• No results found

[PDF] Top 20 The elastic differential pp cross-section at 13 TeV: an empirical model analysis

Has 10000 "The elastic differential pp cross-section at 13 TeV: an empirical model analysis" found on our website. Below are the top 20 most common "The elastic differential pp cross-section at 13 TeV: an empirical model analysis".

The elastic differential pp cross-section at 13 TeV: an empirical model analysis

The elastic differential pp cross-section at 13 TeV: an empirical model analysis

... • 2. There is a sizeable C = − 1 contribution even at asymptotic energies. In QCD language, it is usually interpreted as follows. The leading exchange for hadronic (color singlet) scat- terings is provided by the ... See full document

10

Measurements of the elastic, inelastic and total pp cross sections with the ATLAS, CMS and TOTEM detectors

Measurements of the elastic, inelastic and total pp cross sections with the ATLAS, CMS and TOTEM detectors

... inelastic cross section at √ s = 13 TeV used by ATLAS [5] and CMS [6] is to measure the inelastic cross section in a fiducial region and then use theoretical models to extrapolate ... See full document

6

Measurement of the cross section for inclusive isolated-photon production in pp collisions at √s=13 TeV using the ATLAS detector

Measurement of the cross section for inclusive isolated-photon production in pp collisions at √s=13 TeV using the ATLAS detector

... 8 TeV data ...the analysis sepa- rately to maintain the full information about the ...measured cross sections due to the effects mentioned above are estimated by vary- ing by ± 1 σ each individual ... See full document

21

Measurement of the cross-section for producing a W boson in association with a single top quark in pp collisions at root s=13 TeV with ATLS

Measurement of the cross-section for producing a W boson in association with a single top quark in pp collisions at root s=13 TeV with ATLS

... are model uncertainties (such as flavour composition, η intercalibration model), and other systematics in the JES determination (such as pile-up jet area ...this analysis are the in situ calibration ... See full document

42

Measurement of the total cross section from elastic scattering in pp collisions at √s=8 TeV with the ATLAS detector

Measurement of the total cross section from elastic scattering in pp collisions at √s=8 TeV with the ATLAS detector

... the differential elastic cross section as a function of t for selected systematic uncertainty ...(Physics model) and to the ...the differential elastic cross ... See full document

21

Measurement of the W+ W- production cross section in pp collisions at a centre-of-mass energy of root s=13 TeV with the ATLAS experiment

Measurement of the W+ W- production cross section in pp collisions at a centre-of-mass energy of root s=13 TeV with the ATLAS experiment

... to model signal and background ...The cross sections given by the event generator are at NLO in QCD while the WW, WZ and ZZ samples are normalised using their respective inclusive next-to-next-to-leading ... See full document

37

Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at √s=8 TeV and cross section ratios to 2.76 and 7 TeV

Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at √s=8 TeV and cross section ratios to 2.76 and 7 TeV

... Individuals have received support from the Marie-Curie programme and the Euro- pean Research Council and EPLANET (European Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von Humboldt ... See full document

52

Measurement of the differential inclusive B+ hadron cross sections in pp collisions at √s=13 TeV

Measurement of the differential inclusive B+ hadron cross sections in pp collisions at √s=13 TeV

... of 3.8 T. A silicon pixel and strip tracker, a lead tungstate crystal electromagnetic calorimeter, and a brass and scintillator hadron calorimeter reside within the magnetic volume of the solenoid. The inner tracker ... See full document

22

Measurement of the W<sup>±</sup>Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector

Measurement of the W<sup>±</sup>Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector

... in Section 5, except that a different-flavour, opposite-charge lepton pair is asso- ciated with the Z boson, and the m requirement is removed to increase the number of ...multiplicity differential ... See full document

22

Evidence for Non-Exponential Differential Cross-Section of pp Elastic Scattering at Low |t| and √s = 8 TeV by TOTEM

Evidence for Non-Exponential Differential Cross-Section of pp Elastic Scattering at Low |t| and √s = 8 TeV by TOTEM

... differential cross-section of elastic pp scattering was actually anticipated by a number of theoretical ...8 TeV extrapolating fit parameters from ISR to LHC energies ...of elastic ... See full document

