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fast pQCD calculations for hadron-induced processes
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LHC
pp @ LHC

Tevatron
pp-bar @ Tevatron

HERA
ep @ HERA

RHIC
pp @ RHIC


LHC: pp @ sqrt(s) = 13 TeV
fnl5662j_v23_fix_I1519995 CMS dijet angular 2015 (anti-kT R=0.4; Chi, Mjj); LO, NLO
fnl5662ja_v23_fix_I1519995 CMS dijet angular 2015 (anti-kT R=0.4; Chi, Mjj < 4.8 TeV); LO, NLO
inSPIRE HepData RIVET_ID: CMS_2017_I1519995
Validation plots: fnl5662ja NLO, normalised, Mjj < 4.8TeV
fnl5332g_v23_fix_I1459051 CMS inclusive jets 2015 (anti-kT R=0.7; pT, y); LO, NLO, NP
fnl5362g_v23_fix_I1459051 CMS inclusive jets 2015 (anti-kT R=0.4; pT, y); LO, NLO, NP
inSPIRE HepData RIVET_ID: CMS_2016_I1459051
Validation plots: fnl5332g NLO NLOxNP
Validation plots: fnl5362g NLO NLOxNP
LHC: pp @ sqrt(s) = 2.76 TeV
fnl4332_I1410826 CMS inclusive jets 2013 (anti-kT R=0.7; pT, y); LO, NLO
inSPIRE HepData RIVET_ID: Not yet available. Presumably: CMS_2015_I1410826
Validation plots: fnl4332 NLO
LHC: pp @ sqrt(s) = 8 TeV
fnl3332_I1487277 CMS inclusive jets 2012 (anti-kT R=0.7; pT, |y| < 3.0); LO, NLO
fnl3232e_I1487277_v23_fix CMS inclusive jets 2012 (anti-kT R=0.7; pT, 3.2 < |y| < 4.7); LO, NLO
inSPIRE HepData not yet available. RIVET_ID: Not yet available. Presumably: CMS_2017_I1410826
Validation plots to come after HepData are available. fnl3332
Validation plots to come after HepData are available. fnl3232e_I1487277_v23_fix
LHC: pp @ sqrt(s) = 7 TeV
fnl2332e_v23_fix_I1298810 CMS inclusive jets 2011 (anti-kT R=0.7; pT, y); LO, NLO, NP
fnl2342e_v23_fix_I1298810 CMS inclusive jets 2011 (anti-kT R=0.5; pT, y); LO, NLO, NP
inSPIRE HepData RIVET_ID: CMS_2014_I1298810
Validation plots: fnl2332e NLO NLOxNP NLOxNP(log x-axis)
Validation plots: fnl2342e NLO NLOxNP NLOxNP(log x-axis)
fnl2732numa_I1230937 CMS 3-jet ratio 2011, numerator (anti-kT R=0.7; pT_1,2); LO, NLO
fnl2732dena_I1230937 CMS 3-jet ratio 2011, denominator (anti-kT R=0.7; pT_1,2); LO, NLO
inSPIRE HepData no RIVET analysis available
fnl2332d_I1208923 CMS inclusive jets 2011 (anti-kT R=0.7; pT, y); LO, NLO
inSPIRE HepData RIVET_ID: CMS_2013_I1208923
Validation plots: fnl2332d NLO
fnl2412e_I1208923 CMS dijet mass 2011 (anti-kT R=0.7; Mjj, y_max); LO, NLO
inSPIRE HepData RIVET_ID: CMS_2013_I1208923
fnl2622f_I1090423 CMS dijet angular 2011 (anti-kT R=0.5; Chi, Mjj); LO, NLO
inSPIRE HepData RIVET_ID: CMS_2012_I1090423
(Note: The fastNLO table has been complemented with normalisation information [16.08.2017].
==> Normalised data and theory can be compared directly via YODA and Rivet
except for the highest mass bin, where the data binning is wider than the theory!)
Validation plots: fnl2622f normalised, NLO
fnl2222b_I1087342 CMS inclusive forward jets 2011 (anti-kT R=0.5; pT, eta); LO, NLO
inSPIRE HepData RIVET_ID: CMS_2012_I1087342
(Note: Unfortunately, the RIVET analysis mixes forward and forward+central jets all together into one analysis.)
fnl1016_I1082936 ATLAS inclusive jets 2010 (anti-kT R=0.4; pT, y); LO, NLO, THC-2loop
inSPIRE HepData RIVET_ID: ATLAS_2012_I1082936
(Note: Unfortunately, the RIVET analysis mixes all together, inclusive jets and dijet mass, and two jet sizes into one analysis.)
fnl1015_I1082936 ATLAS inclusive jets 2010 (anti-kT R=0.6; pT, y); LO, NLO, THC-2loop
inSPIRE HepData RIVET_ID: ATLAS_2012_I1082936
(Note: Unfortunately, the RIVET analysis mixes all together, inclusive jets and dijet mass, and two jet sizes into one analysis.)
fnl1014_I902309 CMS inclusive jets 2010 (anti-kT R=0.5; pT, y); LO, NLO, THC-2loop, NPC, Data
fnl1014_cv21_I902309 CMS inclusive jets 2010 (anti-kT R=0.5; pT, y); LO, NLO; NLOJet++-2.0.1 & fastNLO-1.4.0
inSPIRE HepData RIVET_ID: CMS_2011_S9086218
fnl2412c_I895742 CMS dijet mass 2010 (anti-kT R=0.7; pT, y_max)
inSPIRE HepData no RIVET analysis available



Daniel Britzger, Klaus Rabbertz, Georg Sieber, Fred Stober, Markus Wobisch
(send mail to the authors: fastnlo_at_projects.hepforge.org)

This work is supported by grant DE-SC0009859 from the U.S. Department of Energy. This work has received support within the project "Inclusive and Semi-Inclusive Constraints on the Parton Distributions at the LHC and the Study of Hard Processes" by the Helmholtz Alliance "Physics at the Terascale".

Last modified by rabbertz on: