FHRetrieveFlags - retrieve the FeynHiggs flags integer error integer mssmpart, higgsmix, p2approx, looplevel, loglevel integer runningMT, botResum, tlCplxApprox subroutine FHRetrieveFlags(error, mssmpart, higgsmix, p2approx, looplevel, loglevel, runningMT, botResum, tlCplxApprox) FHRetrieveFlags[] FHRetrieveFlags retrieves the flags from FeynHiggs. error (output) zero if successful, otherwise the line number in RetrieveFlags.F from which the error message was emitted mssmpart = 0..4 (output) specifies the scope of the calculation: 0: MT^4-approximation 1: top/stop-sector 2: top/stop- + bottom/sbottom-sector 3: full (s-)quark/lepton-sector 4: full MSSM higgsmix = 1..3 (output) determines the mixing in the Higgs sector: 1: All non-diagonal (ND) Self Energies = 0 2: All CP-violating ND Self Energies = 0 3: Full 3x3 mixing in the neutral sector This means: 2: evaluation in the rMSSM 3: evaluation in the cMSSM p2approx = 0..4 (output) determines the approximation for the 1-loop result: 0: None, i.e. full determination of the propagator matrices's poles, UHiggs is evaluated at p^2 = m^2 1: p^2 = 0 approximation 2: All self energies are calculated at p^2 = m_tree^2 3: imaginary parts of self-energies are discarded 4: as 0, but with UHiggs evaluated at p^2 = 0 looplevel = 0..2 (output) determines the inclusion of higher-order corrections: 0: tree level 1: one-loop contributions only 2: include various two-loop contributions loglevel = 0..3 (output) determines the inclusion of log resummations: 0: no log resummation 1: NLL resummation (for large MSUSY) 2: NLL resummation (for large MCha,MNeu,MGlu,MSUSY) 3: NNLL resummation (for large MCha,MNeu,MGlu,MSUSY) runningMT = 0..3 (input) determines which top mass shall be used in the 1-/2-loop correc- tions: 0: pole MT 1: running MT (SM MSbar 2L) 2: running MT (SM MSbar 1L) 3: running MT (MSSM DRbar) botResum = 0..1 (output) determines whether the O(tan beta^n) corrections shall be re- summed: 0: no resummation 1: 1L resummation 2: 1L resummation for Higgs self-energies, 2L resummation for Higgs decays tlCplxApprox = 0..6 (output) determines how the two-loop corrections are treated in the pres- ence of complex parameters (cMSSM): 0: all corrections are evaluated in the rMSSM 1: only the cMSSM a_s a_t corrections are used 2: the cMSSM a_s a_t corrections are combined with the remaining corrections in the rMSSM 3: the cMSSM a_s a_t corrections are combined with the remaining corrections, interpolated in the complex phases (cf. FHSelec- tIPol) libFH(1) 30-Jan-2018 FHRETRIEVEFLAGS(1)