Holomorphy without supersymmetry in the Standard Model Effective Field Theory

• DOI: 10.1016/j.physletb.2014.10.045
• Publication Date: 2014-10-22T17:18:20Z
• Authors: Rodrigo Alonso; Elizabeth E. Jenkins; Aneesh V. Manohar
• Keywords: High Energy Physics - Theory; Nuclear and High Energy Physics; QC1-999; Mathematical sciences; FOS: Physical sciences; Atomic; 01 natural sciences; Mathematical Sciences; Particle and Plasma Physics; High Energy Physics - Phenomenology (hep-ph); 0103 physical sciences; Nuclear; Mathematical Physics; hep-th; Physics; Molecular; Particle and High Energy Physics; hep-ph; Nuclear and Plasma Physics; Nuclear & Particles Physics; Physical sciences; High Energy Physics - Phenomenology; High Energy Physics - Theory (hep-th); Physical Sciences; Astronomical and Space Sciences

Minor corrections in Table I, see note added at end of paper. The complete SMEFT RGE will be maintained at http://einstein.ucsd.edu/smeft<br/>The anomalous dimensions of dimension-six operators in the Standard Model Effective Field Theory (SMEFT) respect holomorphy to a large extent. The holomorphy conditions are reminiscent of supersymmetry, even though the SMEFT is not a supersymmetric theory.<br/>