The FlexibleSUSY-generated spectrum generators can be called from within Mathematica using Wolfram's LibraryLink interface.
Table of Contents
The following example calculates the pole mass spectrum and the observables in the CMSSM for a given parameter point
Get["models/CMSSM/CMSSM_librarylink.m"];
(* Create a handle to a model given the input parameters.
See Options[FSCMSSMOpenHandle] for all default options. *)
handle = FSCMSSMOpenHandle[
fsSettings -> { precisionGoal -> 1.*^-4 },
fsSMParameters -> { Mt -> 173.3 },
fsModelParameters -> {
m0 -> 125, m12 -> 500, TanBeta -> 10, SignMu -> 1, Azero -> 0 }
];
(* calculate pole mass spectrum *)
FSCMSSMCalculateSpectrum[handle]
(* calculate further observables *)
FSCMSSMCalculateObservables[handle]
(* close the model handle *)
FSCMSSMCloseHandle[handle];
Note: For each model, FlexibleSUSY creates an example Mathematica
script which illustrates the use of the Mathematica interface. The
generated example can be found in models/<model>/run_<model>.m
,
which can be run for example as
math -run "<< \"models/<model>/run_<model>.m\""
Before running the example Mathematica script, the model parameters in the script should be set to reasonable values.
In the following more advanced example the Higgs pole mass is calculated in the HSSUSY model (an EFT calculation of the SM-like Higgs mass, assuming that the high-energy completion is the MSSM) as a function of X_t / M_S for \tan\beta = 5 and different values of the SUSY scale. The example also illustrates how parallelization can be used to exploit the performance of multi-core systems.
Get["models/HSSUSY/HSSUSY_librarylink.m"];
CalcMh[TB_, Xtt_, MS_] := Module[{handle, spec},
handle = FSHSSUSYOpenHandle[
fsSettings -> {
precisionGoal -> 1.*^-5,
calculateStandardModelMasses -> 1,
poleMassLoopOrder -> 4,
ewsbLoopOrder -> 4,
betaFunctionLoopOrder -> 4,
thresholdCorrectionsLoopOrder -> 3,
thresholdCorrections -> 123111321,
parameterOutputScale -> 173.34
},
fsModelParameters -> {
TanBeta -> TB,
MEWSB -> 173.34,
MSUSY -> MS,
M1Input -> MS,
M2Input -> MS,
M3Input -> MS,
MuInput -> MS,
mAInput -> MS,
AtInput -> (Xtt + 1/TB) * MS,
AbInput -> 0,
AtauInput -> 0,
msq2 -> MS^2 IdentityMatrix[3],
msu2 -> MS^2 IdentityMatrix[3],
msd2 -> MS^2 IdentityMatrix[3],
msl2 -> MS^2 IdentityMatrix[3],
mse2 -> MS^2 IdentityMatrix[3],
LambdaLoopOrder -> 2,
TwoLoopAtAs -> 1,
TwoLoopAbAs -> 1,
TwoLoopAtAb -> 1,
TwoLoopAtauAtau -> 1,
TwoLoopAtAt -> 1
}
];
spec = HSSUSY /. FSHSSUSYCalculateSpectrum[handle];
FSHSSUSYCloseHandle[handle];
If[spec =!= $Failed, Pole[M[hh]] /. spec, 0]
];
LaunchKernels[];
DistributeDefinitions[CalcMh];
data = {
ParallelMap[{#, CalcMh[5, #, 1000 ]}&, Range[-3.5, 3.5, 0.1]],
ParallelMap[{#, CalcMh[5, #, 2000 ]}&, Range[-3.5, 3.5, 0.1]],
ParallelMap[{#, CalcMh[5, #, 10000]}&, Range[-3.5, 3.5, 0.1]]
};
plot = ListPlot[data,
PlotLegends -> {"MS = 1 TeV", "MS = 2 TeV", "MS = 10 TeV"},
Axes -> False, Frame -> True,
FrameLabel -> {"Xt / MS", "Mh / GeV"}];
Export["HSSUSY_Mh_Xt.png", plot, ImageSize -> 1000];
Output:
In order to build the LibraryLink library, FlexibleSUSY must be
configured with --enable-meta
(enabled by default).
Example:
./configure --with-models=CMSSM make
The LibraryLink library can be found in
models/<model>/<model>_librarylink.so
, where <model>
is the model
name. In order to use FlexibleSUSY's generated <model>
spectrum
generator at the Mathematica level, the library functions must be
loaded using the models/<model>/<model>_librarylink.m
script.
Example
Get["models/CMSSM/CMSSM_librarylink.m"];
First, a handle to the model must be created using the
FS<model>OpenHandle[]
function. The function takes as arguments
- the spectrum generator settings via the
fsSettings
variable - the Standard Model input parameters via the
fsSMParameters
variable - the model input parameters via the
fsModelParameters
variable
Example
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsSettings -> { precisionGoal -> 1.*^-4 },
fsSMParameters -> { Mt -> 173.3 },
fsModelParameters -> {
m0 -> 125, m12 -> 500, TanBeta -> 10, SignMu -> 1, Azero -> 0 }
];
FSCMSSMGetSettings[handle]
FSCMSSMGetSMInputParameters[handle]
FSCMSSMGetInputParameters[handle]
The FS<model>OpenHandle[]
fixes all settings and input parameters at
once. Unspecified parameters are set to their default values. The
default values are stored in the variables fsDefaultSettings
,
fsDefaultSMParameters
and fs<model>DefaultInputParameters
Get["models/CMSSM/CMSSM_librarylink.m"];
Print[fsDefaultSettings];
Print[fsDefaultSMParameters];
Print[fsCMSSMDefaultInputParameters];
The settings associated to a handle
can be listed using the
FS<model>GetSettings[]
function. Please refer to the
FlexibleSUSY run-time configuration for more information on the
spectrum generator settings.
