RECORD
Running Love Numbers of Charged Black Holes
High Energy Physics - Theory · Submitted 30 Jan 2026 · Published version
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The overall picture that emerges is that the QFT-induced tidal response of magnetic black holes saturates in the strong-field regime.
The compiled record
The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
Open the compiled record
The abstract, sentence by sentence
Loops of virtual particles from the vacuum of quantum field theory (QFT) render black holes tidally deformable. We compute the static tidal response of unspinning charged black holes at arbitrary radius, using the perturbative formalism developed in 2501.18684. Since the gravitational and electromagnetic tidal responses mix, we generalize the notion of Love numbers to Love matrices. We derive the coupled equations of motion for the metric and electromagnetic fluctuations around purely electric and magnetic backgrounds. For large charged black holes, which are described by the Effective Field Theory (EFT) of gravity, we compute the full set of Love matrices induced by an arbitrary tower of $F^{2n}$ operators. We find that, although quantum corrections break electromagnetic duality, the Love matrices in electric and magnetic backgrounds are related by a $Z_2$ symmetry under electric-magnetic exchange. Going beyond EFT, we compute the Love matrices of small magnetic black holes. We show that the running of the Love matrices is governed by the running of the $U(1)$ gauge coupling, and we derive the correspondence between Love and $U(1)$ beta functions for arbitrary harmonics. The overall picture that emerges is that the QFT-induced tidal response of magnetic black holes saturates in the strong-field regime. These results imply that nearly-extremal magnetic black holes charged under an Abelian dark sector could be probed by gravitational-wave observations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Loops of virtual particles from the vacuum of quantum field theory (QFT) render black holes tidally deformable. | background 1.00 | 0.08 | 0.05 | asserted 1.00 |
| s1 | We compute the static tidal response of unspinning charged black holes at arbitrary radius, using the perturbative formalism developed in 2501.18684. | contribution 0.63 | 0.96 | 0.04 | asserted 0.99 |
| s2 | Since the gravitational and electromagnetic tidal responses mix, we generalize the notion of Love numbers to Love matrices. | contribution 0.70 | 0.90 | 0.06 | asserted 0.98 |
| s3 | We derive the coupled equations of motion for the metric and electromagnetic fluctuations around purely electric and magnetic backgrounds. | method 0.78 | 0.95 | 0.03 | asserted 0.99 |
| s4 | For large charged black holes, which are described by the Effective Field Theory (EFT) of gravity, we compute the full set of Love matrices induced by an arbitrary tower of $F^{2n}$ operators. | contribution 0.95 | 0.96 | 0.10 | asserted 1.00 |
| s5 | We find that, although quantum corrections break electromagnetic duality, the Love matrices in electric and magnetic backgrounds are related by a $Z_2$ symmetry under electric-magnetic exchange. | result 1.00 | 0.95 | 0.13 | asserted 1.00 |
| s6 | Going beyond EFT, we compute the Love matrices of small magnetic black holes. | contribution 0.99 | 0.96 | 0.05 | asserted 1.00 |
| s7 | We show that the running of the Love matrices is governed by the running of the $U(1)$ gauge coupling, and we derive the correspondence between Love and $U(1)$ beta functions for arbitrary harmonics. | result 0.97 | 0.96 | 0.30 | asserted 1.00 |
| s8 | The overall picture that emerges is that the QFT-induced tidal response of magnetic black holes saturates in the strong-field regime. | result 0.77 | 0.84 | 0.36 | asserted 0.99 |
| s9 | These results imply that nearly-extremal magnetic black holes charged under an Abelian dark sector could be probed by gravitational-wave observations. | interpretation 1.00 | 0.57 | 0.38 | hedged possibility 0.99 |
What was examined, and what was not
- arXiv listing abstract v2
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
The paper
Original abstract
Loops of virtual particles from the vacuum of quantum field theory (QFT) render black holes tidally deformable. We compute the static tidal response of unspinning charged black holes at arbitrary radius, using the perturbative formalism developed in 2501.18684. Since the gravitational and electromagnetic tidal responses mix, we generalize the notion of Love numbers to Love matrices. We derive the coupled equations of motion for the metric and electromagnetic fluctuations around purely electric and magnetic backgrounds. For large charged black holes, which are described by the Effective Field Theory (EFT) of gravity, we compute the full set of Love matrices induced by an arbitrary tower of $F^{2n}$ operators. We find that, although quantum corrections break electromagnetic duality, the Love matrices in electric and magnetic backgrounds are related by a $Z_2$ symmetry under electric-magnetic exchange. Going beyond EFT, we compute the Love matrices of small magnetic black holes. We show that the running of the Love matrices is governed by the running of the $U(1)$ gauge coupling, and we derive the correspondence between Love and $U(1)$ beta functions for arbitrary harmonics. The overall picture that emerges is that the QFT-induced tidal response of magnetic black holes saturates in the strong-field regime. These results imply that nearly-extremal magnetic black holes charged under an Abelian dark sector could be probed by gravitational-wave observations.
