The meaning of time and covariant superderivatives in supermechanics (Q606111)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: The meaning of time and covariant superderivatives in supermechanics |
scientific article; zbMATH DE number 5816348
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | The meaning of time and covariant superderivatives in supermechanics |
scientific article; zbMATH DE number 5816348 |
Statements
The meaning of time and covariant superderivatives in supermechanics (English)
0 references
16 November 2010
0 references
Summary: We present a review of the basics of supermanifold theory (in the sense of Berezin-Kostant-Leites-Manin) from a physicist's point of view. By considering a detailed example of what does it mean the expression ``to integrate an ordinary superdifferential equation'' we show how the appearance of anticommuting parameters playing the role of time is very natural in this context. We conclude that in dynamical theories formulated whithin the category of supermanifolds, the space that classically parametrizes time (the real line \(\mathbb R\)) must be replaced by the simplest linear supermanifold \(\mathbb R^{1|1}\). This supermanifold admits several different Lie supergroup structures, and we analyze from a group-theoretic point of view what is the meaning of the usual covariant superderivatives, relating them to a change in the underlying group law. This result is extended to the case of \(N\)-supersymmetry.
0 references
0 references
0.8574866
0 references
0.85257125
0 references
0 references
0.84573674
0 references
0.84526193
0 references
0.8436625
0 references
0.8348664
0 references
0.8340907
0 references