Want to take part in these discussions? Sign in if you have an account, or apply for one below
Vanilla 1.1.10 is a product of Lussumo. More Information: Documentation, Community Support.
As announced here, this entry Knizhnik-Zamolodchikov-Kontsevich construction – definition is meant to contain the definition of the Knizhnik-Zamolodchikov connection, and the statement that the Kontsevich integral on braids is the Dyson formula for its holonomy – and nothing else, to be !include
-ed into the relevant entries
only now noticed that a spurious copy of the entry pp-wave spacetime existed, with plural title – am removing it hereby
brief category:people
-entry for hyperlinking references at Kontsevich integral and Knizhnik-Zamolodchikov connection
I have edited fibration
promted by an email question I have added more information on when the pullback of a fibration is a homotopy pullback;
in the discussion of “transport” in topological spaces I added a pointer to Flat ∞-parallel transport in Top which gives details;
I fixed a mistake where quasifibration was mentioned and pointed to, but, fibration in the Joyal model structure was meant (despite the previous warning of exactly this trap…)
I added a subsection “Related concepts”
I added loads and loads of hyperlinks to the keywords.
FInally, I noticed that the following old discussion was sitting there, which hereby I move fromthere to here
begin forwarded discussion
+–{.query} Tim: I do not quite agree with ’transport’ as being the main point of fibrations. Rather ’lifting’ is the main point, in particular lifting of homotopies, at least in topological situations. For transport, one needs connections of some sort to get things working well, but in many cases there is only a very weak notion of action, so perhaps that should be derived as a property rather than taken as a ’defining property’ in some sense.
Perhaps a reference to Stasheff and Wirth
James Wirth & Jim Stasheff
Homotopy Transition Cocycles
math.AT/0609220.
and the discussion
http://golem.ph.utexas.edu/category/2006/09/wirth_and_stasheff_on_homotopy.html
on the cafe would be a good idea to add.
Urs: In situations where one wants to talk of transport, the fibration usually arises as the pullback of some “universal fibration”, a generalized universal bundle. For instance (split op-)fibrations of categories are precisely the pullbacks of the universal -bundle along a functor .
If one looks at this kind of situation where we do have an established notion of (parallel) transport one sees:
For instance, to make this more concrete, consider the category of smooth groupoids (which is a category of fibrant objects), let for any manifold the groupoid be the groupoid of smooth thin-homotopy classes of paths in , let be any Lie group, the corresponding one-object Lie groupoid and consider the _universal fibration _ – the groupoid incarnation of the universal -bundle as described at generalized universal bundle. Then
Theorem: -bundles with connection on are equivalent to functors out of acyclic fibrations over (i.e. smooth anafunctors ). These functors are literally the corresponding “parallel transport”: indeed, evaluated on a path in there is locally a 1-form such that the group element is the traditional parallel transport of that 1-form, .
Now, we can form the fibration which is associated with this parallel transport, namely the pullback
This fibration is what is properly speaking the action groupoid of acting on the fibers of the principal -bundle.
Mike: Can you clarify the distinction between “lifting” and “transport”? In what way does the lifting of a path starting at a point not transport along ? Certainly in geometric situations to get a parallel notion of transport, you need a connection, but I see that as a stronger requirement.
forwarded discussion continued in next entry
added statements of some basic properties to ribbon graph
brief category:people
-entry for hyperlinking references at D=5 supergravity
brief category:people
-entry for hyperlinking references at 3d-3d correspondence
created an entry beable
(Surprisingly, this keyword does not have a Wikipedia entry…)
merging this duplicate with p-adic AdS/CFT correspondence
brief category:people
-entry for hyperlinking references at p-adic AdS/CFT correspondence
Since its creation, the entry étale map started out as wanting to be about the abstraction of the notion of local homeomorphism and étale morphism to more general contexts.
I have added references to such axiomatizations now. But I am not sure that it is good to have “étale map” be interpreted so much differently from “étale morphism”. I think both of these should point to the same page, which discusses the general abstract notion, and then what currently is étale morphism should be renamed to “étale morphism of schemes”.
Finally, I changed the wording of the Idea-section at the beginning of étale map: it used to say that an étale map is like a “local isomorphism”. As we have recently seen in discussion, this is a very misleading thing to say, since it is not like a local isomorphism but like a local homeomorphism. These two concepts, maybe unfortunately termed, are not about the same idea.
brief category:people
-entry for hyperlinking references at Lie algebra weight system, ’t Hooft double line notation and string diagram
brief category:people
-entry for hyperlinking references at Vassiliev invariant and at stringy weight system
brief category:people
-entry for hyperlinking references at holographic QCD and B-meson
Recording Def. 3.11, Theorem 7, Exercise 6.24 from
for hyperlinking references at AKSZ sigma model
brief category:people
-entry for hyperlinking references at Mostow rigidity theorem
added references
The original article:
Review:
Reading over section 5 of her
I thought it worth a reference to
I don’t think we have anything on this refinement.
brief category:people
-entry for hyperlinking references at D=3 N=4 super Yang-Mills theory and D=6 N=(1,0) SCFT
brief category:people
-entry for hyperlinking references at Gromov-Witten/Donaldson-Thomas correspondence
brief category:people
-entry for hyperlinking references at Gromov-Witten/Donaldson-Thomas correspondence
brief category:people
-entry for hyperlinking references at Gromov-Witten/Donaldson-Thomas correspondence
brief category:people
-entry for hyperlinking references at Gromov-Witten/Donaldson-Thomas correspondence
determinant line bundle, Witten index, I commented on some of the motivations for introducing a related series of entries in the last paragraph in comment here. I noticed that we do not have Dirac operator, nor even spin representation. Additional references at quantum anomaly.
recording the statement of Lemma 8.6 in
added pointer on D=3 N=4 super Yang-Mills theories with compact hyperkähler manifold Coulomb branches obtained by KK-compactification of little string theories:
Edit to: intersecting D-brane model by Urs Schreiber at 2018-04-01 00:55:01 UTC.
Author comments:
hyperlinked pointer to textbook by Ibanez-Uranga