Himalaya 3.0.0
New features
-
The 1-, 2- and 3-loop corrections of O(αt), O(αt*αs + αt^2) and O(αt*αs^2) to the squared light CP-even Higgs mass are now available in the EFT limit v^2 << MSUSY^2.
At the C++ level one can use the following new accessors of the
HierarchyObject
class:getDMh2EFTAt(int loops)
: Returns loop corrections in the EFT limit v^2 << MSUSY^2.getDMh2FOAt(int loops)
: Returns loop corrections in the full MSSM.
At the Mathematica level the following new symbols are provided in the output of
HimalayaCalculateDMh3L[]
:Mh2EFTAt
: Loop corrections in the EFT limit v^2 << MSUSY^2.Mh2FOAt
: Loop corrections in the full MSSM.
-
The full 1-loop, 2-loop O((αt+ab)*αs + (αt+αb)^2 + ab*aτ + aτ^2) and 3-loop O(αt*αs^2) to the squared light CP-even Higgs mass are now available.
At the C++ level one can use the new accessor
getDMh2FO(int loops)
of theHierarchyObject
class.At the Mathematica level the new symbol
Mh2FO
is provided in the output ofHimalayaCalculateDMh3L[]
.
Changes
-
The getter to access the loop corrections to the light CP-even Higgs mass in the EFT limit has been renamed
getDMh2EFT
->getDMh2EFTAt
. The new name reflects that fact that only αt-enhanced contributions are returned. -
The Mathematica symbol which contains the loop corrections to the light CP-even Higgs mass in the EFT limit has been renamed
Mh2EFT
->Mh2EFTAt
. The new name reflects that fact that only αt-enhanced contributions are included.