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Plots from Rivet analyses

Precise study of Z pT using novel technique (D0_2010_S8821313)

Spires | arXiv:1010.0262

Using 7.3 pb-1 the distribution of the variable $\phi^*$ is measured, which probes the same physical effects as the $Z/\gamma^*$ boson transverse momentum, but is less susceptible to the effects of experimental resolution and efficiency. Results are presented for both the di-electron and di-muon channel.

D0_2010_S8821313/d01-x01-y01.pdf:
D0_2010_S8821313/d01-x01-y02.pdf:
D0_2010_S8821313/d01-x01-y03.pdf:
D0_2010_S8821313/d02-x01-y01.pdf:
D0_2010_S8821313/d02-x01-y02.pdf:

Measurement of differential $Z/\gamma^*$ pT (D0_2010_S8671338)

Spires | arXiv:1006.0618 [hep-ex]

Cross section as a function of pT of the Z boson decaying into muons in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 0.97 fb$^{-1}$.

D0_2010_S8671338/d01-x01-y01.pdf:
D0_2010_S8671338/d02-x01-y01.pdf:

Z+jets angular distributions (D0_2009_S8349509)

Spires | arXiv:0907.4286 [hep-ex]

First measurements at a hadron collider of differential cross sections for $Z (\to \mu\mu)$+jet+X production in $\Delta\phi(Z, j)$, $|\Delta y(Z, j)|$ and $|y_\mathrm{boost}(Z, j)|$. Vector boson production in association with jets is an excellent probe of QCD and constitutes the main background to many small cross section processes, such as associated Higgs production. These measurements are crucial tests of the predictions of perturbative QCD and current event generators, which have varied success in describing the data. Using these measurements as inputs in tuning event generators will increase the experimental sensitivity to rare signals.

D0_2009_S8349509/d01-x01-y01.pdf:
D0_2009_S8349509/d01-x01-y02.pdf:
D0_2009_S8349509/d02-x01-y01.pdf:
D0_2009_S8349509/d02-x01-y02.pdf:
D0_2009_S8349509/d03-x01-y01.pdf:
D0_2009_S8349509/d03-x01-y02.pdf:
D0_2009_S8349509/d04-x01-y01.pdf:
D0_2009_S8349509/d04-x01-y02.pdf:
D0_2009_S8349509/d05-x01-y01.pdf:
D0_2009_S8349509/d05-x01-y02.pdf:
D0_2009_S8349509/d06-x01-y01.pdf:
D0_2009_S8349509/d06-x01-y02.pdf:

$Z/\gamma^*$ + jet + $X$ cross sections differential in pT(jet 1,2,3) (D0_2009_S8202443)

Spires | arXiv:0903.1748 [hep-ex]

Cross sections as a function of pT of the three leading jets in $Z/\gamma^{*} (\to e^{+} e^{-})$ + jet + X production in $p \bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV, based on an integrated luminosity of 1.0 fb$^{-1}$.

D0_2009_S8202443/d01-x01-y01.pdf:
D0_2009_S8202443/d02-x01-y01.pdf:
D0_2009_S8202443/d03-x01-y01.pdf:
D0_2009_S8202443/d04-x01-y01.pdf:
D0_2009_S8202443/d05-x01-y01.pdf:
D0_2009_S8202443/d06-x01-y01.pdf:

Measurement of differential $Z/\gamma^*$ + jet + $X$ cross sections (D0_2008_S7863608)

Spires | Phys.Lett. B669 (2008) 278-286 | doi:10.1016/j.physletb.2008.09.060 | arXiv:0808.1296 [hep-ex]

Cross sections as a function of pT and rapidity of the boson and pT and rapidity of the leading jet in the di-muon channel in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 1.0 fb$^{-1}$.

D0_2008_S7863608/d01-x01-y01.pdf:
D0_2008_S7863608/d01-x01-y02.pdf:
D0_2008_S7863608/d02-x01-y01.pdf:
D0_2008_S7863608/d02-x01-y02.pdf:
D0_2008_S7863608/d03-x01-y01.pdf:
D0_2008_S7863608/d03-x01-y02.pdf:
D0_2008_S7863608/d04-x01-y01.pdf:
D0_2008_S7863608/d04-x01-y02.pdf:
D0_2008_S7863608/d05-x01-y01.pdf:

$Z/\gamma^* + X$ cross-section shape, differential in $pT(Z)$ (D0_2008_S7554427)

Spires | arXiv:0712.0803

Cross sections as a function of pT of the vector boson inclusive and in forward region ($|y| > 2$, $pT<30$ GeV) in the di-electron channel in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of 0.98~fb$^{-1}$.

D0_2008_S7554427/d01-x01-y01.pdf:
D0_2008_S7554427/d03-x01-y01.pdf:

Measurement of the ratio sigma($Z/\gamma^*$ + $n$ jets)/sigma($Z/\gamma^*$) (D0_2008_S6879055)

Spires | hep-ex/0608052

Cross sections as a function of pT of the three leading jets and $n$-jet cross section ratios in $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of $0.4~\text{fb}^{-1}$.

