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QCD radiative corrections for h→bb¯ in the standard model dimension-6 effective field theory

Gauld, R.; Pecjak, B.D.; Scott, D.J.

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Authors

R. Gauld

D.J. Scott



Abstract

We calculate the O(αs) QCD corrections to the inclusive h→bb¯ decay rate in the dimension-6 standard model effective field theory (SMEFT). The QCD corrections multiplying the dimension-6 Wilson coefficients which alter the hbb¯-vertex at tree-level are proportional to the standard model (SM) ones, so next-to-leading order results can be obtained through a simple rescaling of the tree-level decay rate. On the other hand, contributions from the operators QbG and QHG, which alter the gbb¯-vertex and introduce a hgg-vertex respectively, enter at O(αs) and induce sizeable corrections which are unrelated to the SM ones and cannot be anticipated through a renormalization-group analysis. We present compact analytic results for these contributions, which we recommend to be included in future phenomenological studies.

Citation

Gauld, R., Pecjak, B., & Scott, D. (2016). QCD radiative corrections for h→bb¯ in the standard model dimension-6 effective field theory. Physical Review D, 94(7), Article 074045. https://doi.org/10.1103/physrevd.94.074045

Journal Article Type Article
Acceptance Date Oct 11, 2016
Online Publication Date Oct 31, 2016
Publication Date Oct 31, 2016
Deposit Date Dec 6, 2016
Publicly Available Date Dec 7, 2016
Journal Physical Review D
Print ISSN 2470-0010
Electronic ISSN 2470-0029
Publisher American Physical Society
Peer Reviewed Peer Reviewed
Volume 94
Issue 7
Article Number 074045
DOI https://doi.org/10.1103/physrevd.94.074045
Public URL https://durham-repository.worktribe.com/output/1390017
Related Public URLs https://arxiv.org/abs/1607.06354

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Copyright Statement
Reprinted with permission from the American Physical Society: Physical Review D 94, 074045 © (2016) by the American Physical Society. Readers may view, browse, and/or download material for temporary copying purposes only, provided these uses are for noncommercial personal purposes. Except as provided by law, this material may not be further reproduced, distributed, transmitted, modified, adapted, performed, displayed, published, or sold in whole or part, without prior written permission from the American Physical Society.






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