2023-05-14

279: Product of Connected Topological Spaces Is Connected

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A description/proof of that product of connected topological spaces is connected

Topics


About: topological space

The table of contents of this article


Starting Context



Target Context


  • The reader will have a description and a proof of the proposition that the product of any connected topological spaces is connected.

Orientation


There is a list of definitions discussed so far in this site.

There is a list of propositions discussed so far in this site.


Main Body


1: Description


For any product topological space, T=×αATα where A is any possibly uncountable indices set, such that each Tα is connected, T is connected.


2: Proof


Let us suppose that T was not connected. T=U1U2,U1U2=, U1 and U2 where Ui would be an open set. Ui=βBi×αAUiβα where Bi would be any possibly uncountable indices set, Uiβα would be an open set such that each of only a finite number of Uiβαs would not be Tα for each i and β, by the definition of product topology.

Let us take any point, pγπγT, where πγ would be the projection of T to Tγ:=×αA{γ}Tα. Let us define Biγ:={βBi|pγ×αA{γ}Uiβα} and Uiγ:=βBiγUiβγ. U1γU2γ=Tγ, because for any pγTγ, the corresponding point, pT, such that πγp=pγ and πγp=pγ would be in ×αAUiβα for a βBiγ, as pU1 or pU2. U1γU2γ=, because if pγU1γU2γ, the corresponding point, pT, such that πγp=pγ and πγp=pγ would be in U1U2.

As Tγ is connected, U1γ= or U2γ=, which would mean that for any fixed pγ, all the pγTγs would be entirely in U1 or in U2. Let us suppose that U2γ= and so, inevitably U1γ=Tγ without loss of generality. For any pγU1γ, pγU1βγ for a βB1γ, and the corresponding point, pT, such that πγp=pγ and πγp=pγ would be in a ×αAU1βα for a βB1γ.

But there are only finite number of U1βαs such that U1βαTα for the β. Let us define Aβ as the set of such αs, {α1,α2,...,αn}. Then, every point, pT, such that παAβp=pαU1βα for every αAβ would be in ×αAU1βαU1. α1 could be taken to be the γ of the above procedure, then, every point, pT, such that παAβ{α1}p=pαU1βα for every αAβ{α1} would be in U1, because as the 1 pα1 is known to be in U1, the whole Tα1 have to be in U1. Then, α2 could be taken to be the γ of the above procedure, then, every point, pT, such that παAβ{α1,α2}p=pαU1βα for every αAβ{α1,α2} would be in U1, likewise, and so on. After all, every point, pT would be in U1, a contradiction.


References


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