Analytic bounds on the spectrum of crossing symmetric S-matrices

A bstract We derive two rigorous bounds on the spectrum of massive states that contributes to planar amplitudes in weakly coupled theories with massless scalars. First, we show that the presence of massive spinning states necessitates the existence of lighter states with lower spins. Explicitly, if there exists a massive state with spin J > 2, then there must be a state with spin J − 1 and a non-zero mass lower than that of the lightest spin- J state, a state with spin J − 2 and a mass lower than that of the lightest spin-( J − 1) particle and so on until we reach a mass below which only states with spin less than 2 are exchanged. Second, we find that if there are spin- J states in the spectrum, the maximum mass of the lightest spin-( J + 1) state is determined by the masses of the lightest spin- J and ( J − 1) states. In the approximation that this bound applies to pion scattering in real world QCD, we find it gives a window of only ∼150 MeV for the expected mass of a yet unmeasured spin-7 meson.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-08-08
DOI
https://doi.org/10.1007/jhep08(2025)066
Citations
3
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
5.61

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article

Analytic bounds on the spectrum of crossing symmetric S-matrices

J D Berman
3 citations
Journal of High Energy Physics
Quantum Chromodynamics and Particle Interactions
5.61
article

Analytic bounds on the spectrum of crossing symmetric S-matrices

J D Berman
article en
3 citations

Abstract

A bstract We derive two rigorous bounds on the spectrum of massive states that contributes to planar amplitudes in weakly coupled theories with massless scalars. First, we show that the presence of massive spinning states necessitates the existence of lighter states with lower spins. Explicitly, if there exists a massive state with spin J > 2, then there must be a state with spin J − 1 and a non-zero mass lower than that of the lightest spin- J state, a state with spin J − 2 and a mass lower than that of the lightest spin-( J − 1) particle and so on until we reach a mass below which only states with spin less than 2 are exchanged. Second, we find that if there are spin- J states in the spectrum, the maximum mass of the lightest spin-( J + 1) state is determined by the masses of the lightest spin- J and ( J − 1) states. In the approximation that this bound applies to pion scattering in real world QCD, we find it gives a window of only ∼150 MeV for the expected mass of a yet unmeasured spin-7 meson.

Journal of High Energy PhysicsVol. 2025(8)
University of Michigan (US)
Research Corporation for Science Advancement, University of Michigan
Sustainable cities and communities
Openalex Percentile: Top 5%
Quantum Chromodynamics and Particle Interactions
5.61
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