2015
DOI: 10.1140/epjc/s10052-015-3494-6
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Generic two-loop Higgs mass calculation from a diagrammatic approach

Abstract: We calculate the corrections to the Higgs mass in general theories restricted to the case of massless gauge bosons (the gaugeless limit). We present analytic expressions for the two-loop tadpole diagrams, and corresponding expressions for the zero-momentum limit of the Higgs self-energies, equivalent to the second derivative of the twoloop effective potential. We describe the implementation in SARAH, which allows for an efficient, accurate and rapid evaluation for generic theories. In the appendix, we provide … Show more

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Cited by 94 publications
(137 citation statements)
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References 65 publications
(105 reference statements)
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“…We also used SARAH to generate a SPheno module [41,42] for the NMSSM. With this module we calculate the SUSY and Higgs masses including NMSSM-specific two-loop corrections [43][44][45] which are important in particular for large |λ| [46,47]. Consequently, the accuracy in the Higgs mass prediction is similar to the MSSM and we use 3 GeV for the theoretical uncertainty in the following.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…We also used SARAH to generate a SPheno module [41,42] for the NMSSM. With this module we calculate the SUSY and Higgs masses including NMSSM-specific two-loop corrections [43][44][45] which are important in particular for large |λ| [46,47]. Consequently, the accuracy in the Higgs mass prediction is similar to the MSSM and we use 3 GeV for the theoretical uncertainty in the following.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…All important two-loop corrections stemming from new particles and/or new interactions are covered as discussed in detail in Refs. [53][54][55]. The calculations make use of the generic results of Refs.…”
Section: Higgs Mass Beyond the Mssmmentioning
confidence: 99%
“…This information together with generic expressions for various observables is then used to generate Fortran code for SPheno [87,88] which can be used to obtain numerical results. Up to now, one-and twoloop masses [89][90][91], one-loop flavour and precision observables [92], as well as two-and three-body tree-level decays could be obtained via this setup. We have now enhanced the decay calculation to the next level by a generic ansatz to calculate two-body decay widths at the full one-loop level.…”
Section: Introductionmentioning
confidence: 99%