Search arXiv⌕ Search

arXiv · gr-qc/9511021

Solutions Stationnaires en Théorie de Kaluza-Klein

Abstract

Kaluza-Klein theory is a 5-dimensional Einstein general relativity; it has the interest of describing on an equal footing the laws of gravitation and electromagnetism in a geometrically unified way. We present it in Chapter 1, and we generalize it by adding to the equations of the theory the Lanczos tensor (endowed with the same physical properties as the Einstein tensor but quadratic with respect to the Riemann tensor.) One has obtained in the last decade all the spherically symmetric 2-stationary solutions (independent of time and of the extra coordinate) of the ``special" Kaluza-Klein theory. The study of the stability of these solutions against radial excitations is carried out in Chapter 2. We begin by presenting the spherically symmetric 2-static solutions; then we write and separate the perturbation-linearized equations of the 5-metric. The problem of stability against small oscillations is reduced to an eigenvalue problem which we discuss in detail in the static-solution parameter space. We show that regular solutions of non-vanishing finite energy (Kaluza-Klein solitons) --with non-euclidean spatial topology-- are stable. A broad class of singular solutions, containing among others the Schwarzschild solution, are also stable. Finally our stability results are compared to those obtained previously by Tomimatsu for a less broad class of solutions. We search in Chapter 3 for other exact stationary solutions, endowed this time with cylindrical symmetry, thus actually 4-stationary (depending on only one spacelike coordinate). First we obtain by a systematic study all the 4-stationary solutions of the special theory, some of which are interpreted as neutral or charged distributional cosmic string sources. We generalize these solutions in a following section by considering the Lanczos tensor, and we find

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Mustapha Azreg-Ainou. 1995-12-21. Solutions Stationnaires en Théorie de Kaluza-Klein. https://arxiv.org/abs/gr-qc/9511021

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

An upper bound on the minimum orbital period of black holes

Previous research has focused on establishing lower bounds on the minimum orbital period of black holes. In this work, we explore the complementary question of whether an upper bound exists for the minimum orbital period of black holes. We investigate the minimum orbital periods of three types of black holes: Schwarzschild, Reissner-Nordström and Kerr-Newman black holes. We find that the minimum orbital period of these black holes is bounded by an upper limit $T_{min} \leqslant 6\sqrt{3}πM$, where $M$ is the black hole mass. Our results suggest that this upper bound on the minimum orbital period may be a general property in black hole spacetimes.

gr-qc↗

Bounds on the minimum orbital period in the background of 5-dimensional charged black holes

In this paper, we study the upper and lower bounds on the minimum orbital period of 5-dimensional charged black holes. Our results indicate that the upper bound of the minimum orbital period corresponds to non-charged black holes, while the lower bound is achieved in the case of maximally charged black holes. We further establish precise analytical expressions for the upper and lower bounds of the minimum orbital period. Our findings provide valuable insights into 5-dimensional charged black holes and help constrain theoretical gravity models.

gr-qc↗

Analysis of minimum orbital periods around d-dimensional charged black holes

This paper investigates the bounds on the minimum orbital period for test objects around d-dimensional charged black holes in asymptotically flat spacetimes. We derive the exact critical radius and the minimum orbital period. We then prove analytically that the minimum orbital period decreases strictly as the charge of the black hole increases. Thus, the upper limit is reached for an uncharged black hole, while the lower limit is attained for a maximally charged one, and the two bounds take the closed form $\frac{2π(d-2)}{d-3}[(d-2)M]^{\frac{1}{d-3}}\leqslant T_{min} \leqslant 2π\sqrt{\frac{d-1}{d-3}}\,[(d-1)M]^{\frac{1}{d-3}}$. Since the minimum period equals $2π$ times the shadow radius, the upper bound is equivalently a universal upper bound on the shadow radius. These results improve our understanding of dynamics around d-dimensional black holes and impose constraints on candidate gravity theories.

gr-qc↗