4.6 Article

Deflection angle with electromagnetic interaction and gravitational-electromagnetic dual lensing

Journal

Publisher

IOP Publishing Ltd
DOI: 10.1088/1475-7516/2021/08/022

Keywords

gravitational lensing; GR black holes; gravity

Funding

  1. NNSF China [11504276]
  2. MOST China [2014GB109004]

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This study examines the trajectory deflection and gravitational-electromagnetic dual lensing of charged signals in general charged static and spherically symmetric spacetimes. The electromagnetic corrections affect the apparent angles, magnifications, and time delay of the images, with the sign and relative size of the corrections determined by the mass, charge, signal particle charge, and energy. The results have implications for the deflection and lensing of charged particles in various charged spacetimes.
The trajectory deflection and gravitational-electromagnetic dual lensing (GEL) of charged signal in general charged static and spherically symmetric spacetimes are considered in this work. We show that the perturbative approach previously developed for neutral particles can be extended to the electromagnetic interaction case. The deflection angle still takes a (quasi-)series form and the finite distance effect of both the source and observer can be taken into account. Comparing to pure gravitational case, the apparent angles of the images in the GEL, their magnifications and time delay all receive the electromagnetic corrections starting from the first non-trivial order. The sign and relative size of the leading corrections are determined by similar to Q/M q/E where M, Q, q, E are the spacetime mass and charge, and signal particle charge and energy respectively. It is found that for qQ > 0 (or < 0), the electromagnetic interaction will decrease (or increase) the deflection angle, and in GEL the impact parameters, apparent angles, magnifications and total travel time for each image. The time delay is increased for small beta and qQ > 0, and otherwise always increased regardless the sign of qQ. The results are then applied to the deflection and GEL of charged protons in cosmic rays in Reissner-Nordstrom, charged dilaton and charged Horndeski spacetimes.

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