Quantum Field Theory and Noncommutative Geometry
DOI: 10.1007/11342786_8
|View full text |Cite
|
Sign up to set email alerts
|

Morita Equivalence, Picard Groupoids and Noncommutative Field Theories

Abstract: In this article we review recent developments on Morita equivalence of star products and their Picard groups. We point out the relations between noncommutative field theories and deformed vector bundles which give the Morita equivalence bimodules.Comment: Latex2e, 10 pages. Conference Proceeding for the Sendai Meeting 2002. Some typos fixe

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
9
0

Publication Types

Select...
4
2

Relationship

0
6

Authors

Journals

citations
Cited by 6 publications
(9 citation statements)
references
References 36 publications
0
9
0
Order By: Relevance
“…Deformation quantization of vector bundles p : E −→ M is already established and can be put down to deformation quantization of finitely generated projective modules, since the sections Γ ∞ (E) are such a right module over C ∞ (M ). The well-known definitions and results can all be found in [13] and [43]. Altogether, one considers the deformed bimodule (6.1)…”
Section: Associated Vector Bundlesmentioning
confidence: 99%
See 1 more Smart Citation
“…Deformation quantization of vector bundles p : E −→ M is already established and can be put down to deformation quantization of finitely generated projective modules, since the sections Γ ∞ (E) are such a right module over C ∞ (M ). The well-known definitions and results can all be found in [13] and [43]. Altogether, one considers the deformed bimodule (6.1)…”
Section: Associated Vector Bundlesmentioning
confidence: 99%
“…where the right module structure itself is defined as a deformation quantization of the vector bundle E. It is known, confer [43], Thm. 1, that for a given star product ⋆ the deformed bimodule structures • ′ E , • and the algebra structure ⋆ ′ E are unique up to equivalence and that the two deformed algebras (Γ ∞ (End(E))[ [λ]], ⋆ ′ E ) and (C ∞ (M )[ [λ]], ⋆) are mutual commutants.…”
Section: Associated Vector Bundlesmentioning
confidence: 99%
“…In this particular case we can of course use the canonical fiber metric coming from the canonical inner product on n . We refer to [34,38] for a further discussion.…”
Section: Matter Fields and Deformed Vector Bundlesmentioning
confidence: 99%
“…We have now the following structure for the collection of all Pic str (·, ·), see [37,Sect. 6.1] and [135,136] …”
Section: The Strong Picard Groupoidmentioning
confidence: 99%