Current Data¶
Pool: ATLAS_13_3L trileptons
ATLAS_2016_I1469071, Measurement of the $WZ$ production cross section at 13 TeV [4]
Pool: ATLAS_13_4L four leptons
ATLAS_2019_I1720442, Inclusive 4-lepton lineshape at 13 TeV [24]
ATLAS_2017_I1625109, Measurement of $ZZ -> 4ell$ production at 13 TeV [14]
Pool: ATLAS_13_EEJET e+e- at the Z pole, plus optional jets
ATLAS_2017_I1514251:LMODE=EL, Z plus jets at 13 TeV [11]
ATLAS_2019_I1718132:LMODE=ELEL, Control region measurements for leptoquark search at 13 TeV [26]
Pool: ATLAS_13_GAMMA Inclusive (multi)photons
ATLAS_2017_I1645627, Isolated photon + jets at 13 TeV [17]
Pool: ATLAS_13_JETS Inclusive hadronic final states
ATLAS_2018_I1634970, ATLAS Inclusive jet and dijet cross section measurement at sqrt(s)=13TeV [3]
ATLAS_2019_I1724098, Jet substructure at 13 TeV [23]
Pool: ATLAS_13_LL_GAMMA dilepton plus photon
ATLAS_2019_I1764342, Z(ll)y cross-section at 13 TeV [62]
Pool: ATLAS_13_LMETJET lepton, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
ATLAS_2018_I1656578, Differential $tbar{t}$ $l$+jets cross-sections at 13~TeV [20]
ATLAS_2017_I1614149, Resolved and boosted ttbar l+jets cross sections at 13 TeV [2]
ATLAS_2018_I1705857, ttbb at 13 TeV [25]
Pool: ATLAS_13_MMJET mu+mu- at the Z pole, plus optional jets
ATLAS_2017_I1514251:LMODE=MU, Z plus jets at 13 TeV [11]
ATLAS_2019_I1718132:LMODE=MUMU, Control region measurements for leptoquark search at 13 TeV [26]
Pool: ATLAS_13_TTHAD Fully hadronic top events
ATLAS_2018_I1646686, All-hadronic boosted ttbar at 13 TeV [19]
Pool: ATLAS_13_WW WW analyses in dilepton plus missing transverse momentum channel
ATLAS_2019_I1718132:LMODE=ELMU, Control region measurements for leptoquark search at 13 TeV [26]
ATLAS_2019_I1734263, WW production at 13 TeV [22]
Pool: ATLAS_7_4L four leptons
ATLAS_2012_I1203852:LMODE=LL, Measurement of the $ZZ(*)$ production cross-section in $pp$ collisions at 7 TeV with ATLAS [31]
Pool: ATLAS_7_EEJET e+e- at the Z pole, plus optional jets
ATLAS_2016_I1502620:LMODE=ZEL, W and Z inclusive cross sections at 7 TeV [12]
ATLAS_2013_I1230812:LMODE=EL, $Z$ + jets in $pp$ at 7 TeV [35]
ATLAS_2014_I1306294:LMODE=EL, Measurement of Z boson in association with b-jets at 7 TeV in ATLAS (electron channel) [38]
Pool: ATLAS_7_EE_GAMMA e+e- plus photon(s)
ATLAS_2013_I1217863:LMODE=ZEL, W/Z + gamma production at 7 TeV [36]
Pool: ATLAS_7_EMETJET electron, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
ATLAS_2013_I1219109:LMODE=EL, W + b production at 7 TeV [33]
ATLAS_2014_I1319490:LMODE=EL, W + jets [50]
ATLAS_2016_I1502620:LMODE=WEL, W and Z inclusive cross sections at 7 TeV [12]
Pool: ATLAS_7_EMET_GAMMA electron, missing transverse momentum, plus photon
ATLAS_2013_I1217863:LMODE=WEL, W/Z + gamma production at 7 TeV [36]
Pool: ATLAS_7_GAMMA Inclusive (multi)photons
ATLAS_2013_I1244522, Photon + jets [29]
ATLAS_2012_I1093738, Isolated prompt photon + jet cross-section [27]
ATLAS_2012_I1199269, Inclusive diphoton $+ X$ events at $sqrt{s} = 7$~TeV [32]
ATLAS_2013_I1263495, Inclusive isolated prompt photon analysis with 2011 LHC data [41]
Pool: ATLAS_7_HMDY Dileptons above the Z pole
ATLAS_2013_I1234228, High-mass Drell-Yan at 7 TeV [34]
Pool: ATLAS_7_JETS Inclusive hadronic final states
