1968
DOI: 10.1098/rspa.1968.0073
|View full text |Cite
|
Sign up to set email alerts
|

Cylindrically symmetric charged dust distributions in rigid rotation in general relativity

Abstract: The paper presents a family of stationary cylindrically symmetric solutions of the Einstein-Maxwell equations corresponding to a charged dust distribution in rigid rotation. The interesting feature of the solution is that the Lorentz force vanishes everywhere and the ratio of the charge density and mass density may assume arbitrary value. The solutions do not seem to have any classical analogue.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
20
0

Year Published

1983
1983
2014
2014

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 104 publications
(21 citation statements)
references
References 0 publications
0
20
0
Order By: Relevance
“…Remarkably, the answer is in the positive. These spacetimes were discovered by Som and Raychaudhuri in 1968 [11] as a class of solutions of Einstein-Maxwell equations with a charged dust source. These geometries have the same sort of causal pathologies as the Gödel metric, and like the latter, have sources which obey physically reasonable energy conditions.…”
Section: Raychaudhuri-som Geometriesmentioning
confidence: 99%
See 1 more Smart Citation
“…Remarkably, the answer is in the positive. These spacetimes were discovered by Som and Raychaudhuri in 1968 [11] as a class of solutions of Einstein-Maxwell equations with a charged dust source. These geometries have the same sort of causal pathologies as the Gödel metric, and like the latter, have sources which obey physically reasonable energy conditions.…”
Section: Raychaudhuri-som Geometriesmentioning
confidence: 99%
“…The analogy is further strengthened for stationary spacetimes, where not only is there an exact correspondence between different components of the metric and electric and magnetic fields (such that the geodesic equation can be exactly cast in the form of Lorentz force equation), but that given certain special stationary spacetimes, particles in them exhibit interesting phenemonena such as Landau levels and spatial non-commutativity. One such class of spacetimes was discovered by Som and Raychaudhuri and later re-derived using simple matter field configurations of electromagnetic and scalar fields by one of us (JG) and A. Das [11,12]. We will refer to them as SR spacetimes.…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, we have 27) which depend now on the three dimensionless parameters c 1 , c 2 and c 3 . Using the above variables the metric becomes c 2 4 ds 2 .…”
Section: Non-vanishing Cmentioning
confidence: 99%
“…As homogeneous space-times, they are of the Bianchi type IX (squashed S 3 , here as Gödel space), II (Heisenberg group) and VIII (elliptically squashed AdS 3 ). The second space is also known as Som-Raychaudhuri [27].…”
Section: Jhep04(2014)136mentioning
confidence: 99%
“…Owing to its striking properties, the cosmological solution presented by Gödel has a well-recognized importance and has to a large extent motivated the investigations on rotating cosmological space-times within the framework of general relativity. Particularly, the search for rotating Gödel-type space-times has received a good deal of attention in recent years, and the literature on these geometries is fairly large today see [21] - [34] and references therein).…”
Section: Introductionmentioning
confidence: 99%