Example
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsSettings -> { precisionGoal -> 1.*^-5, betaFunctionLoopOrder -> 3 }
];
FSCMSSMGetSettings[handle]
Output
{ precisionGoal -> 0.00001,
maxIterations -> 0,
calculateStandardModelMasses -> 0,
poleMassLoopOrder -> 2,
ewsbLoopOrder -> 2,
betaFunctionLoopOrder -> 3,
thresholdCorrectionsLoopOrder -> 2,
higgs2loopCorrectionAtAs -> 1,
higgs2loopCorrectionAbAs -> 1,
higgs2loopCorrectionAtAt -> 1,
higgs2loopCorrectionAtauAtau -> 1,
forceOutput -> 0,
top2loopCorrectionsQCD -> 1,
betaZeroThreshold -> 1.*10^-11,
forcePositiveMasses -> 0,
poleMassScale -> 0.,
parameterOutputScale -> 0. }
The Standard Model input parameters associated to a handle
can be
listed using the FS<model>GetSMInputParameters[]
function.
Example
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsSMParameters -> { Mt -> 173.34 }
];
FSCMSSMGetSMInputParameters[handle]
Output
{ alphaEmMZ -> 0.00781763, (* alpha_em(MZ) in the SM(5), MS-bar *)
GF -> 0.000011663787, (* Fermi constant *)
alphaSMZ -> 0.1184, (* alpha_s(MZ) in the SM(5), MS-bar *)
MZ -> 91.1876, (* Z pole mass *)
mbmb -> 4.18, (* MS-bar bottom mass at Q = mb *)
Mt -> 173.34, (* top pole mass *)
Mtau -> 1.777, (* tau pole mass *)
Mv3 -> 0., (* 3rd heaviest neutrino mass *)
MW -> 80.385, (* W pole mass *)
Me -> 0.000510999, (* electron pole mass *)
Mv1 -> 0., (* 1st neutrino mass *)
Mm -> 0.105658, (* muon pole masss *)
Mv2 -> 0., (* 2nd neutrino mass *)
md2GeV -> 0.00475, (* MS-bar down quark mass at Q = 2 GeV *)
mu2GeV -> 0.0024, (* MS-bar up quark mass at Q = 2 GeV *)
ms2GeV -> 0.104, (* MS-bar strange quark mass at Q = 2 GeV *)
mcmc -> 1.27, (* MS-bar charm quark mass at Q = mc *)
alphaEm0 -> 0.00729735, (* alpha_em in the Thompson limit *)
Mh -> 125.09 } (* Higgs pole mass *)
The model input parameters associated to a handle
can be listed
using the FS<model>GetInputParameters[]
function.
Example
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsModelParameters -> { m0 -> 125, m12 -> 500, TanBeta -> 10, SignMu -> 1 }
];
FSCMSSMGetInputParameters[handle]
Output
{ m0 -> 125.,
m12 -> 500.,
TanBeta -> 10.,
SignMu -> 1,
Azero -> 0. }
Using the FS<model>Set[]
function, the input parameters and settings
associated to a certain handle can be modified. The FS<model>Set[]
function takes first as argument the handle, and as second argument
the replacement list of new parameters / settings.
Example
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsSettings -> { precisionGoal -> 1.*^-4 },
fsSMParameters -> { Mt -> 173.3 },
fsModelParameters -> {
m0 -> 125, m12 -> 500, TanBeta -> 10, SignMu -> 1, Azero -> 0 }
];
FSCMSSMGetInputParameters[handle]
FSCMSSMSet[handle, TanBeta -> 20];
FSCMSSMGetInputParameters[handle]
Output
{m0 -> 125., m12 -> 500., TanBeta -> 10., SignMu -> 1, Azero -> 0.}
{m0 -> 125., m12 -> 500., TanBeta -> 20., SignMu -> 1, Azero -> 0.}
For each <model>
, the FS<model>CalculateSpectrum[handle]
function
solves the boundary value problem and calculates the pole mass
spectrum. The function takes a model handle as arguments, referring
to the settings and input parameters
The function returns all running model parameters at the parameter
output scale (either the SUSY scale or the scale set via fsSettings
-> { parameterOutputScale -> 1000. }
) and the running masses at the
same scale. The running masses are denoted by M[p]
where p
is the
particle name. The parameter output scale appears in the returned
list with the symbol SCALE
. The calculated pole masses are denoted
by Pole[M[p]]
, respectively. The mixing matrices which correspond
to the pole masses are denoted by Pole[Z]
, where Z is the name of
the mixing matrix.
