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Gravitational form factors in the perturbative limit

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arxiv 2503.11316 v2 pith:5O4QIKJT submitted 2025-03-14 hep-ph hep-lathep-thnucl-exnucl-th

Gravitational form factors in the perturbative limit

classification hep-ph hep-lathep-thnucl-exnucl-th
keywords gammagdasamplitudeslimitperturbativedistributionexperimentsfactors
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Generalized distribution amplitudes (GDAs) have attracted significant attention in recent years due to their connection with the energy-momentum tensor (EMT) form factors (FFs). The GDAs can be experimentally accessed through the study of amplitudes in $\gamma^{\ast} \gamma \to M_1 M_2$ and $\gamma^{\ast} \to M_1 M_2 \gamma$, where $M_1M_2$ is a pseudoscalar meson pair such as $\pi \eta $ and $\eta \eta^{\prime}$. In this work, we calculate these amplitudes in the perturbative limit and express the extracted $M_1M_2$ GDAs in terms of meson distribution amplitudes that have been constrained by the previous experiments. Our explicit calculation verifies the existence of a new EMT FF that violates the conservation law of EMT when the hadronic matrix element of the EMT operator is considered separately for each quark flavor. In addition, our result shows that the $M_1M_2$ GDAs are identical in $\gamma^{\ast} \gamma \to M_1 M_2$ and $\gamma^{\ast} \to M_1 M_2 \gamma$, which confirms the universality of GDAs in the perturbative limit. In the future, the GDAs and the EMT FFs studied in this paper can be probed at Belle II. Our study enhances the accessibility to the $P$-wave GDAs in $\gamma^{\ast} \gamma \to M_1 M_2$ and $\gamma^{\ast} \to M_1 M_2 \gamma$, and provides a promising approach for searching for exotic hybrid mesons in future experiments.

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  1. Particle seismology: mechanical and gravitational properties from parton-hadron duality

    hep-ph 2026-04 unverdicted novelty 2.0

    A hadronic approach based on dispersion relations and meson dominance achieves a successful description of lattice QCD data for gravitational form factors of pions and nucleons.