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[PDF] Top 20 Determination of the strong coupling constant from the inclusive jet cross section in ppbar collisions at sqrt(s)=1.96 TeV

Has 10000 "Determination of the strong coupling constant from the inclusive jet cross section in ppbar collisions at sqrt(s)=1.96 TeV" found on our website. Below are the top 20 most common "Determination of the strong coupling constant from the inclusive jet cross section in ppbar collisions at sqrt(s)=1.96 TeV".

Determination of the strong coupling constant from the inclusive jet cross section in ppbar collisions at sqrt(s)=1.96 TeV

Determination of the strong coupling constant from the inclusive jet cross section in ppbar collisions at sqrt(s)=1.96 TeV

... using the PDFs to extract α s (M Z ) from the jet ...those jet cross section data points which have provided strong PDF ...While the quark PDFs are ... Voir le document complet

7

Observation of ZZ production in ppbar collisions at sqrt(s) = 1.96 TeV

Observation of ZZ production in ppbar collisions at sqrt(s) = 1.96 TeV

... As in the 4e channel, these sub- samples have significantly different levels of background ...determine the expected number of signal events in each subchan- ...nel. The ... Voir le document complet

7

Measurement of the dijet invariant mass cross section in proton anti-proton collisions at sqrt{s} = 1.96 TeV

Measurement of the dijet invariant mass cross section in proton anti-proton collisions at sqrt{s} = 1.96 TeV

... similar in size to both the PDF and the scale uncertainties, suggesting that the measurement will constrain theoretical mod- ...C.L. The total uncertainties are smaller than those ... Voir le document complet

9

Determination of the top-quark pole mass and strong coupling constant from the t[bar over t] production cross section in pp collisions at √s = 7 TeV

Determination of the top-quark pole mass and strong coupling constant from the t[bar over t] production cross section in pp collisions at √s = 7 TeV

... . The corresponding uncertainties are calculated at the 68% confidence level for all PDF ...recalculating the σ t ¯ t at NNLO + NNLL for each of the provided eigenvectors ... Voir le document complet

23

Measurement of the ratio of differential cross sections {\sigma}(ppbar -> Z + b jet)/{\sigma}(ppbar -> Z + jet) in ppbar collisions at sqrt(s)=1.96 TeV

Measurement of the ratio of differential cross sections {\sigma}(ppbar -> Z + b jet)/{\sigma}(ppbar -> Z + jet) in ppbar collisions at sqrt(s)=1.96 TeV

... on the complete Run II data sample collected by the D0 experiment [12] at Fermilab’s Tevatron pp collider running with a center-of- mass energy of √ s = ...1.96 TeV, and ... Voir le document complet

8

Measurements of inclusive W+jets production rates as a function of jet transverse momentum in ppbar collisions at sqrt{s}=1.96 TeV

Measurements of inclusive W+jets production rates as a function of jet transverse momentum in ppbar collisions at sqrt{s}=1.96 TeV

... have at least two tracks that point to their associ- ated p¯ p ...Energies of jets containing muons are corrected with the measured muon momentum after ac- counting for the typical energy ... Voir le document complet

16

Determination of the strong coupling constant $\alpha _\mathrm {s}$ from transverse energy–energy correlations in multijet events at $\sqrt{s} = 8~\hbox {TeV}$ using the ATLAS detector

Determination of the strong coupling constant $\alpha _\mathrm {s}$ from transverse energy–energy correlations in multijet events at $\sqrt{s} = 8~\hbox {TeV}$ using the ATLAS detector

... Measurements of transverse energy–energy correlations and their associated asymmetries in multi-jet events using the ATLAS detector at the LHC are ...presented. The data ... Voir le document complet

49

Measurement of the inclusive $t\bar{t}$ production cross section in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV and determination of the top quark pole mass

Measurement of the inclusive $t\bar{t}$ production cross section in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV and determination of the top quark pole mass

... varying the values of a specific parameter in the modeling of the data, and determining the effect on the distributions or MC templates of the ... Voir le document complet

21

Measurement of the differential cross section of photon plus jet production in ppbar collisions at sqrt{s}=1.96 TeV

Measurement of the differential cross section of photon plus jet production in ppbar collisions at sqrt{s}=1.96 TeV

... estimate the remaining background contribution from dijet events, we consider photon candidates in the region ...≤ 1 (i.e. the region used for data anal- ysis). The ... Voir le document complet

22

Measurement of transverse energy-energy correlations in multi-jet events in $pp$ collisions at $\sqrt{s} = 7$ TeV using the ATLAS detector and determination of the strong coupling constant $\alpha_{\mathrm{s}}(m_Z)$

