On-shell renormalization of dim-8 SMEFT from complete amplitude basis. Part I. Four-fermion operators

A bstract We compute the complete one-loop renormalization group equations (RGEs) for all the four-fermion operators at dimension-8 Standard Model Effective Field Theory (SMEFT). We adopt the on-shell framework, where the RGEs are obtained from the unitarity cuts of the bubble integrals. To construct a consistent set of RGEs without redundancy, we utilize the Young Tensor amplitude/operator basis [1] as the building blocks of the tree-level amplitudes that constitute the unitarity cuts, which incorporates the full flavor structures of the effective operators. Due to the large number of effective operators for a dimension-8 type, it is crucial to reduce the integrated cuts to the same RGE amplitude basis, which is also made possible by the algorithm in the Young Tensor method. With the Mathematica package ABC4EFT that implements the method, we obtain the full result of the dimension-8 four-fermion RGEs with the output file attached as the supplementary material.

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Publication Details

Journal
Journal of High Energy Physics
Published
2026-08-27
DOI
https://doi.org/10.1007/jhep08(2026)225
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
0.00

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article

On-shell renormalization of dim-8 SMEFT from complete amplitude basis. Part I. Four-fermion operators

Jiang-Hao Yu, Chao Wu, Ming-Lei Xiao, Yu-Hui Zheng
Journal of High Energy Physics
Quantum Chromodynamics and Particle Interactions
article

On-shell renormalization of dim-8 SMEFT from complete amplitude basis. Part I. Four-fermion operators

Jiang-Hao Yu, Chao Wu, Ming-Lei Xiao, Yu-Hui Zheng
article en

Abstract

A bstract We compute the complete one-loop renormalization group equations (RGEs) for all the four-fermion operators at dimension-8 Standard Model Effective Field Theory (SMEFT). We adopt the on-shell framework, where the RGEs are obtained from the unitarity cuts of the bubble integrals. To construct a consistent set of RGEs without redundancy, we utilize the Young Tensor amplitude/operator basis [1] as the building blocks of the tree-level amplitudes that constitute the unitarity cuts, which incorporates the full flavor structures of the effective operators. Due to the large number of effective operators for a dimension-8 type, it is crucial to reduce the integrated cuts to the same RGE amplitude basis, which is also made possible by the algorithm in the Young Tensor method. With the Mathematica package ABC4EFT that implements the method, we obtain the full result of the dimension-8 four-fermion RGEs with the output file attached as the supplementary material.

Journal of High Energy PhysicsVol. 2026(8)
Korea Institute for Advanced Study (KR), Sun Yat-sen University (CN), Chinese Academy of Sciences (CN), International Centre for Theoretical Physics Asia-Pacific (CN), University of Chinese Academy of Sciences (CN)
National Natural Science Foundation of China, Sun Yat-sen University, National Key Research and Development Program of China, Fundamental Research Funds for the Central Universities, Shenzhen Science and Technology Innovation Program, Korea Institute for Advanced Study
Openalex Percentile: Top 11%
Quantum Chromodynamics and Particle Interactions
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On-shell renormalization of dim-8 SMEFT from complete amplitude basis. Part I. Four-fermion operators — Jiang-Hao Yu, Chao Wu, et al. · Journal of High Energy Physics (2026) | TGRS Research Map | TGRS