D0_2008_S6879055/d01-x01-y01.pdf:
D0_2008_S6879055/d02-x01-y01.pdf:
D0_2008_S6879055/d03-x01-y01.pdf:
D0_2008_S6879055/d04-x01-y01.pdf:

$Z/\gamma^* + X$ cross-section shape, differential in $y(Z)$ (D0_2007_S7075677)

Spires | Phys.Rev.D76:012003,2007 | arXiv:hep-ex/0702025

Cross sections as a function of di-electron rapidity $p \bar{p}$ collisions at $\sqrt{s}$ = 1.96 TeV, based on an integrated luminosity of $0.4~\text{fb}^{-1}$.

D0_2007_S7075677/d01-x01-y01.pdf:

Measurement of differential Z/$\gamma^*$ + jet + X cross sections (CDF_2008_S7540469)

Spires | Phys.Rev.Lett.100:102001,2008 | arXiv:0711.3717 [hep-ex]

Cross sections as a function of jet transverse momentum in 1 and 2 jet events, and jet multiplicity in ppbar collisions at sqrt(s) = 1.96 TeV, based on an integrated luminosity of $1.7~\text{fb}^{-1}$. The measurements cover the rapidity region $|y_\text{jet}| < 2.1$ and the transverse momentum range $pT^\text{jet} > 30~\text{GeV}/c$.

CDF_2008_S7540469/d01-x01-y01.pdf:
CDF_2008_S7540469/d02-x01-y01.pdf:
CDF_2008_S7540469/d03-x01-y01.pdf:

Monte Carlo validation observables for $Z[e^+ \, e^-]$ + jets production (MC_ZJETS)

Available observables are Z mass, pT of jets 1-4, jet multiplicity, $\Delta\eta(Z, \text{jet1})$, $\Delta R(\text{jet2}, \text{jet3})$, differential jet rates 0->1, 1->2, 2->3, 3->4, integrated 0--4 jet rates.

MC_ZJETS/Z_jet1_dR.pdf:
MC_ZJETS/Z_jet1_deta.pdf:
MC_ZJETS/Z_mass.pdf:
MC_ZJETS/Z_pT.pdf:
MC_ZJETS/Z_pT_peak.pdf:
MC_ZJETS/Z_phi.pdf:
MC_ZJETS/Z_y.pdf:
MC_ZJETS/jet_eta_1.pdf:
MC_ZJETS/jet_eta_2.pdf:
MC_ZJETS/jet_eta_3.pdf:
MC_ZJETS/jet_eta_4.pdf:
MC_ZJETS/jet_eta_pmratio_1.pdf:
MC_ZJETS/jet_eta_pmratio_2.pdf:
MC_ZJETS/jet_eta_pmratio_3.pdf:
MC_ZJETS/jet_eta_pmratio_4.pdf:
MC_ZJETS/jet_mass_1.pdf:
MC_ZJETS/jet_mass_2.pdf:
MC_ZJETS/jet_mass_3.pdf:
MC_ZJETS/jet_mass_4.pdf:
MC_ZJETS/jet_multi_exclusive.pdf:
MC_ZJETS/jet_multi_inclusive.pdf:
MC_ZJETS/jet_multi_ratio.pdf:
MC_ZJETS/jet_pT_1.pdf:
MC_ZJETS/jet_pT_2.pdf:
MC_ZJETS/jet_pT_3.pdf:
MC_ZJETS/jet_pT_4.pdf:
MC_ZJETS/jet_y_1.pdf:
MC_ZJETS/jet_y_2.pdf:
MC_ZJETS/jet_y_3.pdf:
MC_ZJETS/jet_y_4.pdf:
MC_ZJETS/jet_y_pmratio_1.pdf:
MC_ZJETS/jet_y_pmratio_2.pdf:
MC_ZJETS/jet_y_pmratio_3.pdf:
MC_ZJETS/jet_y_pmratio_4.pdf:
MC_ZJETS/jets_dR_12.pdf:
MC_ZJETS/jets_dR_13.pdf:
MC_ZJETS/jets_dR_14.pdf:
MC_ZJETS/jets_dR_23.pdf:
MC_ZJETS/jets_dR_24.pdf:
MC_ZJETS/jets_dR_34.pdf:
MC_ZJETS/jets_deta_12.pdf:
MC_ZJETS/jets_deta_13.pdf:
MC_ZJETS/jets_deta_14.pdf:
MC_ZJETS/jets_deta_23.pdf:
MC_ZJETS/jets_deta_24.pdf:
MC_ZJETS/jets_deta_34.pdf:
MC_ZJETS/lepton_eta.pdf:
MC_ZJETS/lepton_pT.pdf:
MC_ZJETS/log10_R_0.pdf:
MC_ZJETS/log10_R_1.pdf:
MC_ZJETS/log10_R_2.pdf:
MC_ZJETS/log10_R_3.pdf:
MC_ZJETS/log10_R_4.pdf:
MC_ZJETS/log10_d_01.pdf:
MC_ZJETS/log10_d_12.pdf:
MC_ZJETS/log10_d_23.pdf:
MC_ZJETS/log10_d_34.pdf:

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