ATLAS_2014_I1307243, Measurements of jet vetoes and azimuthal decorrelations in dijet events produced in pp collisions at $sqrt{s}$ = 7 TeV using the ATLAS detector [45]
ATLAS_2014_I1326641, 3-jet cross section with 7 TeV data [49]
ATLAS_2014_I1325553, Measurement of the inclusive jet cross-section at 7 TeV [48]
ATLAS_2014_I1268975, High-mass dijet cross section [39]
Pool: ATLAS_7_LLMET dilepton+MET
ATLAS_2012_I1203852:LMODE=LNU, Measurement of the $ZZ(*)$ production cross-section in $pp$ collisions at 7 TeV with ATLAS [31]
Pool: ATLAS_7_LMDY Dileptons below the Z pole
ATLAS_2014_I1288706, Measurement of the low-mass Drell-Yan differential cross section at 7 TeV [42]
Pool: ATLAS_7_LMETJET lepton, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
ATLAS_2014_I1282447, W + charm production at 7 TeV [43]
ATLAS_2015_I1345452, Pseudo-top-antitop cross sections [46]
Pool: ATLAS_7_MMETJET muon, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
ATLAS_2013_I1219109:LMODE=MU, W + b production at 7 TeV [33]
ATLAS_2014_I1319490:LMODE=MU, W + jets [50]
ATLAS_2016_I1502620:LMODE=WMU, W and Z inclusive cross sections at 7 TeV [12]
Pool: ATLAS_7_MMET_GAMMA muon, missing transverse momentum, plus photon
ATLAS_2013_I1217863:LMODE=WMU, W/Z + gamma production at 7 TeV [36]
Pool: ATLAS_7_MMJET mu+mu- at the Z pole, plus optional jets
ATLAS_2014_I1306294:LMODE=MU, Measurement of Z boson in association with b-jets at 7 TeV in ATLAS (electron channel) [38]
ATLAS_2016_I1502620:LMODE=ZMU, W and Z inclusive cross sections at 7 TeV [12]
ATLAS_2013_I1230812:LMODE=MU, $Z$ + jets in $pp$ at 7 TeV [35]
Pool: ATLAS_7_MM_GAMMA mu+mu- plus photon(s)
ATLAS_2013_I1217863:LMODE=ZMU, W/Z + gamma production at 7 TeV [36]
Pool: ATLAS_7_WW WW analyses in dilepton plus missing transverse momentum channel
ATLAS_2013_I1190187, Measurement of the $W^+ W^-$ production cross-section at 7 TeV [30]
Pool: ATLAS_8_3L trileptons
ATLAS_2016_I1492320:LMODE=3L, WWW production at 8 TeV [13]
Pool: ATLAS_8_4L four leptons
ATLAS_2015_I1394865, Inclusive 4-lepton lineshape [58]
ATLAS_2014_I1310835, H(125) -> 4l at 8 TeV [37]
Pool: ATLAS_8_EEJET e+e- at the Z pole, plus optional jets
ATLAS_2017_I1589844:LMODE=EL, $k_T$ splittings in $Z$ events at 8 TeV [7]
ATLAS_2015_I1408516:LMODE=EL, $Z$ $p_T$ and $Z$ $phi^*$ [55]
ATLAS_2019_I1744201, Z+jet at 8 TeV [60]
Pool: ATLAS_8_EMETJET electron, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
ATLAS_2018_I1635273:LMODE=EL, W + jets production at 8 TeV [15]
ATLAS_2017_I1517194:LMODE=EL, Electroweak $Wjj$ production at 8~TeV [9]
Pool: ATLAS_8_GAMMA Inclusive (multi)photons
ATLAS_2017_I1591327, Inclusive diphoton cross-sections at 8 TeV [10]
ATLAS_2017_I1632756, Photon + heavy flavour at 8 TeV [16]
ATLAS_2016_I1457605, Inclusive prompt photons at 8 TeV [54]
ATLAS_2017_I1644367, Isolated triphotons at 8 TeV [18]
Pool: ATLAS_8_GAMMA_MET photon plus missing transverse momentum
ATLAS_2016_I1448301:LMODE=NU, $Z gamma (gamma)$ cross sections at 8 TeV [57]
Pool: ATLAS_8_HMDY_EL Dileptons above the Z pole
ATLAS_2016_I1467454:LMODE=EL, High-mass Drell-Yan at 8 TeV [53]
Pool: ATLAS_8_HMDY_MU Dileptons above the Z pole
ATLAS_2016_I1467454:LMODE=MU, High-mass Drell-Yan at 8 TeV [53]
