Showing 10 of 2127 results
A measurement of the cross-section for Z-boson production in the forward region of pp collisions at 8TeV centre-of-mass energy is presented. The measurement is based on a sample of $\rm Z\rightarrow e^+e^-$ decays reconstructed using the LHCb detector, corresponding to an integrated luminosity of 2.0fb$^{-1}$. The acceptance is defined by the requirements $2.0<\eta<4.5$ and $p_{\rm T}>20$GeV for the pseudorapidities and transverse momenta of the leptons. Their invariant mass is required to lie in the range 60--120GeV. The cross-section is determined to be $$ \sigma({\rm pp\to Z\to e^+e^-})=93.81\pm0.41({\rm stat})\pm1.48({\rm syst})\pm1.14({\rm lumi})\;{\rm pb}\,,$$ where the first uncertainty is statistical and the second reflects all systematic effects apart from that arising from the luminosity, which is given as the third uncertainty. Differential cross-sections are presented as functions of the Z-boson rapidity and of the angular variable $\phi^*$, which is related to the Z-boson transverse momentum.
Integrated cross-section for Z$\to$ e$^+$e$^-$ within the LHCb acceptance.
Differential cross-section for Z$\to$ e$^+$e$^-$ as a function of Z-boson rapidity. The first error is statistical, the second the uncorrelated experimental systematic, the third the correlated experimental systematic and the last error is the uncertainty in luminosity. The cross-sections are at the Born level, i.e. before FSR. The rightmost column gives values of the additional factor, $f_{\rm FSR}$, by which the results should be multiplied in order to give the cross-sections after FSR.
Differential cross-section for Z$\to$ e$^+$e$^-$ as a function of $\phi^*$. The first error is statistical, the second the uncorrelated experimental systematic, the third the correlated experimental systematic and the last error is the uncertainty in luminosity. The cross-sections are at the Born level, i.e. before FSR. The rightmost column gives values of the additional factor, $f_{\rm FSR}$, by which the results should be multiplied in order to give the cross-sections after FSR.
Forward top quark pair production is studied in $pp$ collisions in the $\mu eb$ final state using a data sample corresponding to an integrated luminosity of 1.93 fb$^{-1}$ collected with the LHCb experiment at a centre-of-mass energy of 13 TeV. The cross-section is measured in a fiducial region where both leptons have a transverse momentum greater than 20 GeV and a pseudorapidity between 2.0 and 4.5. The quadrature sum of the azimuthal separation and the difference in pseudorapidities, denoted $\Delta R$, between the two leptons must be larger than 0.1. The $b$-jet axis is required to be separated from both leptons by a $\Delta R$ of 0.5, and to have a transverse momentum in excess of 20 GeV and a pseudorapidity between 2.2 and 4.2. The cross-section is measured to be $$\sigma_{t\bar{t}}= 126\pm19\,(\mathrm{stat})\pm16\,(\mathrm{syst})\pm5\,(\mathrm{lumi})\,\,\mathrm{ fb}$$ where the first uncertainty is statistical, the second is systematic, and the third is due to the luminosity determination. The measurement is compatible with the Standard Model prediction.
The measured fiducial cross section. The uncertainty is split into statistical, systematic and uncertainty due to luminosity.
Two-particle pseudorapidity correlations are measured in $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV Pb+Pb, $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV $p$+Pb, and $\sqrt{s}$ = 13 TeV $pp$ collisions at the LHC, with total integrated luminosities of approximately 7 $\mu\mathrm{b}^{-1}$, 28 $\mathrm{nb}^{-1}$, and 65 $\mathrm{nb}^{-1}$, respectively. The correlation function $C_{\rm N}(\eta_1,\eta_2)$ is measured as a function of event multiplicity using charged particles in the pseudorapidity range $|\eta|<2.4$. The correlation function contains a significant short-range component, which is estimated and subtracted. After removal of the short-range component, the shape of the correlation function is described approximately by $1+\langle{a_1^2}\rangle \eta_1\eta_2$ in all collision systems over the full multiplicity range. The values of $\sqrt{\langle{a_1^2}\rangle}$ are consistent between the opposite-charge pairs and same-charge pairs, and for the three collision systems at similar multiplicity. The values of $\sqrt{\langle{a_1^2}\rangle}$ and the magnitude of the short-range component both follow a power-law dependence on the event multiplicity. The $\eta$ distribution of the short-range component, after symmetrizing the proton and lead directions in $p$+Pb collisions, is found to be smaller than that in $pp$ collisions with comparable multiplicity.
