections are open).

Proof: Given a open map {f:X \rightarrow Y}, the open map {\delta_Y f} satisfies {\pi_1\delta_Y f = f = \pi_2 \delta_Y f}. Conversely, a map {g:X\rightarrow \square Y} with {\pi_1 g= \pi_2 g} for {i=1,2}, defines {f=\pi_1 g}. Then

\displaystyle \delta_Y f = (\pi_1 g \times \pi_1 g) \delta_Y = (\pi_1 g \times \pi_2 g) \delta_Y = (\pi_1 \times \pi_2) \delta_Y g = g

\Box

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Written by Christian Marks

July 6, 2011 at 3:37 AM

Posted in Bagatelle

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