Pool: ATLAS_8_JETS Inclusive hadronic final states
ATLAS_2015_I1394679, Multijets at 8 TeV [47]
ATLAS_2017_I1604271, ATLAS Inclusive jet cross section measurement at sqrt(s)=8TeV [8]
ATLAS_2017_I1598613:BMODE=3MU, BB to Jpsi plus mu at 8 TeV [1]
Pool: ATLAS_8_LLJET dileptons at the Z pole, plus optional jets
ATLAS_2014_I1279489, Measurements of electroweak production of dijets + $Z$ boson, and distributions sensitive to vector boson fusion [40]
Pool: ATLAS_8_LMETJET lepton, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
ATLAS_2015_I1404878, ttbar (to l+jets) differential cross sections at 8 TeV [59]
ATLAS_2015_I1397637, Boosted ttbar differential cross-section [52]
Pool: ATLAS_8_MMETJET muon, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
ATLAS_2017_I1517194:LMODE=MU, Electroweak $Wjj$ production at 8~TeV [9]
ATLAS_2018_I1635273:LMODE=MU, W + jets production at 8 TeV [15]
Pool: ATLAS_8_MMJET mu+mu- at the Z pole, plus optional jets
ATLAS_2017_I1589844:LMODE=MU, $k_T$ splittings in $Z$ events at 8 TeV [7]
ATLAS_2015_I1408516:LMODE=MU, $Z$ $p_T$ and $Z$ $phi^*$ [55]
Pool: ATLAS_8_MM_GAMMA mu+mu- plus photon(s)
ATLAS_2016_I1448301:LMODE=LL, $Z gamma (gamma)$ cross sections at 8 TeV [57]
Pool: ATLAS_8_WW WW analyses in dilepton plus missing transverse momentum channel
ATLAS_2016_I1426515, WW production at 8 TeV [56]
ATLAS_2016_I1492320:LMODE=2L2J, WWW production at 8 TeV [13]
Pool: CMS_13_EEJET dileptons at the Z pole, plus optional jets
CMS_2018_I1667854:LMODE=EL, Differential cross section of Z boson production in association with jets in proton-proton collisions at $sqrt{s} = 13,$TeV [138]
CMS_2019_I1753680:LMODE=EL, Measurements of differential Z boson production cross sections in proton-proton collisions at 13 TeV [142]
Pool: CMS_13_HMDY Dileptons above the Z pole
CMS_2018_I1711625, Measurement of the differential Drell-Yan cross section in proton-proton collisions at $sqrt{s} = 13,TeV$ [141]
Pool: CMS_13_JETS Inclusive hadronic final states
CMS_2018_I1682495, Jet mass in dijet events in $pp$ collisions at 13~TeV [143]
CMS_2016_I1459051, Measurement of the inclusive jet cross-section in $pp$ collisions at $sqrt{s} = 13;TeV$ [122]
Pool: CMS_13_LMETJET lepton, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
CMS_2018_I1663958, Differential cross sections for top quark pair production using the lepton+jets final state in proton proton collisions at 13 TeV [139]
CMS_2016_I1491950, Differential cross sections for top quark pair production using the lepton+jets final state in proton proton collisions at 13 TeV [125]
CMS_2018_I1662081, Measurement of the differential cross sections of top quark pair production as a function of kinematic event variables in pp collisions at sqrt(s) = 13 TeV [134]
Pool: CMS_13_MMETJET muon, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
CMS_2019_I1705068, Measurement of associated production of a W boson and a charm quark in proton-proton collisions at 13 TeV [140]
CMS_2017_I1610623, Measurements of differential cross sections for the associated production of a W boson and jets in proton-proton collisions at sqrt(s) = 13 TeV [135]
Pool: CMS_13_MMJET dileptons at the Z pole, plus optional jets
