Foliation
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so thank you for the introduction thanks
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for sticking around for this last
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let's talk here so yes the basic complex
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of a singular affiliation
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um so this is a result I worked out for
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part of my thesis which
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will soon be completed
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um and uh so it has to do with singular
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foliations so we'll begin with the
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definition of a singular foliation
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especially these days the term could
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maybe be ambiguous so I have to pin down
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what I mean so for me a singular
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affiliation will be a partition of a
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manifold
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into leaves and these or by Leaf will
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mean a connected and weakly embedded sub
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manifold
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so it's a partition of a manifold into
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these sub manifolds and there's a
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smoothness condition so they need to fit
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together smoothly
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in the following sense
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so it's a bit wordy but I don't think
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it's too bad for each point in the
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manifold you can find a collection of
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vector fields
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and
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these Vector Fields will locally span
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the tangent spaces to the leaves in the
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neighborhood
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so in particular they have to spend the
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attention space to the leaf at X but
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also the leaves near X
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and the reason this is a singular
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foliation or potentially singular one is
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that there's no there were Vector Fields
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can depend on the point x so at
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different points you might have lower
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dimensional leaves
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things can change around as you go
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through the manifold
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there's a small comment on this weekly
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embedded assumption uh it's a bit
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stronger than immersed all it means is
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that the uh or consequence for us is
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that the smooth structure on the leaves
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is unambiguous it's completely
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determined by the leaf as a set and the
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ambience manifold structure so I don't
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need to worry about equipping them with
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um I don't need to worry about this
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restructure on the leaves
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specifying what it is
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uh so give a definition here's an
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example I started off with sort of the
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most
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one of the more General ways you can
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approach it so if you have a lead
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algebraid then the integral sub
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manifolds will assemble into a singular
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foliation
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and
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more Elementary examples are sort of can
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be deduced from this so for instance uh
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connected components of the orbits of a
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lead group action will partition your
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manifold into a singular foliation and
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also the synclectic leaves of a poisson
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manifold will give a singular foliation
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Okay so
Motivating question
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what will we do with these uh the
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question I'm sort of interested in is
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taking a singular foliation and looking
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at the leaf space
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and well what I'll do is I want to use
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What's called the diffiological
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structure on this Leaf space to probe
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information about the transverse
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geometry so here we're going to do a bit
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of a comparison
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which will make precise in a second
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so the leaf space will denote by m mod f
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and like I said it has a natural
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so-called diffiological structure
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so I think Eugene mentioned ethiology
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briefly in his talk in the beginning uh
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it's one of the various Notions of
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generalized smooth structure we can put
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on a set
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I don't want to dwell too much on the
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definition so I just put it a bit
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vaguely here
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due to Chen and Syria independently so a
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diffiology will have a set and we'll
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equip it with a set of maps from various
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euclidean spaces or open subsets of
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euclidean spaces into X and these Maps
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which are called plots will essentially
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determine what it means to be smooth
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so if we have a function from a
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difficult Space X we'll use the plots to
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Define what it means for that function
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to be smooth
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Etc
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in the footnote I gave a brief
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description of these axioms that a
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collection of plots must satisfy but
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again I think I don't want to go too
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much into it because that's basically a
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talk on its own or a 15-minute talk on
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its own
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but the idea is that this Leaf space has
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more structure than its apology it has a
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diffiology
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and so I can give a put a vague
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formulation of The Guiding question here
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what aspects of the foliation sitting
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upstairs can we recover from the leaf
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space viewed as a diffiological space
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and just to give a small motivation as
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to why this might make sense to ask if
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we consider an orthogonal group action
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on RN
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for different ends topologically this
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quotient is just a half Ray and you
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can't tell the different half Rays apart
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from the different dimensions that you
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started with but the diffiological
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structure will be distinct for each of
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these no two will be diffiomorphic
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so I can see these are all
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the theologically
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distinct
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so it's a small reason to believe that
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this question is not hopeless
Downstairs: the leaf space
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so we're going to approach this using
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basic complex so first downstairs on the
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leaf space itself we have the following
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facts that we get from equipping it with
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the diffiology so first the quotient map
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is a smooth map as it probably should be
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moreover it's actually what's called a
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subduction which is a diffiological
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version of submersion
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um diffiological spaces always come
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equipped with a complex of differential
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forms
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so this is that side of things works
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very well
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there's nothing special about it being a
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quotient for these
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complex to exist
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it's just the diffiological structure
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and finally the
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smooth quotient map gives a pullback of
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complexes of differential forms so we
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have the forms on the oops
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yeah we have the forums on there Leaf
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space and they pull back to right now
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it's just forms on the manifold
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so this is a complex we'll look at
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downstairs this Omega M mod f
Upstairs: basic forms
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on the other hand if we don't want to
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pass to the leaf space we can stay with
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the foliation upstairs and we can
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consider What's called the complex of
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basic forms the second part of the title
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this was first introduced by Reinhardt
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in 59th uh he did he was working with
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regular foliations at the time but we
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can make the same definition for
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singular ones so we'll call a
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differential form on the manifold basic
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if it is
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horizontal so this interior derivative
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Vanishing is called horizontal and
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invariant
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this lead derivative Vanishing is called
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invariance and the X we take are those
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which are tangent to the foliation
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if you have a foliation induced by a
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connected Lee group action then
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invariance really just means invariance
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under the group action
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but the horizontal condition just stays
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the ways
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and the notation so we'll call this
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Omega sub b m f
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okay
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so now we have two complexes of
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differential forms
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morally whoops
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these basic forms should capture
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transverse geometry but so should these
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forms on the quotient since that is the
