Light MSSM Higgs boson mass to three-loop accuracy

By Philipp Kant, Robert V. Harlander, L. Mihaila, Matthias Steinhauser. 2010

170 citations recorded by the source corpus.

The light CP even Higgs boson mass, Mh, is calculated to three-loop accuracy within the Minimal Supersymmetric Standard Model (MSSM). The result is expressed in terms of $ \overline {\text{DR}} $ parameters and implemented in the computer program H3m. The calculation is based on the proper approximations and their combination in various regions of the parameter space. The three-loop effects to Mh are typically of the order of a few hundred MeV and opposite in sign to the two-loop corrections. The remaining theory uncertainty due to higher order perturbative corrections is estimated to be less than 1 GeV.

Subfields: Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/f465a825013ecb7061f475f3b59e8f29a26bdfea

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Nuclear and High Energy Physics

Citations in the corpus

Naturalness and the Status of Supersymmetry (2013, background): “Several codes incorporate 2-loop [64–66], or even 3-loop [67, 68], corrections.”
Fully covering the MSSM Higgs sector at the LHC (2015, background): “However, this relation is violated since important radiative corrections, that introduce a dependence on many SUSY parameters, occur in this context [14–25].”
Precise prediction for the light MSSM Higgs-boson mass combining effective field theory and fixed-order calculations (2016, background): “The full one-loop result [3–5], the dominant two-loop corrections [6–20] as well as partial three-loop results [21, 22] are known.”
ILC Higgs White Paper (2013, background): “A more complete treatment of the radiative corrections [133, 134, 135] shows that eq.”
SusHi: A program for the calculation of Higgs production in gluon fusion and bottom-quark annihilation in the Standard Model and the MSSM (2012, unknown): “However, this option allows one to use H3m [81], for example, in order to take into account three-loop effects to the SUSY Higgs mass [80–82].”