CMS_2018_I1667854:LMODE=MU, Differential cross section of Z boson production in association with jets in proton-proton collisions at $sqrt{s} = 13,$TeV [138]
CMS_2019_I1753680:LMODE=MU, Measurements of differential Z boson production cross sections in proton-proton collisions at 13 TeV [142]
Pool: CMS_7_EEJET e+e- at the Z pole, plus optional jets
CMS_2013_I1224539:JMODE=Z, CMS jet mass measurement in $W, Z$ and dijet events [96]
Pool: CMS_7_EMETJET electron, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
CMS_2013_I1224539:JMODE=W, CMS jet mass measurement in $W, Z$ and dijet events [96]
Pool: CMS_7_GAMMA Inclusive (multi)photons
CMS_2014_I1266056, Photon + jets triple differential cross-section [99]
Pool: CMS_7_JETS Inclusive hadronic final states
CMS_2014_I1298810, Ratios of jet pT spectra, which relate to the ratios of inclusive, differential jet cross sections [98]
CMS_2013_I1273574, Studies of 4-jet production in proton-proton collisions at $sqrt{s} = 7$ TeV [97]
CMS_2013_I1208923, Jet-pT and dijet mass at sqrt(s) = 7 TeV [95]
Pool: CMS_7_LLJET dileptons at the Z pole, plus optional jets
CMS_2013_I1256943, Cross-section and angular correlations in $Z$ boson with $b$-hadrons events at $sqrt{s} = 7$ TeV [94]
CMS_2015_I1310737, Jet multiplicity and differential cross-sections of $Z$+jets events in $pp$ at $sqrt{s} = 7$ TeV [121]
Pool: CMS_7_MMETJET muon, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
CMS_2014_I1303894, Differential cross-section of $W$ bosons + jets in $pp$ collisions at $sqrt{s}=7$ TeV [120]
Pool: CMS_8_3L trileptons
CMS_2016_I1487288, $WZ$ production cross-section in $pp$ collisions at 8~TeV [118]
Pool: CMS_8_JETS Inclusive hadronic final states
CMS_2017_I1598460, Triple-differential dijet pT cross section and PDF constraints at 8 TeV [137]
CMS_2016_I1487277, Measurement and QCD analysis of double-differential inclusive jet cross sections in $pp$ collisions at $sqrt{s} = 8;TeV$ and cross-section ratios to 2.76 and 7 TeV [124]
Pool: CMS_8_LLJET dileptons at the Z pole, plus optional jets
CMS_2017_I1499471, Measurements of the associated production of a Z boson and b jets in pp collisions at $sqrt{s} = 8$ TeV [119]
Pool: CMS_8_LMETJET lepton, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
CMS_2016_I1454211, Boosted $tbar{t}$ in $pp$ collisions at $sqrt{s} = 8~TeV$ [123]
CMS_2017_I1518399, Differential $tbar{t}$ production cross-section as a function of the leading jet mass for boosted top quarks at 8 TeV [136]
Pool: CMS_8_MMETJET muon, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
CMS_2016_I1491953, Differential cross sections for associated production of a W boson and jets at 8 TeV [127]
Pool: LHCB_7_EEJET e+e- at the Z pole, plus optional jets
LHCB_2012_I1208102, Differential cross-sections of $mathrm{Z}/gamma^* to e^{+}e^{-}$ vs rapidity and $phi^*$ [63]
Pool: LHCB_7_MMJET mu+mu- at the Z pole, plus optional jets
LHCB_2014_I1262703, Study of forward Z + jet production in $pp$ collisions at $sqrt{s}=7$ TeV in the LHCb fiducial phase-space [64]
Ratio measurements¶
These typically use SM theory for the denominator, and may give unreliable results if your model contributes to both numerator and denominator. On by default, can be turned off via command-line.
