Super-extremal black holes in the quasitopological electromagnetic field theory (2404.03744v1)
Abstract: It has recently been proved that a simple generalization of electromagnetism, referred to as quasitopological electromagnetic field theory, is characterized by the presence of dyonic black-hole solutions of the Einstein field equations that, in certain parameter regions, are characterized by four horizons. In the present compact paper we reveal the existence, in this non-linear electrodynamic field theory, of super-extremal black-hole spacetimes that are characterized by the four degenerate functional relations $[g_{00}(r)]{r=r{\text{H}}}=[dg_{00}(r)/dr]{r=r{\text{H}}}=[d2g_{00}(r)/dr2]_ {r=r_{\text{H}}}=[d3g_{00}(r)/dr3]{r=r{\text{H}}}=0$, where $g_{00}(r)$ is the $tt$-component of the curved line element and $r_{\text{H}}$ is the black-hole horizon radius. In particular, using analytical techniques we prove that the quartically degenerate super-extremal black holes are characterized by the universal (parameter-{\it independent}) dimensionless compactness parameter $M/r_{\text{H}}={2\over3}(2\gamma+1)$, where $\gamma\equiv{_2F_1}(1/4,1;5/4;-3)$.
- We use natural units in which G=c=ℏ=1𝐺𝑐Planck-constant-over-2-pi1G=c=\hbar=1italic_G = italic_c = roman_ℏ = 1.
- Note that the coupling parameter α1subscript𝛼1\alpha_{1}italic_α start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT is dimensionless whereas the coupling parameter α2subscript𝛼2\alpha_{2}italic_α start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT has the dimensions of length22{}^{2}start_FLOATSUPERSCRIPT 2 end_FLOATSUPERSCRIPT.
Collections
Sign up for free to add this paper to one or more collections.