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Amplitudes' Positivity, Weak Gravity Conjecture, and Modified Gravity

Brando Bellazzini, Matthew Lewandowski, Javi Serra

TL;DR

The paper develops IR-safe positivity bounds for 4D theories containing a massless graviton by regulating the forward limit with a 3D cylinder compactification, subtracting gravity-induced KK and zero-mode effects to obtain a finite, positive dispersion relation for the $s^2$ coefficient of elastic amplitudes. Applied to the Einstein-Maxwell EFT, the bounds constrain higher-derivative operators $\alpha_i$, yielding $2\alpha_1-\alpha_3>0$, $2\alpha_1+\alpha_3>0$, and $\alpha_2>0$, which in turn modify extremality conditions and imply a mild form of the weak gravity conjecture: extremal black holes are self-repulsive and can decay to smaller extremal holes. The authors extend the analysis to scalars, axions, $P(X)$ theories, galileons, and curved spacetimes, finding that positivity bounds impose nontrivial UV-consistency constraints such as $\Lambda_{UV}\lesssim\mathrm{few}\times (H^3 m_{Pl})^{1/4}$ and that similar bounds can persist in de Sitter or anti-de Sitter backgrounds. Overall, the work connects fundamental S-matrix principles to concrete EFT constraints and black-hole physics, informing swampland considerations and guiding UV completion of gravity-coupled EFTs.

Abstract

We derive new positivity bounds for scattering amplitudes in theories with a massless graviton in the spectrum in four spacetime dimensions, of relevance for the weak gravity conjecture and modified gravity theories. The bounds imply that extremal black holes are self-repulsive, $M/|Q|<1$ in suitable units, and that they are unstable to decay to smaller extremal black holes, providing an S-matrix proof of the weak gravity conjecture. We also present other applications of our bounds to the effective field theory of axions, $P(X)$ theories, weakly broken galileons, and curved spacetimes.

Amplitudes' Positivity, Weak Gravity Conjecture, and Modified Gravity

TL;DR

The paper develops IR-safe positivity bounds for 4D theories containing a massless graviton by regulating the forward limit with a 3D cylinder compactification, subtracting gravity-induced KK and zero-mode effects to obtain a finite, positive dispersion relation for the coefficient of elastic amplitudes. Applied to the Einstein-Maxwell EFT, the bounds constrain higher-derivative operators , yielding , , and , which in turn modify extremality conditions and imply a mild form of the weak gravity conjecture: extremal black holes are self-repulsive and can decay to smaller extremal holes. The authors extend the analysis to scalars, axions, theories, galileons, and curved spacetimes, finding that positivity bounds impose nontrivial UV-consistency constraints such as and that similar bounds can persist in de Sitter or anti-de Sitter backgrounds. Overall, the work connects fundamental S-matrix principles to concrete EFT constraints and black-hole physics, informing swampland considerations and guiding UV completion of gravity-coupled EFTs.

Abstract

We derive new positivity bounds for scattering amplitudes in theories with a massless graviton in the spectrum in four spacetime dimensions, of relevance for the weak gravity conjecture and modified gravity theories. The bounds imply that extremal black holes are self-repulsive, in suitable units, and that they are unstable to decay to smaller extremal black holes, providing an S-matrix proof of the weak gravity conjecture. We also present other applications of our bounds to the effective field theory of axions, theories, weakly broken galileons, and curved spacetimes.

Paper Structure

This paper contains 10 sections, 48 equations, 2 figures.

Figures (2)

  • Figure 1: Positivity bounds (\ref{['Eq:positivityEM1']}, \ref{['Eq:positivityEM2']}) require $\alpha_1$ and $\alpha_3$ to live inside the the smaller green wedge. The blue striped region is where extremal black holes are self-repulsive, $|Q|>M/(\sqrt{2} m_{\mathrm{Pl}})$.
  • Figure 2: Complex $s$-plane and singularity structure in the 4D theory compactified to 3D. The (double) arcs upon which the forward amplitude is integrated, see (\ref{['arcs']}), are also depicted.