Plots from Rivet analyses
- Dijet invariant mass (D0_2010_S8566488)
- Dijet angular distributions (D0_2009_S8320160)
- Measurement of D0 Run II differential jet cross sections (D0_2008_S7662670)
- Run II jet azimuthal decorrelation analysis (D0_2004_S5992206)
- Dijet mass spectrum (CDF_2008_S8093652)
- CDF Run II inclusive jet cross-section using the Midpoint algorithm (CDF_2008_S7828950)
- CDF Run II $b$-jet shape paper (CDF_2008_S7782535)
- CDF Run II inclusive jet cross-section using the kT algorithm (CDF_2007_S7057202)
- Inclusive jet cross section differential in pT (CDF_2006_S6450792)
- Monte Carlo validation observables for jet production (MC_JETS)
Dijet invariant mass (D0_2010_S8566488)
Spires | arXiv:1002.4594
The inclusive dijet production double differential cross section as a function of the dijet invariant mass and of the largest absolute rapidity ($|y|_\text{max}$) of the two jets with the largest transverse momentum in an event is measured using 0.7 fb$^{-1}$ of data. The measurement is performed in six rapidity regions up to $|y|_\text{max}=2.4$.
Dijet angular distributions (D0_2009_S8320160)
Spires | arXiv:0906.4819 [hep-ex]
Dijet angular distributions in different bins of dijet mass from 0.25 TeV to above 1.1 TeV in $p \bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV, based on an integrated luminosity of 0.7 fb$^{-1}$.
Measurement of D0 Run II differential jet cross sections (D0_2008_S7662670)
Spires | Phys.Rev.Lett.101:062001,2008 | doi:10.1103/PhysRevLett.101.062001 | arXiv:0802.2400v3 [hep-ex]
Measurement of the inclusive jet cross section in $p \bar{p}$ collisions at center-of-mass energy sqrt(s) = 1.96 TeV. The data cover jet transverse momenta from 50--600 GeV and jet rapidities in the range -2.4 to 2.4.
Run II jet azimuthal decorrelation analysis (D0_2004_S5992206)
Spires | Phys. Rev. Lett., 94, 221801 (2005) | arXiv:hep-ex/0409040
Correlations in the azimuthal angle between the two largest pT jets have been measured using the D0 detector in ppbar collisions at 1960~GeV. The analysis is based on an inclusive dijet event sample in the central rapidity region. The correlations are determined for four different pT intervals.
Dijet mass spectrum (CDF_2008_S8093652)
Spires | arXiv:0812.4036 [hep-ex]
Dijet mass spectrum from 0.2 TeV to 1.4 TeV in $p \bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV, based on an integrated luminosity of 1.13 fb$^{-1}$.
CDF Run II inclusive jet cross-section using the Midpoint algorithm (CDF_2008_S7828950)
Spires | arXiv:0807.2204 | Phys.Rev.D78:052006,2008
Measurement of the inclusive jet cross section in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV as a function of jet $E_\perp$, for $E_\perp >$ 62 GeV. The data is collected by the CDF II detector and has an integrated luminosity of 1.13 fb$^{-1}$. The measurement was made using the cone-based Midpoint jet clustering algorithm in rapidity bins within $|y|<2.1$. This measurement can be used to provide increased precision in PDFs at high parton momentum fraction $x$.
CDF Run II $b$-jet shape paper (CDF_2008_S7782535)
Spires | arXiv:0806.1699 | Phys.Rev.D78:072005,2008
A measurement of the shapes of $b$-jets using 300 pb$^{-1}$ of data obtained with CDF II in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV. The measured quantity is the average integrated jet shape, which is computed over an ensemble of jets. This quantity is expressed as $\Psi(r/R) = \langle\frac{p_\perp(0 \rightarrow r)}{p_\perp(0 \rightarrow R)}\rangle$, where $p_\perp(0 \rightarrow r)$ is the scalar sum of the transverse momenta of all objects inside a sub-cone of radius $r$ around the jet axis. The integrated shapes are by definition normalized such that $\Psi(r/R =1) = 1$. The measurement is done in bins of jet pT in the range 52 to 300\;GeV/$c$. The jets have $|\eta| < 0.7$. The $b$-jets are expected to be broader than inclusive jets. Moreover, $b$-jets containing a single $b$-quark are expected to be narrower than those containing a $b \bar{b}$ pair from gluon splitting.
CDF Run II inclusive jet cross-section using the kT algorithm (CDF_2007_S7057202)
Spires | Phys.Rev.D75:092006,2007 | Erratum-ibid.D75:119901,2007 | FNAL-PUB 07/026-E | hep-ex/0701051
CDF Run II measurement of inclusive jet cross sections at a p-pbar collision energy of 1.96~TeV. Jets are reconstructed in the central part of the detector ($|y|<2.1$) using the kT algorithm with an $R$ parameter of 0.7. The minimum jet pT considered is 54~GeV, with a maximum around 700~GeV. The inclusive jet pT is plotted in bins of rapidity $|y|<0.1$, $0.1<|y|<0.7$, $0.7<|y|<1.1$, $1.1<|y|<1.6$ and $1.6<|y|<2.1$.
Inclusive jet cross section differential in pT (CDF_2006_S6450792)
Spires | Phys.Rev.D74:071103,2006 | doi:10.1103/PhysRevD.74.071103 | arXiv:hep-ex/0512020
Measurement of the inclusive jet cross section in ppbar interactions at $\sqrt{s}=1.96$ TeV using 385 $\mathrm{pb}^{-1}$ of data. The data cover the jet transverse momentum range from 61 to 620 GeV/c in $0.1 < |y| < 0.7$. This analysis has been updated with more data in more rapidity bins in CDF_2008_S7828950.
Monte Carlo validation observables for jet production (MC_JETS)
Jets with $p_\perp>20$ GeV are constructed with a $k_\perp$ jet finder with $D=0.7$ and projected onto many different observables.
