230 lines
9.3 KiB
Plaintext
230 lines
9.3 KiB
Plaintext
This is a list of changes to higlu.f since October 1995:
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June 12 2024: - small adjustments to modern compilers (thanks to F. Kahlhoefer)
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September 21 2018: - commented out all calls to the subroutine soft (thanks
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to M. Battaglia and J. Baglio)
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March 19 2018: version 4.50:
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- added option for cxn integrated from pTmin to pTmax
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May 19 2016: version 4.40:
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- bug fix in HDECAY interface for MSbar quark masses
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(thanks to R. Harlander, A. Lazopoulos and H. Mantler)
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January 13 2016: version 4.34:
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- bug fix in SLHA interface
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- bug fix for pseudoscalar Higgs: missing variable
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defined
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(thanks to A. Arbey)
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December 16 2015: version 4.33:
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- bug fixes in matching to dim5 operators
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December 4 2015: version 4.32:
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- scale dependence of c_g improved
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- flag setting corrected
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December 4 2015: version 4.31:
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- added an extensive comment card at the beginning of
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higlu.f explaining the input in higlu.in
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- linked to new version 6.50 of HDECAY (using MSbar
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masses for bottom and charm as input)
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October 14 2015: version 4.30:
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- NNLL scale dependence of point-like Hgg coupling c_g
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included -> input scale added to input file
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- typos corrected (no numerical impact)
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September 4 2015: - Typos in NNLO scale dependence corrected
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April 17 2015: version 4.20:
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- Extension to inclusion of dim5 operator
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L_6 = c_g \alpha_s/\pi G^{a\mu\nu} G^a_{\mu\nu} H/v
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up to NNLO in the inclusive cross section (including the
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mismatch of virtual corrections originating from the
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effective Lagrangian compared to the top loops) and at
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LO for the pT distribution (that contributes to the NLO
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corrections to the inclusive cross section).
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April 7 2015: - Typo in NNLO scale dependence corrected. Numerical
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impact only for different renormalization and
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factorization scales.
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March 6 2015: - Typo in SM4 extension corrected.
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March 3 2015: version 4.10:
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- link to new HDECAY version 6.41
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- addition of charm loops (a per-cent effect on the cxn)
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December 10 2013: version 4.00: major upgrade
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- general link to HDECAY 6.00 with 2HDM extension
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- calculation of consistent LO, NLO and NNLO cross
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sections in a single run (all three PDFs need to be
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defined in higlu.in)
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- model determined by hdecay.in in HDECAY style
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- NNLO corrections (in the heavy quark limit) only added
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to top-loop contributions (and t'/b'-loop
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contributions in the SM4) in all models
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- optionally the SM elw. corrections can be included
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within the 2HDM by rescaling them by the HWW/HZZ
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coupling factors as an approximation
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December 2 2013: - Typos in NNLO corrections to pseudoscalar Higgs
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production corrected (numerical impact small)
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(thanks to R. Harlander).
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November 21 2013: - Typos in NNLO corrections to pseudoscalar Higgs
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production corrected (numerical impact small)
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(thanks to R. Harlander).
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October 31 2012: - Bug in feynhiggs.f corrected (not our fault)
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October 16 2012: - bug for bottom loops corrected (does not affect
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results using the bottom pole mass)
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October 11 2011: version 3.11
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- update of the grid for elw. corrections within the SM4
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September 20 2011: version 3.10:
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- inclusion of elw. SM4 corrections for m_b'=600 GeV and
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m_t' = m_b' + 50*(1+log[M_H/(115 GeV)]/5) GeV. Please,
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cite the following paper for these corrections:
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%\cite{Passarino:2011kv}
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\bibitem{Passarino:2011kv}
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G.~Passarino, C.~Sturm, S.~Uccirati,
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%``Complete Electroweak Corrections to Higgs production in a Standard
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%Model with four generations at the LHC,''
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[arXiv:1108.2025 [hep-ph]].
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July 6 2011: version 3.01:
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- small refinement in the NNLO QCD corrections within the
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SM4
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July 5 2011: version 3.00: major upgrade
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- NNLO QCD corrections and mixed elw./QCD corrections
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to total cxn included
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- NNLO evolution of alpha_s included
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- Extension to 4th-generation SM4 @ NNLO added
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February 16 2011: version 2.504: Bugs in initialization of the quark
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masses corrected (thanks to S. Liebler)
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January 28 2011: version 2.503: Decoupling of quark masses inside the
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loops from quark masses for alpha_s in order to allow
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for 4th-generation quarks etc.