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsModelParameters -> { m0 -> 125, m12 -> 500, TanBeta -> 10, SignMu -> 1 }
];
FSCMSSMCalculateSpectrum[handle]
Output
{CMSSM ->
{M[VG] -> 0., M[Glu] -> 1117.18, M[Fv] -> {0., 0., 0.},
M[Sd] -> {942.251, 977.989, 980.297, 980.3, 1023.94, 1023.94},
M[Sv] -> {347.371, 348.42, 348.424},
M[Su] -> {782.7, 983.889, 983.894, 987.561, 1021., 1021.},
M[Se] -> {219.073, 226.223, 226.248, 356.971, 356.976, 358.335},
M[hh] -> {88.1593, 732.573}, M[Ah] -> {90.0927, 732.337},
M[Hpm] -> {78.4808, 736.531},
M[Chi] -> {207.439, 376.528, 633.944, 647.755},
M[Cha] -> {376.365, 647.464},
M[Fe] -> {0.000520523, 0.107628, 1.81042},
M[Fd] -> {0.00243143, 0.0532355, 2.32379},
M[Fu] -> {0.00122119, 0.549091, 147.438}, M[VWm] -> 78.4808,
M[VP] -> 0., M[VZ] -> 90.0927,
ZD -> {{0., 0., -0.965619, 0., 0., -0.259961}, {0., 0., 0.259961, 0.,
0., -0.965619}, {0., -0.00456672, 0., 0., -0.99999,
0.}, {0.000208583, 0., 0., 1., 0., 0.}, {0., -0.99999, 0., 0.,
0.00456672, 0.}, {1., 0., 0., -0.000208583, 0., 0.}},
ZV -> {{0., 0., 1.}, {0., 1., 0.}, {1., 0., 0.}},
ZU -> {{0., 0., 0.430138, 0., 0., 0.902763}, {0., 0.00896415, 0., 0.,
0.99996, 0.}, {0.000019939, 0., 0., 1., 0., 0.}, {0., 0.,
0.902763, 0., 0., -0.430138}, {1., 0., 0., -0.000019939, 0.,
0.}, {0., 0.99996, 0., 0., -0.00896415, 0.}},
ZE -> {{0., 0., 0.145606, 0., 0., 0.989343}, {0., -0.00903329, 0.,
0., -0.999959, 0.}, {0.0000436949, 0., 0., 1., 0., 0.}, {1., 0.,
0., -0.0000436949, 0., 0.}, {0., -0.999959, 0., 0., 0.00903329,
0.}, {0., 0., 0.989343, 0., 0., -0.145606}},
ZH -> {{0.105881, 0.994379}, {0.994379, -0.105881}},
ZA -> {{-0.102825, 0.994699}, {0.994699, 0.102825}},
ZP -> {{-0.102825, 0.994699}, {0.994699, 0.102825}},
ZN -> {{-0.995744, 0.018728, -0.0832596, 0.0348113}, {0.0389752,
0.971833, -0.194009, 0.127995}, {0. - 0.0331609 I,
0. + 0.0485202 I, 0. + 0.703592 I,
0. + 0.70817 I}, {0.0766551, -0.229862, -0.678518, 0.69347}},
UM -> {{0.960661, -0.277725}, {0.277725, 0.960661}},
UP -> {{0.983012, -0.183543}, {0.183543, 0.983012}},
ZEL -> {{1., 0., 0.}, {0., 1., 0.}, {0., 0., 1.}},
ZER -> {{1., 0., 0.}, {0., 1., 0.}, {0., 0., 1.}},
ZDL -> {{1., 0., 0.}, {0., 1., 0.}, {0., 0., 1.}},
ZDR -> {{1., 0., 0.}, {0., 1., 0.}, {0., 0., 1.}},
ZUL -> {{1., 0., 0.}, {0., 1., 0.}, {0., 0., 1.}},
ZUR -> {{1., 0., 0.}, {0., 1., 0.}, {0., 0., 1.}},
ZZ -> {{-0.871112, 0.491084}, {-0.491084, -0.871112}},
Pole[M[VG]] -> 0., Pole[M[Glu]] -> 1151.38,
Pole[M[Fv]] -> {0., 0., 0.},
Pole[M[Sd]] -> {970.999, 1012.32, 1015.42, 1015.42, 1059.73,
1059.73}, Pole[M[Sv]] -> {351.491, 352.69, 352.694},
Pole[M[Su]] -> {809.283, 1015.61, 1018.71, 1019.46, 1056.91,
1056.91},
Pole[M[Se]] -> {222.482, 229.821, 229.847, 361.599, 361.604,
362.781}, Pole[M[hh]] -> {114.781, 719.259},
Pole[M[Ah]] -> {88.5742, 718.986},
Pole[M[Hpm]] -> {77.7605, 723.723},
Pole[M[Chi]] -> {204.267, 385.936, 636.143, 649.77},
Pole[M[Cha]] -> {385.949, 650.096}, Pole[M[Fe]] -> {0., 0., 0.},
Pole[M[Fd]] -> {0., 0., 0.}, Pole[M[Fu]] -> {0., 0., 0.},
Pole[M[VWm]] -> 80.3924, Pole[M[VP]] -> 0., Pole[M[VZ]] -> 0.,
Pole[ZD] -> {{0., 0., -0.977566, 0., 0., -0.210631}, {0., 0.,
0.210631, 0., 0., -0.977566}, {0., -0.0045424, 0., 0., -0.99999,
0.}, {0.000207472, 0., 0., 1., 0., 0.}, {0., -0.99999, 0., 0.,
0.0045424, 0.}, {1., 0., 0., -0.000207472, 0., 0.}},
Pole[ZV] -> {{0., 0., 1.}, {0., 1., 0.}, {1., 0., 0.}},
Pole[ZU] -> {{0., 0., 0.427999, 0., 0., 0.903779}, {0., 0., 0.903779,
0., 0., -0.427999}, {0., 0.00911132, 0., 0., 0.999958,
0.}, {0.0000202664, 0., 0., 1., 0., 0.}, {1., 0.,
0., -0.0000202664, 0., 0.}, {0., 0.999958, 0., 0., -0.00911132,
0.}}, Pole[
ZE] -> {{0., 0., 0.144271, 0., 3.02431*10^-15,
0.989538}, {0., -0.00895024, 2.08714*10^-14, 0., -0.99996,
0.}, {0.0000432932, 0., 0., 1., 0., 0.}, {1., 0.,
0., -0.0000432932, 0., 0.}, {0., -0.99996, -1.86811*10^-16, 0.,
0.00895024, 0.}, {0., 0., -0.989538, 0., -2.06711*10^-14,
0.144271}},
Pole[ZH] -> {{0.106581, 0.994304}, {0.994304, -0.106581}},
