2006
DOI: 10.1088/0264-9381/23/6/014
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Gravitational field of charged gyratons

Abstract: Abstract. We study relativistic gyratons which carry an electric charge. The Einstein-Maxwell equations in arbitrary dimensions are solved exactly in the case of a charged gyraton propagating in an asymptotically flat metric.

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Cited by 34 publications
(40 citation statements)
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“…A complementary generalisation of pp-waves (13) was considered by Bonnor ([Bon70]) and independently by Frolov and his collaborators in [FF05,FIZ05,FZ06,YZF07]. Here the ndimensional transverse space N is considered to remain flat but non-trivial off-diagonal terms A i (x, u) are allowed to obtain gyratonic pp-waves…”
Section: The Spacetime Metricmentioning
confidence: 99%
“…A complementary generalisation of pp-waves (13) was considered by Bonnor ([Bon70]) and independently by Frolov and his collaborators in [FF05,FIZ05,FZ06,YZF07]. Here the ndimensional transverse space N is considered to remain flat but non-trivial off-diagonal terms A i (x, u) are allowed to obtain gyratonic pp-waves…”
Section: The Spacetime Metricmentioning
confidence: 99%
“…Solutions for electrically charged gyratons were obtained in [21]. The gyraton solutions might be used for study the gravitational interaction of ultrarelativistic particles with spin (and charge).…”
Section: Summary and Discussionmentioning
confidence: 99%
“…For the initial conditions given above, the Kinetic energy of the particle increases or decreases after the passage of the wave, according to the sign oḟ ρ 0 , as shown in Figures [10] and [11]. We recall that the dot represents variation with respect to u.…”
Section: H 0 Given By Equation (16)mentioning
confidence: 99%
“…Likewise, ifρ 0 < 0, the particle is initially getting away from the source. As Figures [10] (ρ 0 > 0) and [11] (ρ 0 < 0) indicate, the particle gain or loose energy as it approaches or gets away from the source located around the axis z = 0.…”
Section: H 0 Given By Equation (16)mentioning
confidence: 99%