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)
C_N(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)
SRC(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (260<=Nch<300)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (260<=Nch<300)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (240<=Nch<260)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (240<=Nch<260)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (220<=Nch<240)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (220<=Nch<240)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (200<=Nch<220)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (200<=Nch<220)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (180<=Nch<200)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (180<=Nch<200)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (160<=Nch<180)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (160<=Nch<180)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.5GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for Pb+Pb, pT>0.2GeV, (10<=Nch<20)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (120<=Nch<140)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (100<=Nch<120)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (100<=Nch<120)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (80<=Nch<100)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (80<=Nch<100)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (60<=Nch<80)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (60<=Nch<80)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (40<=Nch<60)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (40<=Nch<60)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (20<=Nch<40)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (20<=Nch<40)
C_N(eta_1, eta_2) for p+Pb, pT>0.5GeV, (10<=Nch<20)
C_N(eta_1, eta_2) for p+Pb, pT>0.2GeV, (10<=Nch<20)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (120<=Nch<140)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (100<=Nch<120)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (100<=Nch<120)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (80<=Nch<100)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (80<=Nch<100)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (60<=Nch<80)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (60<=Nch<80)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (40<=Nch<60)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (40<=Nch<60)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (20<=Nch<40)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (20<=Nch<40)
SRC(eta_1, eta_2) for p+Pb, pT>0.5GeV, (10<=Nch<20)
SRC(eta_1, eta_2) for p+Pb, pT>0.2GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (260<=Nch<300)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (260<=Nch<300)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (240<=Nch<260)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (240<=Nch<260)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (220<=Nch<240)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (220<=Nch<240)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (200<=Nch<220)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (200<=Nch<220)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (180<=Nch<200)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (180<=Nch<200)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (160<=Nch<180)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (160<=Nch<180)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.5GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for p+Pb, pT>0.2GeV, (10<=Nch<20)
C_N(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)
C_N(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)
C_N(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)
C_N(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)
C_N(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)
C_N(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)
C_N(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)
C_N(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)
C_N(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)
C_N(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)
C_N(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)
C_N(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)
C_N(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)
C_N(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)
C_N(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)
SRC(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)
SRC(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)
SRC(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)
SRC(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)
SRC(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)
SRC(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)
SRC(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)
SRC(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)
SRC(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)
SRC(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)
SRC(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)
SRC(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)
SRC(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)
SRC(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)
SRC(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)
SRC(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (140<=Nch<160)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (120<=Nch<140)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (100<=Nch<120)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (80<=Nch<100)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (60<=Nch<80)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (40<=Nch<60)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (20<=Nch<40)
C_N^sub(eta_1, eta_2) for pp, pT>0.5GeV, (10<=Nch<20)
C_N^sub(eta_1, eta_2) for pp, pT>0.2GeV, (10<=Nch<20)
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 100<=Nch<120, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 80<=Nch<100, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 60<=Nch<80, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 40<=Nch<60, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 20<=Nch<40, w SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 10<=Nch<20, w SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for Pb+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs
