Higgs pseudo-observables in e+e-→ hγ
Abstract
We analyse the process e+e-→ hγ in the Standard Model (SM) and in generic extensions with heavy new physics, using the framework of Higgs pseudo-observables. We decompose the one-loop amplitude into separately gauge-invariant photon-pole, Z-pole, and non-pole contributions. For heavy new physics, we show that the leading deviations from the SM are necessarily encoded in the hγγ and hZγ on-shell effective couplings. Genuine e+e-hγ contact interactions arise only at higher orders in a derivative expansion, both in SMEFT and HEFT. Although Higgs decays constrain the magnitudes of these pseudo-observables, they leave their relative sign undetermined. Measurements of e+e-→ hγ at different FCC-ee energies can resolve this ambiguity. Deviations incompatible with this description would instead point towards relatively light new degrees of freedom, as illustrated by a simplified Z' model.
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BibTeX
@misc{boniotti2026higgs,
title = {{Higgs pseudo-observables in $e^+e^-\to hγ$}},
author = {Fausto Boniotti and Gino Isidori and Christiane Mayer and Emanuelle Pinsard},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.35981},
eprint = {2609.35981},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.35981},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Higgs pseudo-observables in e^+e^-→ hγ
AU - Fausto Boniotti
AU - Gino Isidori
AU - Christiane Mayer
AU - Emanuelle Pinsard
PY - 2026
DA - 2026/09/28
PB - arXiv
DO - 10.48550/arxiv.2609.35981
UR - https://arxiv.org/abs/2609.35981
AB - We analyse the process e^+e^-→ hγ in the Standard Model (SM) and in generic extensions with heavy new physics, using the framework of Higgs pseudo-observables. We decompose the one-loop amplitude into separately gauge-invariant photon-pole, Z-pole, and non-pole contributions. For heavy new physics, we show that the leading deviations from the SM are necessarily encoded in the hγγ and hZγ on-shell effective couplings. Genuine e^+e^-hγ contact interactions arise only at higher orders in a derivative expansion, both in SMEFT and HEFT. Although Higgs decays constrain the magnitudes of these pseudo-observables, they leave their relative sign undetermined. Measurements of e^+e^-→ hγ at different FCC-ee energies can resolve this ambiguity. Deviations incompatible with this description would instead point towards relatively light new degrees of freedom, as illustrated by a simplified Z' model.
ER -