6

Measurement of the W+W− Cross Section in s√=7  TeV pp Collisions with ATLAS

Measurement of the W+W− Cross Section in s√=7  TeV pp Collisions with ATLAS

... T. N. Trinh, 78 M. F. Tripiana, 70 N. Triplett, 64 W. Trischuk, 158 A. Trivedi, 24,x B. Trocme´, 55 C. Troncon, 89a M. Trottier-McDonald, 142 A. Trzupek, 38 C. Tsarouchas, 29 J. C-L. Tseng, 118 M. Tsiakiris, 105 P. V. ... See full document

18

Measurements of the production cross section of a Z boson in association with jets in pp collisions at root s=13 TeV with the ATLAS detector

Measurements of the production cross section of a Z boson in association with jets in pp collisions at root s=13 TeV with the ATLAS detector

... M. King 170 , J. Kirk 133 , A.E. Kiryunin 103 , T. Kishimoto 157 , D. Kisielewska 41a , F. Kiss 51 , K. Kiuchi 164 , O. Kivernyk 138 , E. Kladiva 146b , M.H. Klein 38 , M. Klein 77 , U. Klein 77 , K. Kleinknecht 86 , P. ... See full document

47

Measurement of the inclusive φ cross section in pp collisions at √s=7 TeV

Measurement of the inclusive φ cross section in pp collisions at √s=7 TeV

... The luminosity was measured by two van der Meer scans [10] and a novel method measuring the beam geometry with the VELO, as described in Ref. [11]. Both methods rely on the measurement of the beam currents as well as the ... See full document

8

Measurement of the B ± production cross section in pp collisions at √s = 7 TeV

Measurement of the B ± production cross section in pp collisions at √s = 7 TeV

... second one confirms the single-muon from L0 and looks for another muon in the event, and the third one confirms the dimuon candidates from L0. Both the second and third selections require the dimuon invariant mass to be ... See full document

14

Precision RENORM / MBR Diffraction Predictions Tested by Recent LHC Results

Precision RENORM / MBR Diffraction Predictions Tested by Recent LHC Results

... total, elastic and total-inelastic, as well as the single di ff ractive (SD) and double di ff ractive (DD) components of the proton-proton cross section at high energies based RENORM / MBR ...DD ... See full document

5

Measurement of the cross-section for electroweak production of dijets in association with a Z boson in pp collisions at √s=13 TeV with the ATLAS detector

Measurement of the cross-section for electroweak production of dijets in association with a Z boson in pp collisions at √s=13 TeV with the ATLAS detector

... Fiducial cross-sections for the electroweak production of two jets in association with a leptonically decaying Z boson in proton– proton collisions are measured at a centre-of-mass energy of 13 TeV, ... See full document

23

Measurements of the production cross section of a Z boson in association with jets in pp collisions at root s=13 TeV with the ATLAS detector

Measurements of the production cross section of a Z boson in association with jets in pp collisions at root s=13 TeV with the ATLAS detector

... R. Staszewski 42 , P. Steinberg 27 , B. Stelzer 144 , H. J. Stelzer 32 , O. Stelzer-Chilton 163a , H. Stenzel 55 , G. A. Stewart 56 , J. A. Stillings 23 , M. C. Stockton 90 , M. Stoebe 90 , G. Stoicea 28b , P. Stolte 57 ... See full document

31

Measurement of the W+W  cross section in √s=7 TeV pp collisions with ATLAS

Measurement of the W+W cross section in √s=7 TeV pp collisions with ATLAS

... There are two major sources of systematic uncertainty in the jet-veto efficiency. The first is the modeling of jet production in association with W þ W due to initial state radiation, radiation from the internal line in ... See full document

19

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

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

... measured cross sections is ...The analysis is repeated using different sets of variables: tighter (looser) identification criteria are defined by applying tight requirements to an extended (restricted) set of ... See full document

26

Measurement of the cross-section for producing a W boson in association with a single top quark in pp collisions at root s=13 TeV with ATLS

Measurement of the cross-section for producing a W boson in association with a single top quark in pp collisions at root s=13 TeV with ATLS

... underlying-event model uncertainty is estimated by comparing Powheg-Box interfaced with either Pythia 6 or ...element model, parton shower model, and PDF uncertainties are estimated using ... See full document

40

Show all 10000 documents...