<a_n a_m> for Pb+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 260<=Nch<300, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 260<=Nch<300, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 240<=Nch<260, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 240<=Nch<260, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 220<=Nch<240, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 220<=Nch<240, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 200<=Nch<220, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 200<=Nch<220, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 180<=Nch<200, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 180<=Nch<200, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 160<=Nch<180, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 160<=Nch<180, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 120<=Nch<140, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 120<=Nch<140, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 100<=Nch<120, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 100<=Nch<120, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 80<=Nch<100, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 80<=Nch<100, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 60<=Nch<80, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 60<=Nch<80, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 40<=Nch<60, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 20<=Nch<40, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, opposite pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, same pairs
<a_n a_m> for p+Pb, pT>0.5GeV, 10<=Nch<20, wo SRC, all pairs
<a_n a_m> for p+Pb, pT>0.2GeV, 10<=Nch<20, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, same pairs
<a_n a_m> for pp, pT>0.5GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for pp, pT>0.2GeV, 140<=Nch<160, wo SRC, all pairs
<a_n a_m> for pp, pT>0.5GeV, 120<=Nch<140, wo SRC, opposite pairs
<a_n a_m> for pp, pT>0.2GeV, 120<=Nch<140, wo SRC, opposite pairs
Differential cross sections for the production of at least four jets have been measured in proton-proton collisions at $\sqrt{s} = 8$ TeV at the Large Hadron Collider using the ATLAS detector. Events are selected if the four anti-$k_{t}$ R=0.4 jets with the largest transverse momentum ($p_{T}$) within the rapidity range $|y|<2.8$ are well separated ($dR^{\rm min}_{4j}>0.65$), all have $p_{T}>64$ GeV, and include at least one jet with $p_{T} >100$ GeV. The dataset corresponds to an integrated luminosity of 20.3 $fb^{-1}$. The cross sections, corrected for detector effects, are compared to leading-order and next-to-leading-order calculations as a function of the jet momenta, invariant masses, minimum and maximum opening angles and other kinematic variables.
Measured differential four-jet cross section for R=0.4 jets, in bins of pT1, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All uncertainties are given in %. The first uncertainty quoted is due to the number of data events. DSYS:mcstat is the statistical uncertainty due to the number of MC simulation events. The other columns, denoted with DSYS, correspond to the experimental systematic uncertainties arising from JES, JER, unfolding and luminosity, respectively.
Measured differential four-jet cross section for R=0.4 jets, in bins of pT2, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of pT3, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of pT4, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of HT, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of min(m_2j)/m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as m_2j>500 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of min(m_2j)/m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as m_2j>1000 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of min(m_2j)/m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as m_2j>1500 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of min(m_2j)/m_4j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as m_2j>2000 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>700 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>1000 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>700 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDphi_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>1000 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>700 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>1000 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>700 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of minDy_3j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>1000 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of maxDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of maxDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>250 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of maxDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>400 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of maxDy_2j, along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts, as well as pT1>550 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>1. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>1, as well as pT1>250 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>1, as well as pT1>400 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>1, as well as pT1>550 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>2. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>2, as well as pT1>250 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>2, as well as pT1>400 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>2, as well as pT1>550 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>3. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>3, as well as pT1>250 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>3, as well as pT1>400 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>3, as well as pT1>550 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>4. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>4, as well as pT1>250 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>4, as well as pT1>400 GeV. All other details are as for pT1.
Measured differential four-jet cross section for R=0.4 jets, in bins of sum(pT), along with the uncertainties in the measurement. The events are selected using the inclusive analysis cuts and maxDy_2j>4, as well as pT1>550 GeV. All other details are as for pT1.
Measurements of the differential cross sections for the production of exactly four jets in proton-proton collisions are presented as a function of the transverse momentum pt and pseudorapidity eta, together with the correlations in azimuthal angle and the pt balance among the jets. The data sample was collected in 2010 at a center-of-mass energy of 7 TeV with the CMS detector at the LHC, with an integrated luminosity of 36 inverse picobarns. The cross section for a final state with a pair of hard jets with pt > 50 GeV and another pair with pt > 20 GeV within abs(eta) < 4.7 is measured to be sigma = 330 +- 5 (stat.) +- 45 (syst.) nb. It is found that fixed-order matrix element calculations including parton showers describe the measured differential cross sections in some regions of phase space only, and that adding contributions from double parton scattering brings the Monte Carlo predictions closer to the data.
