Scope of the 1-loop part: mt^4 approximation (for real parameters) top/stop sector top/stop + bottom/sbottom sector full (s)quark/(s)lepton sector full MSSM
Mixing in the neutral Higgs sector: no mixing 2x2 (h0-HH) mixing = real parameters 3x3 (h0-HH-A0) mixing = complex parameters
Approximation for the 1-loop result: no approximation p^2 = 0 approximation self-energies are calculated at p^2 = M_tree^2 imaginary parts of self-energies are discarded no approx., UHiggs evaluated at p^2 = 0
Higher-order corrections: tree level only 1-loop corrections 2-loop corrections
Inclusion of log resummation: no log resummation NLL resummation (for large MSUSY) NLL resummation (for large MCha,MNeu,MGlu,MSUSY) NNLL resummation (for large MCha,MNeu,MGlu,MSUSY) 2HDM as low-energy model
m_{t} in the 1-/2-loop corrections: pole top mass running top mass (SM MSbar 2L) running top mass (SM MSbar 1L) running top mass (MSSM DRbar)
m_{b} in the 1-/2-loop corrections: non-resummed MB resummed MB 1-loop resummed MB 2-loop
complex parameters in the 2-loop corrections: all corrections evaluated in the rMSSM αs αt + αt αt corrections in the cMSSM only αs αt + αt αt corr. in cMSSM + rest in rMSSM αs αt + αt αt corr. in cMSSM + rest interpolated in At, Ab, M3, μ αs αt + αt αt corr. in cMSSM + rest interpolated in At, Xb, M3, μ αs αt + αt αt corr. in cMSSM + rest interpolated in Xt, Ab, M3, μ αs αt + αt αt corr. in cMSSM + rest interpolated in Xt, Xb, M3, μ
p^{2}-dependent terms in the 2-loop corrections: not included included (warning: may take long)
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