paper

New form of the Kerr-Newman solution

arXiv:2211.10394 · doi:10.1103/PhysRevD.107.L021501

Abstract

A new form of the Kerr-Newman solution is presented. The solution involves a time coordinate which represents the local proper time for a charged massive particle released from rest at spatial infinity. The chosen coordinates ensure that the solution is well-behaved at horizons and enable an intuitive description of many physical phenomena. If the charge of the particle , the coordinates reduce to Doran coordinates for the Kerr solution with the replacement , where and are the mass and charge of the black hole, respectively. Such coordinates are valid only for , however, which corresponds to the region that a neutral particle released from rest at infinity can penetrate. By contrast, for and of opposite sign to , the new coordinates have a progressively extended range of validity as increases and tend to advanced Eddington-Finkelstein (EF) null coordinates as , hence becoming global in this limit. The Kerr solution (i.e.\ with ) may also be written in terms of the new coordinates by setting , where is a real parameter unrelated to charge; in this case the coordinate system is global for all non-negative values of and the limits and correspond to Doran coordinates and advanced EF null coordinates, respectively, without any need to transform between them.

arXiv comment4 pages, no figures, accepted as a Letter by PRD. Contains minor updates to match accepted version

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