NNLL-fast
is a computer program which computes the squark and gluino hadroproduction cross sections including approximate next-to-next-to-leading order (NNLOApprox) supersymmetric QCD corrections and the resummation of soft gluon emission at next-to-next-to-leading-logarithmic (NNLL) accuracy, including the resummation of Coulomb gluons with a NLO Coulomb potential and bound-state contributions below the production threshold. NNLL-fast
also provides an estimate of the theoretical uncertainty due to scale variation, the parton distribution functions, and the value of the strong coupling αs. The program reads in grid files with NLO and NNLOApprox+NNLL results, the scale uncertainty and the PDF and αs error and uses a fast interpolation routine to provide predictions for any value of squark and gluino masses in the mass ranges specified below. The results are provided for the latest LHC collision energy of 13.6 TeV for Run 3, and will be updated for future runs of the LHC. The predictions are created with the recent PDF4LHC21_40_pdfas PDF sets.
NNLL-fast
is the successor to NLL-fast
, the code which provided predictions at NLO+NLL accuracy for squark and gluino production with previous generations of PDF sets.
Separate versions of NNLL-fast for other models are also available:
NNLL-fast-MRSSM
for the calculation of squark-antisquark and squark-squark production in the Minimal R-symmetric Supersymmetric Standard Model (MRSSM) at NLO+(N)NLL accuracy,NNLL-fast-LQ
for the calculation of scalar leptoquark pair-production at NLO+NNLL accuracy.
NNLL-fast
is based on results obtained by many authors over the years. In alphabetical order, the contributions were provided by: Wim Beenakker, Silja Brensing-Thewes, Christoph Borschensky, Michael Krämer, Anna Kulesza, Eric Laenen, Laura Moreno Valero, Leszek Motyka, Irene Niessen, and Daniel Schwartländer. Additionally, NNLL-fast
uses NLO results obtained with Prospino. Therefore we ask to cite the following papers when referring to NNLL-fast
:
Squark and gluino production:
Stop (sbottom) production:
Squark production in the MRSSM:
NLO numbers for squark production in the MRSSM are obtained on the basis of:
Scalar Leptoquark pair production:
NLO cross sections with t-channel are calculated with the help of MadGraph5_aMC@NLO, please cite
NEW: NNLL-fast-MRSSM (LHC @ 13 TeV and LHC @ 13.6 TeV)
NNLL-fast-MRSSM
is run in the same way as NNLL-fast
, as described below, for the two implemented processes of squark-antisquark and squark-squark production, with the squark and gluino masses as an input.NNLL-fast-MRSSM
also outputs an uncertainty with respect to the variation of the sgluon mass from 100 TeV (central value) to 2 TeV.NEW: NNLL-fast, version 2.0 (LHC @ 13.6 TeV)
NNLL-fast-LQ (LHC @ 13 TeV)
NNLL-fast, version 1.1 (LHC @ 13 TeV)
NNLL-fast, version 1.0 (LHC @ 13 TeV)
NNLL-fast-LQ
is a python script that runs with python 2.7.X or python 3 with numpy and scipy.
NNLL-fast
is written in the Fortran programming language, so most Fortran compilers should be able to compile the code. One that it has been tested with is the free GNU Fortran compiler gfortran
. On a Linux terminal, the command to compile the code is:
$ gfortran nnllfast.f -o name_of_the_executable
where nnllfast.f
has to be replaced by the correct Fortran source file, depending on the version of NNLL-fast
.
NNLL-fast-LQ:
can be used in two different ways. NNLLfast_LQ.py
can be executed with command line arguments:
$ python NNLLfast_LQ.py PDF m
Here PDF
is the parton distribution function and can be either NNPDF31 or CT18. m
is the leptoquark mass in GeV between 500 GeV and 2300 GeV. The output is in this case written on screen.
NNLLfast_LQ.py
can also be executed without command line arguments:
$ python NNLLfast_LQ.py
In this case the script uses PDF and masses, which are defined in the script NNLLfast_LQ.py
. The default values can be edited to obtain the output for a list of masses between 500 GeV and 2300 GeV. The output is written in a file with default name output.out.
NNLL-fast:
After compiling nnllfast.f
, it should be called in the following way for all four squark and gluino production processes:
$ ./name_of_the_executable process squark_mass gluino_mass
or, for the case of stop-antistop (sbottom-antisbottom) production:
$ ./name_of_the_executable st stop_mass gluino_mass
The command line attribute process
can take the following values:
sb squark-antisquark production, ss squark-squark production, gg gluino-gluino production, sg squark-gluino production.
Ranges of gluino and squark masses (squark_mass, gluino_mass, stop_mass) are:
for gluino-pair production: 500 GeV <= gluino mass <= 3000 GeV and 500 GeV <= squark mass <= 3000 GeV, for squark-gluino production: 500 GeV <= gluino mass <= 3000 GeV and 500 GeV <= squark mass <= 3000 GeV, for squark-antisquark and squark-pair production: 500 GeV <= squark mass <= 3000 GeV and 500 GeV <= gluino mass <= 3000 GeV and for stop-antistop production: 100 GeV <= stop mass <= 3000 GeV and 500 GeV <= gluino mass <= 5000 GeV (other SUSY parameters: light flavour squark and stop 2 masses considered as very heavy, and stop mixing angle according to CMSSM benchmark point 40.2.5 as defined in arXiv:1109.3859.)
NNLL-fast:
# LHC @ 13.6 TeV, NNLO PDF4LHC21 (LHAPDF ID 93300) # process: sg # ms[GeV] mg[GeV] NLO[pb] NNLL+NNLO_app[pb] d_mu+[%] d_mu-[%] d_pdfas+[%] d_pdfas-[%] K_NNLL -------------------------------------------------------------------------------------------------------------- 1700. 2100. 0.733E-02 0.891E-02 3.69 -5.49 9.86 -9.86 1.21
NNLL-fast-MRSSM:
# LHC @ 13.6 TeV, NNLO PDF4LHC21 (LHAPDF ID 93300) # process: sb (in the MRSSM with msgluon = 100 TeV) # ms[GeV] mg[GeV] NLO[pb] NNLL+NNLO_app[pb] d_msgluon[%] d_mu+[%] d_mu-[%] d_pdfas+[%] d_pdfas-[%] K_NNLL ---------------------------------------------------------------------------------------------------------------------------- 1500. 1800. 0.467E-02 0.508E-02 2.93 3.70 -3.49 16.03 -16.03 1.09
NNLL-fast-LQ:
NNLLfast output for leptoquark pair production LHC @ 13 TeV, NNPDF31 mLQ = 1000.0 GeV NLO(QCD) = 5.237E-03 + 6.049E-04 - 7.102E-04 +- 1.990E-04 pb NLO(QCD)+NNLL = 5.436E-03 + 2.302E-05 - 2.302E-05 +- 2.011E-04 pb delta NNLL(mu=m) = 5.221E-04 pb delta NNLL(mu=m/2) = 1.912E-05 pb delta NNLL(mu=2m) = 1.201E-03 pb
The previous versions of NLL-fast
can be downloaded from here.
If you have questions, comments, or want to report a problem regarding the code, please contact Anna Kulesza or Christoph Borschensky.