Pole[ZA] -> {{-0.0989827, 0.995089}, {0.995089, 0.0989827}},
Pole[ZP] -> {{-0.0995943, 0.995028}, {0.995028, 0.0995943}},
Pole[ZN] -> {{-0.995819, 0.0174686, -0.082821,
0.0343646}, {0.0380335, 0.970567, -0.197841,
0.131955}, {0. - 0.0332126 I, 0. + 0.0483916 I, 0. + 0.703447 I,
0. + 0.70832 I}, {0.0761299, -0.235272, -0.677615, 0.692596}},
Pole[UM] -> {{0.95912, -0.283001}, {0.283001, 0.95912}},
Pole[UP] -> {{0.981917, -0.189314}, {0.189314, 0.981917}},
Pole[ZEL] -> {{0., 0., 0.}, {0., 0., 0.}, {0., 0., 0.}},
Pole[ZER] -> {{0., 0., 0.}, {0., 0., 0.}, {0., 0., 0.}},
Pole[ZDL] -> {{0., 0., 0.}, {0., 0., 0.}, {0., 0., 0.}},
Pole[ZDR] -> {{0., 0., 0.}, {0., 0., 0.}, {0., 0., 0.}},
Pole[ZUL] -> {{0., 0., 0.}, {0., 0., 0.}, {0., 0., 0.}},
Pole[ZUR] -> {{0., 0., 0.}, {0., 0., 0.}, {0., 0., 0.}},
Pole[ZZ] -> {{0., 0.}, {0., 0.}},
Yd -> {{0.000136987, 0., 0.}, {0., 0.0029993, 0.}, {0., 0.,
0.130923}},
Ye -> {{0.0000293264, 0., 0.}, {0., 0.00606377, 0.}, {0., 0.,
0.102}},
Yu -> {{7.1123*10^-6, 0., 0.}, {0., 0.00319794, 0.}, {0., 0.,
0.858685}}, \[Mu] -> 630.611, g1 -> 0.467953, g2 -> 0.642978,
g3 -> 1.06483, vd -> 25.1013, vu -> 242.823,
T[Yd] -> {{-0.192259, 0., 0.}, {0., -4.20945, 0.}, {0.,
0., -171.869}},
T[Ye] -> {{-0.00878455, 0., 0.}, {0., -1.81633, 0.}, {0.,
0., -30.3818}},
T[Yu] -> {{-0.00817412, 0., 0.}, {0., -3.67535, 0.}, {0.,
0., -764.191}}, B[\[Mu]] -> 54854.6,
mq2 -> {{1.04513*10^6, 0., 0.}, {0., 1.04512*10^6, 0.}, {0., 0.,
889135.}},
ml2 -> {{125372., 0., 0.}, {0., 125369., 0.}, {0., 0., 124639.}},
mHd2 -> 109915., mHu2 -> -385101.,
md2 -> {{960350., 0., 0.}, {0., 960345., 0.}, {0., 0., 951180.}},
mu2 -> {{969326., 0., 0.}, {0., 969321., 0.}, {0., 0., 659257.}},
me2 -> {{49272.2, 0., 0.}, {0., 49266.9, 0.}, {0., 0., 47778.5}},
MassB -> 209.358, MassWB -> 388.421, MassG -> 1117.18,
SCALE -> 879.186}
}
For each <model>
, the FS<model>CalculateObservables[handle]
function calculates further observables, such as effective Higgs
couplings to two photons or gluons. See the section on Observables
for a list of all available observables.
Note: The FS<model>CalculateObservables[handle]
function assumes,
that the pole mass spectrum has been calculated before, using the
FS<model>CalculateSpectrum[handle]
function.
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsModelParameters -> { m0 -> 125, m12 -> 500, TanBeta -> 10, SignMu -> 1 }
];
FSCMSSMCalculateSpectrum[handle]
FSCMSSMCalculateObservables[handle]
Output
{CMSSM ->
{ FlexibleSUSYObservable``CpHiggsPhotonPhoton ->
{0.0000296409 - 2.1245*10^-7 I, 7.82123*10^-7 + 9.1076*10^-7 I},
FlexibleSUSYObservable``CpHiggsGluonGluon ->
{-0.0000670724 - 2.65658*10^-6 I, 2.72135*10^-6 + 4.91993*10^-6 I},
FlexibleSUSYObservable``CpPseudoScalarPhotonPhoton ->
1.05105*10^-6 - 8.33068*10^-7 I,
FlexibleSUSYObservable``CpPseudoScalarGluonGluon ->
6.71448*10^-6 + 8.41625*10^-7 I }
}
After the spectrum has been calculated, one should check for problems
or warnings. They can be obtained for a given handle using the
FS<model>GetProblems[handle]
and FS<model>GetWarnings[handle]
functions, respectively. These functions return the empty list if no
problems / warnings occurred.
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsModelParameters -> { m0 -> 1000, m12 -> 500, Azero -> -10000, TanBeta -> 2, SignMu -> 1 }
];
FSCMSSMCalculateSpectrum[handle];
FSCMSSMGetProblems[handle]
Output
{CMSSM ->
{ Tachyons -> {M[Sd], M[Su]},
NoPoleMassConvergence -> {Pole[M[hh]]} }
}
This list of problems states, that the running up-type and down-type squarks are tachyonic for this parameter point. Thus, the spectrum calculated by FlexibleSUSY for this point cannot be trusted. Furthermore, the iteration to determine the Higgs pole mass did not converge. Thus, the calculated Higgs pole mass cannot be trusted either for this parameter point.
The running parameters, the mass spectrum and/or the observables can
be converted to SLHA format using the FS<model>ToSLHA[handle]
function. The function returns a string formatted according to
[SLHA1, SLHA2].