Measurement of transverse energy-energy correlations in multi-jet events in $pp$ collisions at $\sqrt{s} = 7$ TeV using the ATLAS detector and determination of the strong coupling constant $\alpha_{\mathrm{s}}(m_Z)$

... T. Obermann 21 , J. Ocariz 80 , A. Ochi 67 , I. Ochoa 78 , J.P. Ochoa-Ricoux 32a , S. Oda 70 , S. Odaka 66 , H. Ogren 61 , A. Oh 84 , S.H. Oh 45 , C.C. Ohm 15 , H. Ohman 166 , H. Oide 30 , W. Okamura 118 , H. Okawa 160 , ... Voir le document complet

36

Measurement of direct photon pair production cross sections in ppbar collisions at sqrt(s)=1.96 TeV

Measurement of direct photon pair production cross sections in ppbar collisions at sqrt(s)=1.96 TeV

... subtraction of the estimated ZDY contribution) compose a 4-component vector (N pp , N pf , N f p , N f f ...). The difference in relative efficiencies of the O NN > ... Voir le document complet

11

Constraints on parton distribution functions and extraction of the strong coupling constant from the inclusive jet cross section in pp collisions at √s = 7 TeV

Constraints on parton distribution functions and extraction of the strong coupling constant from the inclusive jet cross section in pp collisions at √s = 7 TeV

... colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS ... Voir le document complet

43

Measurement of the WW production cross section in $p\overline{p}$ collisions at $\sqrt{s}$ = 1.96 TeV

Measurement of the WW production cross section in $p\overline{p}$ collisions at $\sqrt{s}$ = 1.96 TeV

... For the normalization of Z/γ ∗ and W +jet/γ events, the NNLO cross sections from ...used. The cross section times branching ratio of Z/γ ∗ production ... Voir le document complet

7

Measurement of the $tt\bar$ production cross section in $pp\bar$ collisions at $\sqrt{s} = 1.96 TeV$

Measurement of the $tt\bar$ production cross section in $pp\bar$ collisions at $\sqrt{s} = 1.96 TeV$

... that at least one jet be tagged as a b-jet, ...contain the decay of a long-lived particle such as a b-hadron ...determine the number of background events without prompt ... Voir le document complet

7

Measurement of the inclusive differential jet cross section in pp collisions at sqrt{s} = 2.76 TeV

Measurement of the inclusive differential jet cross section in pp collisions at sqrt{s} = 2.76 TeV

... Table 1 shows all contributions to the systematic uncertainty of JES, determined from the variation in corrected jet yield arising from systematic variation ... Voir le document complet

18

Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector

... ]. The calculations are performed using the MMHT2014 [ 52 ] PDF set and the BFG set II of parton-to-photon fragmentation functions [ 53 ], both at ...NLO. The strong ... Voir le document complet

40

Measurement of inclusive jet and dijet production in pp collisions at sqrt(s) = 7 TeV using the ATLAS detector

Measurement of inclusive jet and dijet production in pp collisions at sqrt(s) = 7 TeV using the ATLAS detector

... regarding the non-perturbative correc- tions. We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS ... Voir le document complet

54

Measurement of the Zgamma to nunugamma production cross section and limits on anomalous ZZgamma and Zgammagamma couplings in ppbar collisions at sqrt{s} = 1.96 TeV

Measurement of the Zgamma to nunugamma production cross section and limits on anomalous ZZgamma and Zgammagamma couplings in ppbar collisions at sqrt{s} = 1.96 TeV

... reduce the copious non-collision background (events in which muons from the beam halo or cosmic rays un- dergo bremsstrahlung, and produce energetic photons), we use a pointing algorithm [12], ... Voir le document complet

7

Measurement of the total cross section from elastic scattering in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

Measurement of the total cross section from elastic scattering in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

... out in order to cross-check the fitting ...only the covariance matrix of statistical uncertainties yields σ tot = ...(stat.) in good agreement with the results from ... Voir le document complet

35

Measurement of the forward $W$ boson cross-section in $pp$ collisions at $\sqrt{s} = 7 {\rm \, TeV}$

Measurement of the forward $W$ boson cross-section in $pp$ collisions at $\sqrt{s} = 7 {\rm \, TeV}$

... J.M. Otalora Goicochea 2 , P. Owen 53 , A. Oyanguren 64 , B.K. Pal 59 , A. Palano 13,c , F. Palombo 21,u , M. Palutan 18 , J. Panman 38 , A. Papanestis 49,38 , M. Pappagallo 51 , L.L. Pappalardo 16,f , C. Parkes 54 , ... Voir le document complet

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