Static multipolar Einstein-vector-Gauss-Bonnet black holes
Abstract
We construct and analyze static multipolar black holes in Einstein-vector-Gauss-Bonnet theory with a quadratic coupling function. The vectorized solutions bifurcate from the Schwarzschild black hole at discrete values of the Gauss-Bonnet coupling, obtained from a perturbative eigenvalue problem on the Schwarzschild background and labelled by the angular multipole number ℓ. We restrict to the fundamental radial branches. The electric sector contains the known spherically symmetric ℓ = 0 branch as well as axisymmetric branches with ℓ > 0. These electric branches extend to larger values of the coupling. The magnetic sector features a sequence of axisymmetric branches, including the previously found magnetic dipole branch at ℓ = 0 . The magnetic branches instead exist only on finite intervals of the coupling, ending at critical solutions. Away from the bifurcation point, nonlinearities generate additional multipoles, but even-ℓ and odd-ℓ moments remain separated.
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BibTeX
@article{kleihaus2026static,
title = {{Static multipolar Einstein-vector-Gauss-Bonnet black holes}},
author = {Burkhard Kleihaus and Jutta Kunz},
journal = {Physics Letters B},
year = {2026},
month = oct,
doi = {10.1016/j.physletb.2026.141089},
url = {https://linkinghub.elsevier.com/retrieve/pii/S0370269326009391},
note = {CC BY 4.0},
}
RIS
TY - JOUR
TI - Static multipolar Einstein-vector-Gauss-Bonnet black holes
AU - Burkhard Kleihaus
AU - Jutta Kunz
PY - 2026
DA - 2026/10/30
JO - Physics Letters B
DO - 10.1016/j.physletb.2026.141089
UR - https://linkinghub.elsevier.com/retrieve/pii/S0370269326009391
AB - We construct and analyze static multipolar black holes in Einstein-vector-Gauss-Bonnet theory with a quadratic coupling function. The vectorized solutions bifurcate from the Schwarzschild black hole at discrete values of the Gauss-Bonnet coupling, obtained from a perturbative eigenvalue problem on the Schwarzschild background and labelled by the angular multipole number ℓ. We restrict to the fundamental radial branches. The electric sector contains the known spherically symmetric ℓ = 0 branch as well as axisymmetric branches with ℓ > 0. These electric branches extend to larger values of the coupling. The magnetic sector features a sequence of axisymmetric branches, including the previously found magnetic dipole branch at ℓ = 0 . The magnetic branches instead exist only on finite intervals of the coupling, ending at critical solutions. Away from the bifurcation point, nonlinearities generate additional multipoles, but even-ℓ and odd-ℓ moments remain separated.
SN - 0370-2693
SN - 1873-2445
ER -