Example
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsModelParameters -> { m0 -> 1000, m12 -> 500, Azero -> 0, TanBeta -> 10, SignMu -> 1 }
];
FSCMSSMCalculateSpectrum[handle];
FSCMSSMCalculateObservables[handle];
Export["spectrum.slha", FSCMSSMToSLHA[handle], "String"];
Output: spectrum.slha
Block SPINFO 1 FlexibleSUSY 2 1.7.1 5 CMSSM 9 4.9.1 Block FlexibleSUSY 0 1.00000000E-04 # precision goal 1 0.00000000E+00 # max. iterations (0 = automatic) 2 0.00000000E+00 # algorithm (0 = two_scale) 3 0.00000000E+00 # calculate SM pole masses 4 2.00000000E+00 # pole mass loop order 5 2.00000000E+00 # EWSB loop order 6 3.00000000E+00 # beta-functions loop order 7 2.00000000E+00 # threshold corrections loop order 8 1.00000000E+00 # Higgs 2-loop corrections O(alpha_t alpha_s) 9 1.00000000E+00 # Higgs 2-loop corrections O(alpha_b alpha_s) 10 1.00000000E+00 # Higgs 2-loop corrections O((alpha_t + alpha_b)^2) 11 1.00000000E+00 # Higgs 2-loop corrections O(alpha_tau^2) 12 0.00000000E+00 # force output 13 1.00000000E+00 # Top pole mass QCD corrections (0 = 1L, 1 = 2L, 2 = 3L) 14 1.00000000E-11 # beta-function zero threshold 15 0.00000000E+00 # calculate observables (a_muon, ...) 16 0.00000000E+00 # force positive majorana masses 17 0.00000000E+00 # pole mass renormalization scale (0 = SUSY scale) 18 0.00000000E+00 # pole mass renormalization scale in the EFT (0 = min(SUSY scale, Mt)) 19 0.00000000E+00 # EFT matching scale (0 = SUSY scale) 20 2.00000000E+00 # EFT loop order for upwards matching 21 1.00000000E+00 # EFT loop order for downwards matching 22 0.00000000E+00 # EFT index of SM-like Higgs in the BSM model 23 1.00000000E+00 # calculate BSM pole masses Block SMINPUTS 1 1.27916000E+02 # alpha^(-1) SM MSbar(MZ) 2 1.16637000E-05 # G_Fermi 3 1.18400000E-01 # alpha_s(MZ) SM MSbar 4 9.11876000E+01 # MZ(pole) 5 4.18000000E+00 # mb(mb) SM MSbar 6 1.73340000E+02 # mtop(pole) 7 1.77700000E+00 # mtau(pole) 8 0.00000000E+00 # mnu3(pole) 9 8.03850000E+01 # MW(pole) 11 5.10998902E-04 # melectron(pole) 12 0.00000000E+00 # mnu1(pole) 13 1.05658372E-01 # mmuon(pole) 14 0.00000000E+00 # mnu2(pole) 21 4.75000000E-03 # md 22 2.40000000E-03 # mu 23 1.04000000E-01 # ms 24 1.27000000E+00 # mc Block FlexibleSUSYInput 0 7.29735257E-03 # alpha_em(0) 1 1.25090000E+02 # mh_pole Block MODSEL 6 0 # quark/lepton flavour violation 12 0.00000000E+00 # DRbar parameter output scale (GeV) Block MINPAR 1 1.00000000E+03 # m0 2 5.00000000E+02 # m12 3 1.00000000E+01 # TanBeta 4 1 # SignMu 5 0.00000000E+00 # Azero Block gauge Q= 1.08941472E+03 1 3.62448909E-01 # gY 2 6.41812871E-01 # g2 3 1.05659964E+00 # g3 Block Yu Q= 1.08941472E+03 1 1 7.21657623E-06 # Yu(1,1) 1 2 0.00000000E+00 # Yu(1,2) 1 3 0.00000000E+00 # Yu(1,3) 2 1 0.00000000E+00 # Yu(2,1) 2 2 3.28521207E-03 # Yu(2,2) 2 3 0.00000000E+00 # Yu(2,3) 3 1 0.00000000E+00 # Yu(3,1) 3 2 0.00000000E+00 # Yu(3,2) 3 3 8.57291451E-01 # Yu(3,3) Block Yd Q= 1.08941472E+03 1 1 1.38593672E-04 # Yd(1,1) 1 2 0.00000000E+00 # Yd(1,2) 1 3 0.00000000E+00 # Yd(1,3) 2 1 0.00000000E+00 # Yd(2,1) 2 2 3.03447401E-03 # Yd(2,2) 2 3 0.00000000E+00 # Yd(2,3) 3 1 0.00000000E+00 # Yd(3,1) 3 2 0.00000000E+00 # Yd(3,2) 3 3 1.31773557E-01 # Yd(3,3) Block Ye Q= 1.08941472E+03 1 1 2.86516322E-05 # Ye(1,1) 1 2 0.00000000E+00 # Ye(1,2) 1 3 0.00000000E+00 # Ye(1,3) 2 1 0.00000000E+00 # Ye(2,1) 2 2 5.92424993E-03 # Ye(2,2) 2 3 0.00000000E+00 # Ye(2,3) 3 1 0.00000000E+00 # Ye(3,1) 3 2 0.00000000E+00 # Ye(3,2) 3 3 9.96402101E-02 # Ye(3,3) Block Te Q= 1.08941472E+03 1 1 -8.51105194E-03 # TYe(1,1) 1 2 0.00000000E+00 # TYe(1,2) 1 3 0.00000000E+00 # TYe(1,3) 2 1 0.00000000E+00 # TYe(2,1) 2 2 -1.75978274E+00 # TYe(2,2) 2 3 0.00000000E+00 # TYe(2,3) 3 1 0.00000000E+00 # TYe(3,1) 3 2 0.00000000E+00 # TYe(3,2) 