2015
DOI: 10.1007/s11005-015-0765-y
|View full text |Cite
|
Sign up to set email alerts
|

Homotopy Colimits and Global Observables in Abelian Gauge Theory

Abstract: We study chain complexes of field configurations and observables for Abelian gauge theory on contractible manifolds, and show that they can be extended to non-contractible manifolds by using techniques from homotopy theory. The extension prescription yields functors from a category of manifolds to suitable categories of chain complexes. The extended functors properly describe the global field and observable content of Abelian gauge theory, while the original gauge field configurations and observables on contra… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
24
0

Year Published

2016
2016
2019
2019

Publication Types

Select...
5

Relationship

5
0

Authors

Journals

citations
Cited by 22 publications
(24 citation statements)
references
References 48 publications
0
24
0
Order By: Relevance
“…Because there are no non‐trivial principal double-struckR‐bundles, the groupoid of gauge fields (cf. Example ) on M is given by truerightBG con (M)0.16em=0.16em{Obj:AnormalΩ1false(Mfalse)Mor:AεA+dεwithεCfalse(Mfalse).Following, one easily computes the nerve of this groupoid and, after applying the Dold‐Kan correspondence to the resulting simplicial vector space, obtains the chain complex F=(normalΩ1false(Mfalse)(0)normaldnormalΩ0false(Mfalse)(1)),where we indicated in round brackets the homological degrees and identified functions with 0‐forms normalΩ0false(Mfalse)=Cfalse(Mfalse). As expected, this chain complex has only ‘stacky’ positive degrees and no ‘derived’ negative degrees.…”
Section: Higher Structures In Gauge Theorymentioning
confidence: 99%
See 2 more Smart Citations
“…Because there are no non‐trivial principal double-struckR‐bundles, the groupoid of gauge fields (cf. Example ) on M is given by truerightBG con (M)0.16em=0.16em{Obj:AnormalΩ1false(Mfalse)Mor:AεA+dεwithεCfalse(Mfalse).Following, one easily computes the nerve of this groupoid and, after applying the Dold‐Kan correspondence to the resulting simplicial vector space, obtains the chain complex F=(normalΩ1false(Mfalse)(0)normaldnormalΩ0false(Mfalse)(1)),where we indicated in round brackets the homological degrees and identified functions with 0‐forms normalΩ0false(Mfalse)=Cfalse(Mfalse). As expected, this chain complex has only ‘stacky’ positive degrees and no ‘derived’ negative degrees.…”
Section: Higher Structures In Gauge Theorymentioning
confidence: 99%
“…Following, [51] one easily computes the nerve of this groupoid and, after applying the Dold-Kan correspondence to the resulting simplicial vector space, obtains the chain complex…”
Section: Derived Geometry Of Linear Gauge Fieldsmentioning
confidence: 99%
See 1 more Smart Citation
“…Another advantage of our synthetic approach to classical field theory is that it is a suitable starting point for generalizations to gauge theories. In particular, the groupoids of gauge field configurations appearing in our recently proposed homotopy theoretic approach to gauge theories [BSS15] can be easily promoted to groupoid objects in the Cahiers topos, i.e. "generalized smooth groupoids".…”
Section: Introductionmentioning
confidence: 99%
“…"generalized smooth groupoids". The relevant homotopy theoretical concepts used in [BSS15] generalize to such "generalized smooth groupoids" [JT91], while locally-convex Lie groupoids (which arise in the framework of [BFR12]) are not suitable for homotopy theory.…”
Section: Introductionmentioning
confidence: 99%