Holomorphy without supersymmetry in the Standard Model Effective Field Theory
Abstract
The anomalous dimensions of dimension-six operators in the Standard Model Effective Field Theory (SMEFT) respect holomorphy to a large extent. Holomorphy conditions are reminiscent of supersymmetry, even though the SMEFT is not a supersymmetric theory.
- Authors:
-
- Univ. of California, San Diego, CA (United States). Dept. of Physics
- Publication Date:
- Research Org.:
- Univ. of California, San Diego, CA (United States)
- Sponsoring Org.:
- USDOE
- OSTI Identifier:
- 1197960
- Alternate Identifier(s):
- OSTI ID: 1454835
- Grant/Contract Number:
- SC0009919
- Resource Type:
- Published Article
- Journal Name:
- Physics Letters. B
- Additional Journal Information:
- Journal Name: Physics Letters. B Journal Volume: 739 Journal Issue: C; Journal ID: ISSN 0370-2693
- Publisher:
- Elsevier
- Country of Publication:
- Netherlands
- Language:
- English
- Subject:
- 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
Citation Formats
Alonso, Rodrigo, Jenkins, Elizabeth E., and Manohar, Aneesh V. Holomorphy without supersymmetry in the Standard Model Effective Field Theory. Netherlands: N. p., 2014.
Web. doi:10.1016/j.physletb.2014.10.045.
Alonso, Rodrigo, Jenkins, Elizabeth E., & Manohar, Aneesh V. Holomorphy without supersymmetry in the Standard Model Effective Field Theory. Netherlands. https://doi.org/10.1016/j.physletb.2014.10.045
Alonso, Rodrigo, Jenkins, Elizabeth E., and Manohar, Aneesh V. Fri .
"Holomorphy without supersymmetry in the Standard Model Effective Field Theory". Netherlands. https://doi.org/10.1016/j.physletb.2014.10.045.
@article{osti_1197960,
title = {Holomorphy without supersymmetry in the Standard Model Effective Field Theory},
author = {Alonso, Rodrigo and Jenkins, Elizabeth E. and Manohar, Aneesh V.},
abstractNote = {The anomalous dimensions of dimension-six operators in the Standard Model Effective Field Theory (SMEFT) respect holomorphy to a large extent. Holomorphy conditions are reminiscent of supersymmetry, even though the SMEFT is not a supersymmetric theory.},
doi = {10.1016/j.physletb.2014.10.045},
journal = {Physics Letters. B},
number = C,
volume = 739,
place = {Netherlands},
year = {Fri Dec 12 00:00:00 EST 2014},
month = {Fri Dec 12 00:00:00 EST 2014}
}
Free Publicly Available Full Text
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https://doi.org/10.1016/j.physletb.2014.10.045
https://doi.org/10.1016/j.physletb.2014.10.045
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Cited by: 53 works
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Figures / Tables:
Table 1: Form of the one-loop anomalous dimension matrix as defined in Eqs. (10), (11) for d = 6 operators. Y is a Yukawa coupling. The first 4 rows and columns involve holomorphic operators, and the rest involve non-holomorphic operators. The RGE for the rows can depend on the Cmore »
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Figures/Tables have been extracted from DOE-funded journal article accepted manuscripts.