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Charged particle motion and electromagnetic field in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>γ</mml:mi></mml:mrow></mml:math> spacetime

Carlos A. Benavides-GallegoCenter for Field Theory and Particle Physics and Department of Physics, Fudan University, 200438 Shanghai, ChinaAhmadjon AbdujabbarovCenter for Field Theory and Particle Physics and Department of Physics, Fudan University, 200438 Shanghai, ChinaDaniele MalafarinaDepartment of Physics, Nazarbayev University, 53 Kabanbay Batyr Avenue, 010000 Astana, KazakhstanBobomurat AhmedovUlugh Beg Astronomical Institute, Astronomicheskaya 33, Tashkent 100052, UzbekistanCosimo BambiCenter for Field Theory and Particle Physics and Department of Physics, Fudan University, 200438 Shanghai, China
ABI

Аннотация

We consider the electromagnetic field occurring in the background of a static, axially symmetric vacuum solution of Einstein's field equations immersed in an external magnetic field. The solution, known as the $\ensuremath{\gamma}$ metric (or Zipoy-Voorhees), is related to the Schwarzschild spacetime through a real positive parameter $\ensuremath{\gamma}$ that describes its departure from spherical symmetry. We study the motion of charged and uncharged particles in this spacetime and particle collision in the vicinity of the singular surface and compare with the corresponding result for Schwarzschild. We show that there is a sharp contrast with the black hole case; in particular, in the prolate case ($\ensuremath{\gamma}&lt;1$) particle collision can occur with an arbitrarily high center of mass energy. This mechanism could in principle allow one to distinguish such a source from a black hole.

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