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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.

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arXiv ID2602.00349 (version 2)
Pith IDC3E46FZV, Pith's permanent record of this paper and its review
CitationLucas de Souza, Sergio Barbosa, Sylvain Fichet. "Running Love Numbers of Charged Black Holes." arXiv:2602.00349 (2026). https://pith.science/paper/C3E46FZV
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What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.21 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.10 · compares with prior results 0.18 · mentions code or data availability 0.03.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

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

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
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 kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.93.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

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.

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References
How the literature uses it

4 arXiv papers cite this in 8 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

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
Uses the method or tool of 2 papers
Compares with 3 papers
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

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