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One-loop non-renormalization results in EFTs

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arxiv 1412.7151 v3 pith:CUHAJUBE submitted 2014-12-22 hep-ph hep-th

classification hep-phhep-th
keywords one-loopoperatorseftsmanyanomalousdimensionslevelsupersymmetry
verification ladder T0 review T1 audit T2 compute T3 formal
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In Effective Field Theories (EFTs) with higher-dimensional operators many anomalous dimensions vanish at the one-loop level for no apparent reason. With the use of supersymmetry, and a classification of the operators according to their embedding in super-operators, we are able to show why many of these anomalous dimensions are zero. The key observation is that one-loop contributions from superpartners trivially vanish in many cases under consideration, making supersymmetry a powerful tool even for non-supersymmetric models. We show this in detail in a simple U(1) model with a scalar and fermions, and explain how to extend this to SM EFTs and the QCD Chiral Langrangian. This provides an understanding of why most "current-current" operators do not renormalize "loop" operators at the one-loop level, and allows to find the few exceptions to this ubiquitous rule.

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Cited by 2 Pith papers

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  1. Supersymmetric geometry in non-supersymmetric effective field theory

    hep-th 2026-06 unverdicted novelty 6.0 of 10

    Authors construct supersymmetric embeddings for non-SUSY gauge theory operators up to dimension six and use vector bundles to reveal an underlying complex geometry that organizes operators under field redefinitions ac...

  2. Renormalization of effective field theories via on-shell methods: the case of axion-like particles

    hep-ph 2024-12 conditional novelty 6.0 of 10

    Complete one-loop anomalous dimension matrix for a CP-violating ALP effective field theory, derived via on-shell unitarity methods and extended to dimension-6 SMEFT operators.

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