3 3 -2.94405366E+01 # TYe(3,3) Block Td Q= 1.08941472E+03 1 1 -1.88977041E-01 # TYd(1,1) 1 2 0.00000000E+00 # TYd(1,2) 1 3 0.00000000E+00 # TYd(1,3) 2 1 0.00000000E+00 # TYd(2,1) 2 2 -4.13759191E+00 # TYd(2,2) 2 3 0.00000000E+00 # TYd(2,3) 3 1 0.00000000E+00 # TYd(3,1) 3 2 0.00000000E+00 # TYd(3,2) 3 3 -1.68021836E+02 # TYd(3,3) Block Tu Q= 1.08941472E+03 1 1 -8.04938899E-03 # TYu(1,1) 1 2 0.00000000E+00 # TYu(1,2) 1 3 0.00000000E+00 # TYu(1,3) 2 1 0.00000000E+00 # TYu(2,1) 2 2 -3.66431893E+00 # TYu(2,2) 2 3 0.00000000E+00 # TYu(2,3) 3 1 0.00000000E+00 # TYu(3,1) 3 2 0.00000000E+00 # TYu(3,2) 3 3 -7.39719203E+02 # TYu(3,3) Block MSQ2 Q= 1.08941472E+03 1 1 1.92793919E+06 # mq2(1,1) 1 2 0.00000000E+00 # mq2(1,2) 1 3 0.00000000E+00 # mq2(1,3) 2 1 0.00000000E+00 # mq2(2,1) 2 2 1.92792577E+06 # mq2(2,2) 2 3 0.00000000E+00 # mq2(2,3) 3 1 0.00000000E+00 # mq2(3,1) 3 2 0.00000000E+00 # mq2(3,2) 3 3 1.46411510E+06 # mq2(3,3) Block MSE2 Q= 1.08941472E+03 1 1 1.02965849E+06 # me2(1,1) 1 2 0.00000000E+00 # me2(1,2) 1 3 0.00000000E+00 # me2(1,3) 2 1 0.00000000E+00 # me2(2,1) 2 2 1.02959546E+06 # me2(2,2) 2 3 0.00000000E+00 # me2(2,3) 3 1 0.00000000E+00 # me2(3,1) 3 2 0.00000000E+00 # me2(3,2) 3 3 1.01183185E+06 # me2(3,3) Block MSL2 Q= 1.08941472E+03 1 1 1.09811858E+06 # ml2(1,1) 1 2 0.00000000E+00 # ml2(1,2) 1 3 0.00000000E+00 # ml2(1,3) 2 1 0.00000000E+00 # ml2(2,1) 2 2 1.09808726E+06 # ml2(2,2) 2 3 0.00000000E+00 # ml2(2,3) 3 1 0.00000000E+00 # ml2(3,1) 3 2 0.00000000E+00 # ml2(3,2) 3 3 1.08926184E+06 # ml2(3,3) Block MSU2 Q= 1.08941472E+03 1 1 1.85944942E+06 # mu2(1,1) 1 2 0.00000000E+00 # mu2(1,2) 1 3 0.00000000E+00 # mu2(1,3) 2 1 0.00000000E+00 # mu2(2,1) 2 2 1.85943524E+06 # mu2(2,2) 2 3 0.00000000E+00 # mu2(2,3) 3 1 0.00000000E+00 # mu2(3,1) 3 2 0.00000000E+00 # mu2(3,2) 3 3 9.41968516E+05 # mu2(3,3) Block MSD2 Q= 1.08941472E+03 1 1 1.85122889E+06 # md2(1,1) 1 2 0.00000000E+00 # md2(1,2) 1 3 0.00000000E+00 # md2(1,3) 2 1 0.00000000E+00 # md2(2,1) 2 2 1.85121598E+06 # md2(2,2) 2 3 0.00000000E+00 # md2(2,3) 3 1 0.00000000E+00 # md2(3,1) 3 2 0.00000000E+00 # md2(3,2) 3 3 1.82729635E+06 # md2(3,3) Block Phases Q= 1.08941472E+03 1 1.00000000E+00 # Re(PhaseGlu) Block IMPhases Q= 1.08941472E+03 1 0.00000000E+00 # Im(PhaseGlu) Block MASS 1000021 1.19858229E+03 # Glu 24 8.03923382E+01 # VWm 1000024 3.92101428E+02 # Cha(1) 1000037 6.38758479E+02 # Cha(2) 25 1.15429842E+02 # hh(1) 35 1.20308783E+03 # hh(2) 37 1.20580267E+03 # Hpm(2) 36 1.20306748E+03 # Ah(2) 1000012 1.04330120E+03 # Sv(1) 1000014 1.04765714E+03 # Sv(2) 1000016 1.04767257E+03 # Sv(3) 1000022 2.07437446E+02 # Chi(1) 1000023 3.92113022E+02 # Chi(2) 1000025 -6.23279987E+02 # Chi(3) 1000035 6.38634777E+02 # Chi(4) 1000001 1.23941353E+03 # Sd(1) 1000003 1.38335815E+03 # Sd(2) 1000005 1.39207702E+03 # Sd(3) 2000001 1.39208249E+03 # Sd(4) 2000003 1.42196160E+03 # Sd(5) 2000005 1.42196587E+03 # Sd(6) 1000011 1.00717444E+03 # Se(1) 1000013 1.01697963E+03 # Se(2) 1000015 1.01701468E+03 # Se(3) 2000011 1.04734697E+03 # Se(4) 2000013 1.05094581E+03 # Se(5) 2000015 1.05095815E+03 # Se(6) 1000002 9.94140079E+02 # Su(1) 1000004 1.26241854E+03 # Su(2) 1000006 1.39428015E+03 # Su(3) 2000002 1.39428785E+03 # Su(4) 2000004 1.41992874E+03 # Su(5) 2000006 1.41993106E+03 # Su(6) Block UMIX 1 1 9.53292717E-01 # Re(UM(1,1)) 1 2 -3.02048004E-01 # Re(UM(1,2)) 2 1 3.02048004E-01 # Re(UM(2,1)) 2 2 9.53292717E-01 # Re(UM(2,2)) Block VMIX 1 1 9.78125635E-01 # Re(UP(1,1)) 1 2 -2.08015004E-01 # Re(UP(1,2)) 2 1 2.08015004E-01 # Re(UP(2,1)) 2 2 9.78125635E-01 # Re(UP(2,2)) Block PSEUDOSCALARMIX 1 1 -1.00061419E-01 # ZA(1,1) 1 2 9.94981262E-01 # ZA(1,2) 2 1 9.94981262E-01 # ZA(2,1) 2 2 1.00061419E-01 # ZA(2,2) Block DSQMIX 1 1 -0.00000000E+00 # ZD(1,1) 