On the usage of photon PDF by Syscalc
Dear developers
I have doubts how the photon PDF is handled in MG5_aMC_v2_3_3
I am calculating the photo-production of a spin-2 particle at LHC using the default RS model of MG.
I do:
define p = a
generate p p > y
The PDF I am trying are
NNPDF23_
NNPDF23_
CT14qed_proton
MRST2004qed_proton
In the run card I tried as beam: 1=proton, 2=photon from proton.
If I use beam = 2 I get a huge cross section (larger than gluglu>y), what cannot be,
If intead I use beam = 1 I get a reasonable behaved cross section, well behaved with m_y
For example LHC14, to m_y = 1 TeV
1: Cross-section : 9.87e-09 +- 1.528e-11 pb
2: Cross-section : 4.444e+18 +- 1.65e+10 pb
Up to here I could guess that the correct is use beam = 1 (just proton) and a PDF with QED part.
However when I use the Syscalc to calculate the alpha_s and PDF uncertainties I get as result alwyays:
The Syscalc.dat I use is
=======
# Central scale factors
scalefact:
1 2 0.5
# choice of correlation scheme between muF and muR
# set here to reproduce aMC@NLO order
#scalecorrelation:
0 3 6 1 4 7 2 5 8
# PDF sets and number of members (0 or none for all members)
PDF:
cteq6l1.LHgrid
NNPDF23_
NNPDF23_
NNPDF23_
CT10nlo.LHgrid
PDF4LHC15_
PDF4LHC15_
=======
scale fact cross-section :11 -nan
...
pdf reweighted cross-section :2 -nan
I explitly check that events are generated.
I am not sure what happens... Maybe I should specify something regarding photons to be in initial state in syscalc?
Could you advice me please?
thank you
Xanda
Question information
- Language:
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- Assignee:
- Alexis Kalogeropoulos Edit question
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