Human review
References
How the literature uses it
4 arXiv papers cite this in 8 sentences
Papers citing it · 6 sentences without a confident label
Cites it as background 2 papers
-
Additional developments encompass finite-frequency effects [ref] , more general black hole backgrounds [ref] – most notably rotating (Kerr) black holes [ref] – as well as nonlinear tidal response coefficients [ref] .[For a comprehensive overview spanning both recent and past publications, see [ref] .]
Tidal Response and Thermodynamics of Black Holes · Introduction · 0.85
-
They have by now been found for time-dependent (dynamical) tides [ref] , in higher dimensions [ref] , in AdS backgrounds [ref] , for magnetically charged black holes [ref] , in modified gravity and for exotic compact objects [ref] , and in quantum-corrected spacetimes [ref] .
Extremal non-rotating black holes have no fermionic Love · Introduction · 0.85
What it cites · 115 sentences without a confident label
Builds on 2 papers
-
We review the analysis of [ref] and extend it to multiple tides.
Running Love Numbers and the Effective Field Theory of Gravity · Structure and Properties · 0.97
-
This section extends the analysis made in [ref] .
2503.20910 · Black Hole Properties from Dimensional Analysis · 1.00
Uses the method or tool of 2 papers
-
We compute the static tidal response of unspinning charged black holes at arbitrary radius, using the perturbative formalism developed in [ref] .
Running Love Numbers and the Effective Field Theory of Gravity · Introduction · 0.86
-
We decompose the $a_μ$ and $h_μν$ fluctuations into vector and tensor spherical harmonics on the two-sphere [ref] (see also [ref] ).
Static response and Love numbers of Schwarzschild black holes · Spherical Harmonics and Parity · 0.90
Compares with 3 papers
-
Consistently, the equation for $Ψ_h$ in the neutral limit reproduces the one from the Regge–Wheeler variable, (6.52) of [ref] .]
Running Love Numbers and the Effective Field Theory of Gravity · The Fluctuations of Electrically-Charged Black Holes · 0.90
-
Therefore, the transformed form of Eq. [ref] reads [equation] This result agrees with [ref] upon translating the conventions.
Love numbers and magnetic susceptibility of charged black holes · Leading-Order · 0.99
-
Therefore, the transformed form of Eq. [ref] reads [equation] This result agrees with [ref] upon translating the conventions.
Master equations for perturbations of generalised static black holes with charge in higher dimensions · Leading-Order · 0.99
Cites as support 1 paper
-
Therefore, extremal black holes of any size are dominated by the electromagnetic sector [ref] .
2503.20910 · Extremal Black Holes and Weak Gravity Conjecture · 0.96
Cites as background 69 papers
-
A general perturbative formula for the Love beta functions is derived in [ref] , and general considerations along these lines are also presented in [ref] .
Running Love Numbers and the Effective Field Theory of Gravity · Review: Black Holes as Point Particles · 0.80
-
A general perturbative formula for the Love beta functions is derived in [ref] , and general considerations along these lines are also presented in [ref] .
On the logarithmic Love number of black holes beyond general relativity · Review: Black Holes as Point Particles · 0.80
-
[The leading curvature corrections to neutral and charged black holes have been computed in [ref] . ] We consider purely electric or purely magnetic black holes, so that the invariant $F_μνF^μν$ vanishes.
Higher-order corrections to mass-charge relation of extremal black holes · Deformed Geometry in Weak-Field Regime · 0.84
Discussion
Know something about this paper? Leave a comment, or highlight any passage above to comment on it.