1 2 -0.00000000E+00 # ZD(1,2) 1 3 -9.99033786E-01 # ZD(1,3) 1 4 -0.00000000E+00 # ZD(1,4) 1 5 -0.00000000E+00 # ZD(1,5) 1 6 -4.39487765E-02 # ZD(1,6) 2 1 0.00000000E+00 # ZD(2,1) 2 2 0.00000000E+00 # ZD(2,2) 2 3 4.39487765E-02 # ZD(2,3) 2 4 0.00000000E+00 # ZD(2,4) 2 5 0.00000000E+00 # ZD(2,5) 2 6 -9.99033786E-01 # ZD(2,6) 3 1 0.00000000E+00 # ZD(3,1) 3 2 5.00403353E-03 # ZD(3,2) 3 3 0.00000000E+00 # ZD(3,3) 3 4 0.00000000E+00 # ZD(3,4) 3 5 9.99987480E-01 # ZD(3,5) 3 6 0.00000000E+00 # ZD(3,6) 4 1 2.28556802E-04 # ZD(4,1) 4 2 0.00000000E+00 # ZD(4,2) 4 3 0.00000000E+00 # ZD(4,3) 4 4 9.99999974E-01 # ZD(4,4) 4 5 0.00000000E+00 # ZD(4,5) 4 6 0.00000000E+00 # ZD(4,6) 5 1 0.00000000E+00 # ZD(5,1) 5 2 9.99987480E-01 # ZD(5,2) 5 3 0.00000000E+00 # ZD(5,3) 5 4 0.00000000E+00 # ZD(5,4) 5 5 -5.00403353E-03 # ZD(5,5) 5 6 0.00000000E+00 # ZD(5,6) 6 1 9.99999974E-01 # ZD(6,1) 6 2 0.00000000E+00 # ZD(6,2) 6 3 0.00000000E+00 # ZD(6,3) 6 4 -2.28556802E-04 # ZD(6,4) 6 5 0.00000000E+00 # ZD(6,5) 6 6 0.00000000E+00 # ZD(6,6) Block SELMIX 1 1 0.00000000E+00 # ZE(1,1) 1 2 0.00000000E+00 # ZE(1,2) 1 3 1.38267119E-01 # ZE(1,3) 1 4 0.00000000E+00 # ZE(1,4) 1 5 0.00000000E+00 # ZE(1,5) 1 6 9.90394974E-01 # ZE(1,6) 2 1 0.00000000E+00 # ZE(2,1) 2 2 -9.59493336E-03 # ZE(2,2) 2 3 0.00000000E+00 # ZE(2,3) 2 4 0.00000000E+00 # ZE(2,4) 2 5 -9.99953968E-01 # ZE(2,5) 2 6 0.00000000E+00 # ZE(2,6) 3 1 4.64326774E-05 # ZE(3,1) 3 2 0.00000000E+00 # ZE(3,2) 3 3 0.00000000E+00 # ZE(3,3) 3 4 9.99999999E-01 # ZE(3,4) 3 5 0.00000000E+00 # ZE(3,5) 3 6 0.00000000E+00 # ZE(3,6) 4 1 0.00000000E+00 # ZE(4,1) 4 2 0.00000000E+00 # ZE(4,2) 4 3 9.90394974E-01 # ZE(4,3) 4 4 0.00000000E+00 # ZE(4,4) 4 5 0.00000000E+00 # ZE(4,5) 4 6 -1.38267119E-01 # ZE(4,6) 5 1 0.00000000E+00 # ZE(5,1) 5 2 -9.99953968E-01 # ZE(5,2) 5 3 0.00000000E+00 # ZE(5,3) 5 4 0.00000000E+00 # ZE(5,4) 5 5 9.59493336E-03 # ZE(5,5) 5 6 0.00000000E+00 # ZE(5,6) 6 1 9.99999999E-01 # ZE(6,1) 6 2 0.00000000E+00 # ZE(6,2) 6 3 0.00000000E+00 # ZE(6,3) 6 4 -4.64326774E-05 # ZE(6,4) 6 5 0.00000000E+00 # ZE(6,5) 6 6 0.00000000E+00 # ZE(6,6) Block SCALARMIX 1 1 1.04543664E-01 # ZH(1,1) 1 2 9.94520298E-01 # ZH(1,2) 2 1 9.94520298E-01 # ZH(2,1) 2 2 -1.04543664E-01 # ZH(2,2) Block NMIX 1 1 9.95491987E-01 # Re(ZN(1,1)) 1 2 -1.79498849E-02 # Re(ZN(1,2)) 1 3 8.57113475E-02 # Re(ZN(1,3)) 1 4 -3.64289843E-02 # Re(ZN(1,4)) 2 1 4.08078351E-02 # Re(ZN(2,1)) 2 2 9.66067231E-01 # Re(ZN(2,2)) 2 3 -2.10338253E-01 # Re(ZN(2,3)) 2 4 1.44245090E-01 # Re(ZN(2,4)) 3 1 -3.37628172E-02 # Re(ZN(3,1)) 3 2 4.88174736E-02 # Re(ZN(3,2)) 3 3 7.03404869E-01 # Re(ZN(3,3)) 3 4 7.08306796E-01 # Re(ZN(3,4)) 4 1 7.86797123E-02 # Re(ZN(4,1)) 4 2 -2.52999529E-01 # Re(ZN(4,2)) 4 3 -6.73522809E-01 # Re(ZN(4,3)) 4 4 6.90049105E-01 # Re(ZN(4,4)) Block CHARGEMIX 1 1 -1.00190943E-01 # ZP(1,1) 1 2 9.94968228E-01 # ZP(1,2) 2 1 9.94968228E-01 # ZP(2,1) 2 2 1.00190943E-01 # ZP(2,2) Block USQMIX 1 1 0.00000000E+00 # ZU(1,1) 1 2 0.00000000E+00 # ZU(1,2) 1 3 2.45143979E-01 # ZU(1,3) 1 4 0.00000000E+00 # ZU(1,4) 1 5 7.81067721E-14 # ZU(1,5) 1 6 9.69486683E-01 # ZU(1,6) 2 1 0.00000000E+00 # ZU(2,1) 2 2 0.00000000E+00 # ZU(2,2) 2 3 -9.69486683E-01 # ZU(2,3) 2 4 0.00000000E+00 # ZU(2,4) 2 5 -3.08861911E-13 # ZU(2,5) 2 6 2.45143979E-01 # ZU(2,6) 3 1 0.00000000E+00 # ZU(3,1) 3 2 -1.04715235E-02 # ZU(3,2) 3 3 3.18616538E-13 # ZU(3,3) 3 4 0.00000000E+00 # ZU(3,4) 3 5 -9.99945172E-01 # ZU(3,5) 3 6 0.00000000E+00 # ZU(3,6) 4 1 2.30067962E-05 # ZU(4,1) 4 2 0.00000000E+00 # ZU(4,2) 4 3 0.00000000E+00 # ZU(4,3) 4 4 1.00000000E+00 # ZU(4,4) 4 5 0.00000000E+00 # ZU(4,5) 4 6 0.00000000E+00 # ZU(4,6) 5 1 0.00000000E+00 # ZU(5,1) 5 2 -9.99945172E-01 # ZU(5,2) 5 3 -3.33658350E-15 # ZU(5,3) 5 4 0.00000000E+00 # ZU(5,4) 5 5 