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leaf space itself
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and we also have conveniently the
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pullback by the quotient so we can ask
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how does the pullback compare these two
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complexes and we begin with this little
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Lemma again this is a consequence of
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General results in diffiology so the
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pullback will restrict to amorphism of
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these complexes
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so it will always go into basic forms
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and it's also injective
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uh yeah yeah yeah yeah yeah yeah yeah
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yeah yeah
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and uh yeah so here you have injective
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and then sort of the more formal version
Specific question (and partial answer)
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of the question I started with uh we're
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going to specifically ask when is it an
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isomorphism
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and in particular uh because of this
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earlier Lemma we're really asking when
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is it on to
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and that's the result that we have
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so I did this maybe not a little like a
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year ago or so
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I guess that's two years now anyway uh
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so we have the quotient will induce an
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isomorphism
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or will be subjective
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in the following three cases so first
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when f is regular
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and I later found that this was also
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done by Hector marcius Virgos and San
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Martin carbon in 2009
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and also uh Elin and chandong yang also
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have an argument for this to be true in
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one of their recent preprints
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uh so when f is a regular foliation
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we are onto
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more generally though uh we can now go
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to singular foliations and the following
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condition suffices so
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for each
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k for each dimension of the leaves look
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at all the leaves of that dimension
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take the union so it's a subset of the
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manifold and require that this Union is
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a sub manifold
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now I'm a bit General in what I mean by
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sub manifolds but we can just take
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weekly embedded or you could think
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embedded if you want
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uh most of the examples it's an embedded
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manifold so for each K that Union of
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leaves is a sub manifold then the
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pullback will be an isomorphism for that
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singular foliation
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I'd like to call this stratified you
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know the foliation is stratified by
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Dimension or something but I don't know
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that it's a stratification in the sense
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that that word usually used
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that's why I don't write it here
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and there's a finally a third strange
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sort of condition that we can have which
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is more General than the previous two uh
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if you discard all the zero leaves
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from your manifold that's what is M
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bigger than zero is
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and then you equip it with the foliation
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where you remove those zero leaves
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and if the pullback is an isomorphism
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for that
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open subset of your manifold
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then you can throw the zero leaves back
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in and it will remain an isomorphism
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so somehow this question of when the
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pullback is an isomorphism you can
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sprinkle in zero leaves however you like
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in any closed subset and you'll remain
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in isomorphism if you started off as one
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which I think it's a bit strange to
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you can make some strange examples with
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this
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okay and uh yeah irmrn is where this can
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appear
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how about that five minutes
Small example
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okay
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um I just wanted to give a little
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example of me how to to see how the
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diffiology
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sort of works or how you might use it
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um consider the action of sln on
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matrices by left multiplication
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then we want to sort of ask what are the
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basic forms for this foliation of the
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set of matrices and we make the
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following diagram so we split the
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determinants into the quotient map and
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this map I just call it C
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then
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on the difficulty theology side you can
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prove that this C induces an isomorphism
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on the complexes of differential forms
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from R to X X so the diffiology is here
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to make sense of that
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and then
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the theorem comes in because we're in
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case two there's a sort of decomposition
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by dimension for this action and so then
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we know that the quotient will give an
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isomorphism
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and when you put these together we can
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see that pulling back by the
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determinants gives you all the basic
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forms
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for this little example
Bigger examples
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some more sophisticated examples I guess
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I call them bigger uh if we have a
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properly groupoid
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then linearization theorems tell us that
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we're in this decomp decomposed by
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Dimension case
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this item two
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and this uh you can use that fact to
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sort of reproduce work by karshan and
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Watts
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um on the same question in a more a more
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special case of a group acting properly
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or more generally a group whose identity
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component acts properly so you can
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reproduce some earlier results with this
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um
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you can also say for a Romanian singular
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foliation
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results by Molino from the 80s tell you
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that these foliations are decomposed by
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dimension so for each K the union of K
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leaves is a sub manifold in fact in that
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case it's embedded
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and I just want to make a little note
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that this second example actually
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subsumes the first one uh using the hoyo
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and Fernandez's linearization uh you can
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say that every properly groupoid induces
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a singular singular Romanian foliation
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on the base
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the its orbits are singular Romanian
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affiliation so then the second one
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really gives you the first one
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and finally using this sort of stranger
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third part where the zero leaves don't
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matter so to speak any one-dimensional
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singular foliation uh the quotient will
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have this
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property of being an isomorphism when
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you pull back
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because when you remove the zero leaves
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you just have a one a regular
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one-dimensional foliation
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so you can use this to generate a lot of
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examples where the quotient is an
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isomorphism
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but of course that's not all the
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singular relations that could exist so
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there's two sort of big
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well big for me I guess unknown
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questions here so first I don't know of
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an example where Pi star is an
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isomorphism
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and it's not covered by this theorem
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so I don't know of a singular
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affiliation that's not one of those
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three types earlier where Pi star is
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still a an isomorphism
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and
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bigger than that I don't know if there's
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a counter example
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it would be I think interesting if there
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was one uh what type affoliation that
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would look like
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and I'm not sure
Key points in the proof
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so in the last I think of 15 seconds I
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guess the only item I'll highlight here
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is that
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um to do this decomposed by Dimension
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case uh the fact requiring them to be
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sub manifolds allows us to do induction
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and sort of on each level for each K you
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have a manifold with a foliation
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so you use the fact you know it's a
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isomorphism when you have a foliation
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and you can sort of piece it together to
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get the entire quotient as an
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isomorphism
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so that's yeah thank you for your
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attention
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[Applause]