Abstract:We present cylindrically symmetric, static solutions of the Einstein field equations around a line singularity such that the energy momentum tensor corresponds to infinitely thin photonic shells. Positivity of the energy density of the thin shell and the line singularity is discussed. It is also shown that thick shells containing mostly radiation are possible in a numerical solution.
“…This is also true for a shell with particles moving only in the axial direction. Similar behavior has been observed for a static cylindrical shell with counter moving photons in z direction [12]. This might be an expected result since for these cases there is no pressure in the fluid against collapse (p φ = 0) and we need an repelling force to keep these shells static.…”
Static cylindrical shells composed of massive particles arising from matching of two different Levi-Civita space-times are studied for the shell satisfying either isotropic or anisotropic equation of state. We find that these solutions satisfy the energy conditions for certain ranges of the parameters.
“…This is also true for a shell with particles moving only in the axial direction. Similar behavior has been observed for a static cylindrical shell with counter moving photons in z direction [12]. This might be an expected result since for these cases there is no pressure in the fluid against collapse (p φ = 0) and we need an repelling force to keep these shells static.…”
Static cylindrical shells composed of massive particles arising from matching of two different Levi-Civita space-times are studied for the shell satisfying either isotropic or anisotropic equation of state. We find that these solutions satisfy the energy conditions for certain ranges of the parameters.
“…Such particle can also follow axial timelike (null) geodesics if the parameters satisfy the inequality (equality) 2σ(2σ − 2 + p) − p + (p 2 + q 2 )/2 > 0(= 0). These are in accordance with four dimensional Levi-Civita solution [8,[60][61][62].…”
Section: Equations Of Motion Of Test Particlessupporting
confidence: 84%
“…Note that if one choses the coordinate x 4 as the radial coordinate and the remaining coordinates as usual cylindrical coordinates in (67) with properly chosen signature, then one obtains the cylindrical static vacuum Levi-Civita solution [8] in its Kasner form. There is a simple transformation between these two different forms of cylindrical vacuum solutions (See for example [26,62]). Actually, Kasner type cosmological [65][66][67] or cylindrical vacuum solutions [26,27] were generalized to higher dimensions.…”
Section: D Dimensional Kasner-type Einstein-maxwell Solutionsmentioning
confidence: 99%
“…In this special case the coordinate r must be extended to include −∞ < r < r 0 . The interesting point of this value of parameters σ = 1/2, p i = 0 is that it is the higher dimensional generalization of four dimensional case where the Levi-Civita metric describes an infinite plane geometry [15,60,62] rather than a cylindrical one. Thus, for this case we have a charged infinite plane at r = r 0 where r in this case should be considered as a Cartesian coordinate.…”
Section: The Singularity Structure and The Range Of Solutionsmentioning
We consider a D dimensional Kasner type diagonal spacetime where metric functions depend only on a single coordinate and electromagnetic field shares the symmetries of spacetime. These solutions can describe static cylindrical or cosmological Einstein-Maxwell vacuum spacetimes. We mainly focus on electrovacuum solutions and four different types of solutions are obtained in which one of them has no four dimensional counterpart. We also consider the properties of the general solution corresponding to the exterior field of a charged line mass and discuss its several properties. Although it resembles the same form with four dimensional one, there is a difference on the range of the solutions for fixed signs of the parameters. General magnetic field vacuum solution are also briefly discussed, which reduces to Bonnor-Melvin magnetic universe for a special choice of the parameters. The Kasner forms of the general solution are also presented for the cylindrical or cosmological cases.
“…For this metric, the parameter d is related to the energy density of the source of the metric and the parameter W 0 is related to the global topology (conicity) of space-time [22][23][24][25] and gains significance in the context of the cosmic strings. In order to find a plausible interpretation for these parameters, several interior concentric cylinders [22][23][24][25][26][27] and thin shells [28][29][30][31][32] have been constructed as the sources for this particular vacuum solution. For d = 0 this metric is identical to that of a straight cosmic string metric [33].…”
We investigate cylindrically symmetric vacuum solutions with both null and non-null electromagnetic fields in the framework of the Brans-Dicke theory and compare these solutions with some of the well-known solutions of general relativity for special values of the parameters of the resulting field functions. We see that, unlike general relativity where the gravitational force of an infinite and charged line mass acting on a test particle is always repulsive, it can be attractive or repulsive for BransDicke theory depending on the values of the parameters as well as the radial distance from the symmetry axis.
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