1.04715235E-02 # ZU(5,5) 5 6 0.00000000E+00 # ZU(5,6) 6 1 1.00000000E+00 # ZU(6,1) 6 2 0.00000000E+00 # ZU(6,2) 6 3 0.00000000E+00 # ZU(6,3) 6 4 -2.30067962E-05 # ZU(6,4) 6 5 0.00000000E+00 # ZU(6,5) 6 6 0.00000000E+00 # ZU(6,6) Block SNUMIX 1 1 0.00000000E+00 # ZV(1,1) 1 2 0.00000000E+00 # ZV(1,2) 1 3 1.00000000E+00 # ZV(1,3) 2 1 0.00000000E+00 # ZV(2,1) 2 2 1.00000000E+00 # ZV(2,2) 2 3 0.00000000E+00 # ZV(2,3) 3 1 1.00000000E+00 # ZV(3,1) 3 2 0.00000000E+00 # ZV(3,2) 3 3 0.00000000E+00 # ZV(3,3) Block FlexibleSUSYOutput 0 2.04206021E+16 # HighScale 1 1.08941472E+03 # SUSYScale 2 9.11876000E+01 # LowScale Block FlexibleSUSYLowEnergy Q= 1.08941472E+03 21 2.25853630E-10 # Delta(g-2)_muon/2 FlexibleSUSY 1L Block EFFHIGGSCOUPLINGS 25 22 22 2.99452411E-05 # Abs(effective H-Photon-Photon coupling) 35 22 22 1.10853075E-06 # Abs(effective H-Photon-Photon coupling) 25 21 21 6.71211022E-05 # Abs(effective H-Gluon-Gluon coupling) 35 21 21 2.79047785E-06 # Abs(effective H-Gluon-Gluon coupling) 36 22 22 1.73035166E-06 # Abs(effective A-Photon-Photon coupling) 36 21 21 3.59315156E-06 # Abs(effective A-Gluon-Gluon coupling) Block ALPHA -1.04735039E-01 # ArcSin(Pole(ZH(2,2))) Block HMIX Q= 1.08941472E+03 1 6.15787614E+02 # Mu 2 9.64402142E+00 # vu/vd 3 2.43666046E+02 # Sqrt(Sqr(vd) + Sqr(vu)) 4 1.47855510E+06 # Sqr(MAh(2)) 101 1.51682262E+05 # BMu 102 2.51312780E+01 # vd 103 2.42366584E+02 # vu Block Au Q= 1.08941472E+03 1 1 -1.11540275E+03 # TYu(1,1)/Yu(1,1) 2 2 -1.11539799E+03 # TYu(2,2)/Yu(2,2) 3 3 -8.62856153E+02 # TYu(3,3)/Yu(3,3) Block Ad Q= 1.08941472E+03 1 1 -1.36353297E+03 # TYd(1,1)/Yd(1,1) 2 2 -1.36352854E+03 # TYd(2,2)/Yd(2,2) 3 3 -1.27508007E+03 # TYd(3,3)/Yd(3,3) Block Ae Q= 1.08941472E+03 1 1 -2.97052953E+02 # TYe(1,1)/Ye(1,1) 2 2 -2.97047351E+02 # TYe(2,2)/Ye(2,2) 3 3 -2.95468431E+02 # TYe(3,3)/Ye(3,3) Block MSOFT Q= 1.08941472E+03 1 2.10560904E+02 # MassB 2 3.89213480E+02 # MassWB 3 1.10405452E+03 # MassG 21 1.05177189E+06 # mHd2 22 -3.46241804E+05 # mHu2 31 1.04791153E+03 # SignedAbsSqrt(ml2(1,1)) 32 1.04789659E+03 # SignedAbsSqrt(ml2(2,2)) 33 1.04367708E+03 # SignedAbsSqrt(ml2(3,3)) 34 1.01472089E+03 # SignedAbsSqrt(me2(1,1)) 35 1.01468983E+03 # SignedAbsSqrt(me2(2,2)) 36 1.00589853E+03 # SignedAbsSqrt(me2(3,3)) 41 1.38850250E+03 # SignedAbsSqrt(mq2(1,1)) 42 1.38849767E+03 # SignedAbsSqrt(mq2(2,2)) 43 1.21000624E+03 # SignedAbsSqrt(mq2(3,3)) 44 1.36361630E+03 # SignedAbsSqrt(mu2(1,1)) 45 1.36361110E+03 # SignedAbsSqrt(mu2(2,2)) 46 9.70550625E+02 # SignedAbsSqrt(mu2(3,3)) 47 1.36059873E+03 # SignedAbsSqrt(md2(1,1)) 48 1.36059398E+03 # SignedAbsSqrt(md2(2,2)) 49 1.35177526E+03 # SignedAbsSqrt(md2(3,3))
When FlexibleSUSY is configured with --enable-verbose
, a lot of
additional debug output is written to stdout
and stderr
if
FlexibleSUSY is used at the command line. When the Mathematica
interface is used, this output is redirected to the notebook and
printed if form of messages of type FS<model>::info
, where <model>
is the model name.
By default, no more than three messages of the same type are witten to the notebook. In order to write all messages to the notebook, set
Off[General::stop];
The function, which writes the messages is called
FS<model>Message
and is defined as
FS<model>Message[s_] := Message[FS<model>::info, s]
where s
is the message string. If one would like to write the
messages to a file, the function can be re-defined to
FS<model>Message[s_] := WriteString["info.txt", s <> "\n"];
Example
Get["models/CMSSM/CMSSM_librarylink.m"];
handle = FSCMSSMOpenHandle[
fsModelParameters -> { m0 -> 125, m12 -> 500, TanBeta -> 10, SignMu -> 1 }
];
(* write all messages to "info.txt" *)
FSCMSSMMessage[s_] := WriteString["info.txt", s <> "\n"];
FSCMSSMCalculateSpectrum[handle]