The measured fiducial cross section. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the transverse momentum PT of the leading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the transverse momentum PT of the subleading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the transverse momentum PT of the third jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the transverse momentum PT of the fourth jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the pseudorapidity eta of the leading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the pseudorapidity eta of the subleading jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the pseudorapidity eta of the third jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the pseudorapidity eta of the fourth jet. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the azimuthal angle DeltaPhi between the third and the fourth jet, normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the normalized PT balance DELTARELPT between the third and the fourth jet, normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
Differential cross section as a function of the azimuthal angle between the two dijet planes (first-second and third-fourth jets), normalized to the total number of selected events. The first uncertainty is the statistical one, the second uncertainty is the combined systematic uncertainty including luminosity, jet energy scale, model dependence and jet energy resolution and trigger efficiency correction.
We report on measurements of e+e- annihilation into hadrons and lepton pairs. The data have been collected with the L3 detector at LEP at centre-of-mass energies between 130 and 189 GeV. Using a total integrated luminosity of 243.7 pb^-1, 25864 hadronic and 8573 lepton-pair events are selected for the measurement of cross sections and leptonic forward-backward asymmetries. The results are in good agreement with Standard Model predictions.
Measured cross sections for the hadronic events.
Measured cross sections for the muon-pair events.
Measured cross sections for the tau-pair events.
Measured cross sections for the electron-pair events. For Bhabha scattering events both the leptons have to be inside 44 to 136 degrees.
Forward backward asymmetry for lepton-pair events.
Measured cross sections for the tau-pair events.
Measured cross sections for the electron-pair events. For Bhabha scattering events both the leptons have to be inside 44 to 136 degrees.
Angular distributions for (MU+ MU-) and (TAU+ TAU-) events for the inclusive data sample. Statistical and systematic errors are combined.
Angular distributions for (MU+ MU-) and (TAU+ TAU-) events for the high-energy data sample. Statistical and systematic errors are combined.
Angular distributions for (E+ E-) events for the high energy event sample (ZETA <25 DEGS) Statistical and systematic errors are combined.
Hadron production and lepton-pair production in e+e- collisions are studied with data collected with the L3 detector at LEP at centre-of-mass energies sqrt{s}=192-208GeV. Using a total integrated luminosity of 453/pb, 36057 hadronic events and 12863 lepton-pair events are selected. The cross sections for hadron production and lepton-pair production are measured for the full sample and for events where no high-energy initial-state-radiation photon is emitted prior to the collisions. Lepton-pair events are further investigated and forward-backward asymmetries are measured. Finally, the differential cross sections for electron-positron pair-production is determined as a function of the scattering angle. An overall good agreement is found with Standard Model predictions.
Measured hadron cross section for the inclusive data sample.
Measured hadron cross section for the high-energy data sample.
Measured MU+ MU- cross section for the inclusive data sample.
Measured MU+ MU- cross section for the high-energy data sample.
Measured TAU+ TAU- cross section for the inclusive data sample.
Measured TAU+ TAU- cross section for the high-energy data sample.
Measured E+ E- --> E+ E- cross section for the inclusive data sample.
Measured E+ E- --> E+ E- cross section for the high-energy data sample.
Measured Forward-Backward asymmetry in MU+ MU- production from the inclusive data sample.
Measured Forward-Backward asymmetry in MU+ MU- production from the high-energy data sample.
Measured Forward-Backward asymmetry in TAU+ TAU- production from the inclusive data sample.
Measured Forward-Backward asymmetry in TAU+ TAU- production from the high-energy data sample.
Measured Forward-Backward asymmetry in E+ E- production for the inclusive data sample.
Measured Forward-Backward asymmetry in E+ E- production for the high-energy data sample.
Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 192 GeV.
Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 196 GeV.
Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 200 GeV.
Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 202 GeV.
Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 205 GeV.
Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 207 GeV.
Differential cross sections for E+ E- production as a function of the scattering angle for the high-energy data sample for centre of mass energy 208 GeV.