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November 26 2010: version 2.502: Bug in transformation from bottom pole
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mass to MSbar mass corrected, numerical effect small
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November 5 2010: version 2.501: Bug in Higgs pT distribution in the gq
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channel corrected. Numerical effect small (thanks to
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R. Harlander and H. Mantler).
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April 20 2010: version 2.500:
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- Flag for electroweak corrections provided with check if
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calculation within the SM
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- Squark loops added for MSSM including the pure QCD
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corrections of
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%\cite{Muhlleitner:2006wx}
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\bibitem{Muhlleitner:2006wx}
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M.~Muhlleitner and M.~Spira,
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%``Higgs boson production via gluon fusion: Squark loops at NLO QCD,''
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Nucl.\ Phys.\ B {\bf 790} (2008) 1
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[arXiv:hep-ph/0612254].
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%%CITATION = NUPHA,B790,1;%%
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The Squark couplings G_SBi, G_STi are the ones of
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Eqs.(21,25,29) of this paper, if MODEL = 0. Within the
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MSSM they multiply the MSSM couplings, i.e.
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G_SBi = G_STi = 1 defines the MSSM.
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February 18 2010: - version 2.400:
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Electroweak corrections to SM Higgs boson production
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implemented in factorized form (thanks to G. Passarino
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et al.). Please, cite the following papers for these
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corrections:
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%\cite{Actis:2008ts}
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\bibitem{Actis:2008ts}
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S.~Actis, G.~Passarino, C.~Sturm and S.~Uccirati,
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%``NNLO Computational Techniques: the Cases H -> gamma gamma and H -> g g,''
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Nucl.\ Phys.\ B {\bf 811} (2009) 182
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[arXiv:0809.3667 [hep-ph]].
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%%CITATION = NUPHA,B811,182;%%
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%\cite{Actis:2008ug}
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\bibitem{Actis:2008ug}
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S.~Actis, G.~Passarino, C.~Sturm and S.~Uccirati,
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%``NLO Electroweak Corrections to Higgs Boson Production at Hadron
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%Colliders,''
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Phys.\ Lett.\ B {\bf 670} (2008) 12
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[arXiv:0809.1301 [hep-ph]].
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%\cite{Actis:2008uh}
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\bibitem{Actis:2008uh}
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S.~Actis, G.~Passarino, C.~Sturm and S.~Uccirati,
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%``Two-Loop Threshold Singularities, Unstable Particles and Complex Masses,''
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Phys.\ Lett.\ B {\bf 669} (2008) 62
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[arXiv:0809.1302 [hep-ph]].
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%%CITATION = PHLTA,B669,62;%%
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November 20 2009: - Link to LHAPDF implemented. Fortran compiler
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gfortran added to makefile. Links to PDFLIB, MRST2001
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and MSTW2008 removed (included in LHAPDF).
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October 16 2009: - Option to choose between bottom pole mass and bottom
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MSbar mass (including independent scale choice) added
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**********************************************************
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BOTTOM MASS: 0 = POLE MASS 1 = MSBAR MASS
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============ SCALE = MU_1*M_HIGGS + MU_2 (FOR MSBAR MASS)
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BOTMASS = 0
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MU_1 = 0.D0
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MU_2 = 10.D0
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**********************************************************
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Careful: Best choices are pole mass or MSbar bottom
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mass at a scale of O(m_b) due to large logs if the
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scale is of O(Higgs mass)! (see Fig.7a of NPB453 (1995) 17)
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--> version 2.300
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October 15 2009: - Link to MSTW2008 PDFs
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- dsigma/p_T and d2sigma/dp_T/dy distributions added (LO):
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**********************************************************
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DISTRIBUTIONS: 0=TOT CXN 1=D2SIGMA/DP_T/DY 2=DSIGMA/DP_T
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============= (ONLY FOR GG --> H)
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DISTRIB = 0
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P_T = 100.D0
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Y = 0.D0
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**********************************************************
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--> version 2.200
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Note that the central scale for the pt distributions is
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defined to be the transverse mass by default!
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April 3 2006: - Adding delta_mb corrections to bottom Yukawa couplings
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March 1 2006: - Removing an instability in the subroutine AMHAMA
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(thanks to P. Trueb)
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April 12 2005: - Link to CTEQ6 and MRST2001 PDFs
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(NGROUP = -1: CTEQ6 -2: MRST2001)
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November 7 2003: - Lines 919,920 added due to problems with g77 compiler
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(thanks to M. Schumacher)
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November 6 2003: - Lines 491-495 commented out to allow arbitrary Yukawa
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couplings (thanks to M. Schumacher)
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February 28 2003: - Extension of MSSM subroutines such that they are in
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agreement with HDECAY (version 3.0) now.
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