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Do you mean topological spaces? Does "/X" mean what I wrote as "↓X"? Don't we need to at least restrict it to only include epic arrows?Hurkyl said:If T is the category of spaces, then T/X is precisely the category of bundles over X. The fiber bundles are a full subcategory therein.
This is how I think of fiber bundles. Every surjection [itex]\pi:E\rightarrow B[/itex], partitions its domain into disjoint subsets of the form [itex]\pi^{-1}(b)[/itex] with [itex]b\in B[/itex]. This surjection is all we need to define a fiber bundle in the category of sets. If we add the requirements that E and B are topological spaces, and require that [itex]\pi[/itex] is continuous, we get a fiber bundle in the category of topological spaces. And we can of course do something very similar with manifolds.
Are you distinguishing between "bundles" and "fiber bundles"? I suppose we could call what I just described "bundles" and reserve the term "fiber bundle" for those cases when all the [itex]\pi^{-1}(b)[/itex] are isomorphic. Is that what you're doing?
I understand that model theory is only guaranteed to answer the question when we've been given exact information about which symbols are to be considered part of the structure. But that covers a lot of cases, and it's not clear (to me) how far this can be generalized. I would be very surprised if it can't be generalized to at least include metric spaces and vector spaces, and I expect that it can also be generalized to manifolds and fiber bundles.Hurkyl said:Not really -- it has the same problem. Model theory tells you what the homomorphism are if and only if the particular structure you are interested in is "models of a particular theory" -- and even then you have to know which theory.
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It's common to define structures to be models of a particular choice of first-order theory. If you do so, then obviously model theory tells you what the homomorphisms are.
A part of the reason why I want to define structures as "sets with additional stuff" is...physics. For example, suppose that we're trying to define a new theory of physics, and that this specific theory is built up around a vector space. The theory is defined by a set of axioms that tells us how to interpret some of the mathematics as predictions about results of experiments. Now it would be interesting to find out which other vector spaces we could have used in the definition of the theory. If we define our isomorphisms as structure-preserving bijections, we're guaranteed that isomorphic structures will work equally well in the theory. If we define them by choosing some random bunch of functions that are consistent with the category theory requirements on "arrows", it's not at all clear that isomorphic objects in the category work equally well in the theory.Hurkyl said:Of course, the same is true of category theory. If you define structures as "objects in a category", then obviously category theory tells you what the homomorphism are.
I'm aware that my approach wouldn't give us all the structures we could have used in the theory. For example, except for some issues with what coordinate systems we're allowed to use, SR works equally well with spacetime defined as a vector space instead of as a manifold. Structure-preserving maps don't tell us that, but then neither does category theory.
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