A measurement of event-shape variables in proton$-$proton collisions at large momentum transfer is presented using data collected at $\sqrt{s} = 13$ TeV with the ATLAS detector at the Large Hadron Collider. Six event-shape variables calculated using hadronic jets are studied in inclusive multijet events using data corresponding to an integrated luminosity of 139 fb$^{-1}$. Measurements are performed in bins of jet multiplicity and in different ranges of the scalar sum of the transverse momenta of the two leading jets, reaching scales beyond 2 TeV. These measurements are compared with predictions from Monte Carlo event generators containing leading-order or next-to-leading order matrix elements matched to parton showers simulated to leading-logarithm accuracy. At low jet multiplicities, shape discrepancies between the measurements and the Monte Carlo predictions are observed. At high jet multiplicities, the shapes are better described but discrepancies in the normalisation are observed.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ = 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.0 < $H_{\textrm{T2}}$ < 1.5 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.
Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.0 < $H_{\textrm{T2}}$ < 1.5 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.
Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.5 < $H_{\textrm{T2}}$ < 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.
Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for 1.5 < $H_{\textrm{T2}}$ < 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.
Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for $H_{\textrm{T2}}$ > 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.
Measured total cross section for multijet production as a function of $n^{\textrm{jet}}$ for $H_{\textrm{T2}}$ > 2.0 TeV. The total cross-sections are measured in the same fiducial phase-space region than the measured relative cross-sections as functions of event-shape variables for the corresponding $H_{\textrm{T2}}$ interval. The measurement in the last bin corresponds to $n^{\textrm{jet}}\geq$ 6.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $\tau_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of T$_{\textrm{m}}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of S$_{\perp}$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $A$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $C$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1 TeV < $H_{\textrm{T2}}$ < 1.5 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and 1.5 TeV < $H_{\textrm{T2}}$ < 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 3 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 4 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}\geq$ 5 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
Measured relative cross sections for multijet production as a function of $D$ for $n^{\textrm{jet}}$ $\geq$ 6 and $H_{\textrm{T2}}$ > 2.0 TeV.
The production of W bosons in association with two jets in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$=7 TeV has been analysed for the presence of double-parton interactions using data corresponding to an integrated luminosity of 36/pb, collected with the ATLAS detector at the LHC. The fraction of events arising from double-parton interactions, $f_{DP}^{(D)}$ has been measured through the momentum balance between the two jets and amounts to $f_{DP}^{(D)} = 0.08 \pm 0.01 (stat.) \pm 0.02 (sys.)$ for jets with transverse momentum PT > 20 GeV and rapidity |y|<2.8. This corresponds to a measurement of the effective area parameter for hard double-parton interactions of $\sigma_{eff} = 15 \pm 3 (stat.)^{+5}_{-3}$ (sys.) mb.
Distribution of Delta(jets,normalised), defined in Eq. (11) of the paper as the transverse momentum of the dijet system normalised by the sum of the individual transverse momenta, in the data after unfolding to hadron level. The errors on the data represent the quadrature sum of the statistical and systematic uncertainties. Data have been normalised to unity.
Distribution of Delta(jets), defined in Eq. (10) of the paper as the transverse momentum of the dijet system, in the data after unfolding to hadron level. The errors on the data represent the quadrature sum of the statistical and systematic uncertainties. Data have been normalised to unity.
Inclusive production of $\mathrm{D^{*\pm}}$ mesons in two-photon collisions was measured by the L3 experiment at LEP. The data were collected at a centre-of-mass energy $\sqrt{s} = 189$ GeV with an integrated luminosity of $176.4 \mathrm{pb^{-1}}$. Differential cross sections of the process $\mathrm{e^+e^- \to D^{*\pm} X}$ are determined as functions of the transverse momentum and pseudorapidity of the $\mathrm{D^{*\pm}}$ mesons in the kinematic region 1 GeV $< p_{T}^{\mathrm{D^*}} < 5 $ GeV and $\mathrm{|\eta^{D^*}|} < 1.4$. The cross section integrated over this phase space domain is measured to be $132 \pm 22(stat.) \pm 26(syst.)$ pb. The differential cross sections are compared with next-to-leading order perturbative QCD calculations.
The measured cross sections, as a function of PT over the bin ranges and the differential cross sections after bin-centre corrections.
The measured cross sections, as a function of pseudorapidity over the bin ranges and the differential cross sections after bin-centre corrections.
Integrated cross section in the visible kinematic region.
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