dc.contributor.author |
Bronnikov K. |
|
dc.contributor.author |
Chervon S. |
|
dc.contributor.author |
Sushkov S. |
|
dc.date.accessioned |
2018-09-18T20:07:04Z |
|
dc.date.available |
2018-09-18T20:07:04Z |
|
dc.date.issued |
2009 |
|
dc.identifier.issn |
0202-2893 |
|
dc.identifier.uri |
https://dspace.kpfu.ru/xmlui/handle/net/136663 |
|
dc.description.abstract |
We consider static, spherically symmetric solutions of general relativity with a non-linear sigma model (NSM) as a source, i.e., a set of scalar fields Φ = (Φ 1,...,Φ n) (so-called chiral fields) parametrizing a target space with a metric h ab(Φ). For NSM with zero potential V (Φ), it is shown that the space-time geometry is the same as with a single scalar field but depends on h ab. If the matrix h ab is positive-definite, we obtain the Fisher metric, originally found for a canonical scalar field with positive kinetic energy; otherwise we obtain metrics corresponding to a phantom scalar field, including singular and nonsingular horizons (of infinite area) and wormholes. In particular, the Schwarzschild metric can correspond to a nontrivial chiral field configuration, which in this case has zero stress-energy. Some explicit examples of chiral field configurations are considered. Some qualitative properties of NSM configurations with nonzero potentials are pointed out. © Pleiades Publishing, Ltd., 2009. |
|
dc.relation.ispartofseries |
Gravitation and Cosmology |
|
dc.title |
Wormholes supported by chiral fields |
|
dc.type |
Article |
|
dc.relation.ispartofseries-issue |
3 |
|
dc.relation.ispartofseries-volume |
15 |
|
dc.collection |
Публикации сотрудников КФУ |
|
dc.relation.startpage |
241 |
|
dc.source.id |
SCOPUS02022893-2009-15-3-SID71449083347 |
|