[PDF] Top 20 Measurement of charged particle spectra in minimum-bias events from proton-proton collisions at root s =13 TeV
Has 10000 "Measurement of charged particle spectra in minimum-bias events from proton-proton collisions at root s =13 TeV" found on our website. Below are the top 20 most common "Measurement of charged particle spectra in minimum-bias events from proton-proton collisions at root s =13 TeV".
Measurement of charged particle spectra in minimum-bias events from proton-proton collisions at root s =13 TeV
... performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS ...effort. In addition, we ... See full document
29
Measurement of jet substructure observables in t(t)over-bar events from proton-proton collisions at root s=13 TeV
... separations in pseu- dorapidity and azimuth (in radians) of lepton and PF candidate, respectively] around the lepton direction, di- vided by the lepton p T , and is required to be smaller than ... See full document
37
Measurement of charm and beauty production at central rapidity versus charged-particle multiplicity in proton-proton collisions at root s=7 TeV
... scheme in all the systems, ...generated in the Gribov-Regge multiple scattering framework, using the “Parton based Gribov-Regge” formalism [ 71 ...composed of a pQCD hard process with initial and ... See full document
47
Measurement of the energy density as a function of pseudorapidity in proton-proton collisions at root s=13 TeV
... smearing in pseudorapidity; it is basically the characteristic response of the calorimeters as well as the event selection acceptance and inefficiency that are ...evaluated from the ratio of ... See full document
25
Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at sqrt(s) = 2.76 TeV
... sample of proton-proton collisions collected with the CMS detector at √ s = ...2.76 TeV during a dedicated run in March 2011, corresponding to an integrated ... See full document
30
Charged jet cross section and fragmentation in proton-proton collisions at root S=7 TeV
... luminosity of ð2.9 0.1Þ nb −1 [25] . The mini- mum bias trigger requires at least one hit in either the V0 forward scintillators or in the two innermost silicon pixel detector layers ... See full document
17
Charged jet cross sections and properties in proton-proton collisions at root s=7 TeV
... primary charged particles (prompt particles produced in the collisions and all decay products, except products from weak decays of strange particles such as K 0 S and ... See full document
34
Search for heavy neutral leptons in events with three charged leptons in proton-proton collisions at $\sqrt{s} =$ 13 TeV
... cases of N masses below and above that of the W boson, two search regions are defined, referred to as the low- and high-mass ...regions. In the low-mass region (targeting m N < m W ), N is ... See full document
20
Search for electroweak production of charginos and neutralinos in WH events in proton-proton collisions at root s=13 TeV
... feature of the CMS apparatus is a superconducting solenoid, 13 m in length and 6 m in diameter, which provides an axial magnetic field of ...several particle detection systems. ... See full document
42
Search for excited leptons in final states in proton-proton collisions at root s=13 TeV
... a particle-flow algorithm [ 35 ] for optimal efficiency, kinematic resolution and purity in physics object reconstruction and ...The particle- flow algorithm aims to reconstruct and identify ... See full document
38
Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at root s=13 TeV
... precision in estimating the misreconstructed jet background is limited by the amount of data at high dilepton mass, and a conservative uncertainty of 50% is ...uncertainty in the ... See full document
37
Measurement of the top quark mass using single top quark events in proton-proton collisions at root s=8 TeV
... support from the Marie-Curie programme and the European Research Council and EPLANET (European Union); the Leventis Foundation; the ...Ministry of Education, Youth and Sports (MEYS) of the Czech ... See full document
26
Combination of searches for Higgs boson pair production in proton-proton collisions at root s=13 TeV
... solenoid of 6 m internal diameter, providing a magnetic field of ...composed of a barrel and two end cap ...detected in gas-ionization chambers embedded in the steel flux-return yoke ... See full document
19
Search for W ' -> tb in proton-proton collisions at root s=8 TeV
... applicability of the QCD background estimation in data, we apply the average b-tagging rate to control regions of the t-tagging selection defined in section ...inverted minimum pairwise ... See full document
43
Search for pair-produced three-jet resonances in proton-proton collisions at root s=13 TeV
... Additional proton-pro- ton interactions within the same or nearby bunch crossings can contribute additional tracks and calorimetric energy depositions to the jet ...originating from pileup vertices are ... See full document
22
Measurement of pseudorapidity distributions of charged particles in proton-proton collisions at root s=8 TeV by the CMS and TOTEM experiments
... composed of three subdetectors: the Roman pots and the T1 and T2 ...telescopes. Minimum bias events are triggered by the two T2 telescopes, which are placed symmetrically on each side ... See full document
27
Measurement of charged-particle distributions sensitive to the underlying event in $ \sqrt{s}=13 $ TeV proton-proton collisions with the ATLAS detector at the LHC
... support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and ... See full document
40
Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $
... j. In this analysis, two different correction procedures were ...use of the full detector simulation, while in the second method (method 2) a parametrization of the detector response is ... See full document
38
Measurement of charged pion, kaon, and proton production in proton-proton collisions at root s=13 TeV
... ingredients of PYTHIA 6 and PYTHIA8 are (multiple) leading-order perturbative QCD 2 → 2 matrix elements, complemented with initial- and final-state parton radiation (ISR and FSR), folded with parton distribution ... See full document
25
Charged-particle multiplicities in proton-proton collisions at root s=0.9 to 8 TeV
... result of the unfolding ...uncertainty from all the sources considered was esti- mated as the overall spread between the resulting distribu- ...(center of the band covered by the 72 curves) was used ... See full document
40
temas relacionados