Pool: ATLAS_13_METJET missing transverse momentum plus jets
ATLAS_2017_I1609448, $p_T^text{miss}$+jets cross-section ratios at 13 TeV [6]
Higgs to diphotons¶
Higgs to two photons use a data-driven background subtraction. If your model predicts non-resonant photon production this may lead to unreliable results. On by default, can be turned off via command-line.
Pool: ATLAS_8_GAMMA Inclusive (multi)photons
ATLAS_2014_I1306615, Higgs diphoton events at 8 TeV in ATLAS [44]
Searches¶
Detector-level, using Rivet smearing functions. Off by default, can be turned on via command-line.
Pool: ATLAS_13_HMDY Dileptons above the Z pole
ATLAS_2019_I1725190, Dilepton mass spectrum in 13 TeV pp collisions with 139/fb Run 2 dataset [61]
Pool: ATLAS_13_METJET missing transverse momentum plus jets
ATLAS_2016_I1458270, 0-lepton SUSY search with 3.2/fb of 13 TeV $pp$ data [5]
Higgs to WW¶
Typically involve large data-driven top background subtraction. If your model contributes to the background as well the results maybe unreliable. Off by default, can be turned on via command-line.
Pool: ATLAS_8_WW WW analyses in dilepton plus missing transverse momentum channel
ATLAS_2016_I1444991, Higgs-to-WW differential cross sections at 8 TeV [51]
Pool: CMS_8_WW WW analyses in dilepton plus missing transverse momentum channel
CMS_2017_I1467451, Measurement of the transverse momentum spectrum of the Higgs boson produced in $pp$collisions at $sqrt{s} = 8$ TeV using H to WW decays [126]
b-jet veto issue¶
The following measurements apply a detector-level b-jet veto which is not part of the particle-level fiducial definition and therefore not applied in Rivet. Also applies to CMS Higgs-to-WW analysis. Off by default, can be turned on via command-line, but use with care.
Pool: CMS_13_MMETJET muon, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
CMS_2017_I1610623, Measurements of differential cross sections for the associated production of a W boson and jets in proton-proton collisions at sqrt(s) = 13 TeV [135]
Pool: CMS_7_MMETJET muon, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
CMS_2014_I1303894, Differential cross-section of $W$ bosons + jets in $pp$ collisions at $sqrt{s}=7$ TeV [120]
Pool: CMS_8_MMETJET muon, missing transverse momentum, plus optional jets (typically W, semi-leptonic ttbar analyses)
CMS_2016_I1491953, Differential cross sections for associated production of a W boson and jets at 8 TeV [127]
Pool: CMS_8_WW WW analyses in dilepton plus missing transverse momentum channel
CMS_2017_I1467451, Measurement of the transverse momentum spectrum of the Higgs boson produced in $pp$collisions at $sqrt{s} = 8$ TeV using H to WW decays [126]