[PDF] Top 20 Diseño de rutas de vehículos en una empresa de transporte de hidrocarburos
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Central Exclusive Production in Proton-Proton Collisions with the STAR Experiment at RHIC
... is produced mostly around pseudorapidity η ≈ 0 (midrapidity). This process belongs to a class of Double Pomeron Exchange (DPE) processes and is commonly called a Central Production process. The case when ... See full document
16
Central exclusive production of K+K− pairs in proton-proton collisions
... the RHIC and LHC ...are exclusive processes, where all centrally produced particles are ...pair production pp → ppK + K − , which can be used for studies of low-mass resonances, including searches ... See full document
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Exclusive meson pair production in proton-proton collisions
... the proton lines. We include ab- sorption effects due to proton-proton interaction and pion/kaon ...the RHIC, Tevatron and LHC ...of exclusive production of a scalar χ c0 meson ... See full document
6
Measurements of open charm production and flow in √sNN = 200GeV Au+Au collisions with the STAR experiment at RHIC
... at STAR is provided by the ionization energy loss (dE/dx) measured in the Time Projection Chamber (TPC) [11] and the velocity measured using the Time of Flight (TOF) detector ...at RHIC are ... See full document
11
Recent results on cold-QCD from RHIC
... Polarized proton-proton collisions at the Relativistic Heavy Ion Collider (RHIC) provide unique opportunities to study the spin structure of the ...the STAR and PHENIX experiments at ... See full document
24
Central Exclusive Production in pp collisions at LHCb
... Central exclusive production (CEP) at the LHC is characterised by an isolated system of particles surrounded by two rapidity gaps that extend down to the intact colliding protons; see [1] and the ... See full document
7
Quarkonium photoproduction in pp and AA collisions at the LHC
... J/ψ exclusive production in the fixed energies of 7 TeV(solid line), 8 TeV (dashed line) and 14 TeV (dot- dashed ...and central rapidity, y = ... See full document
5
Measurement of quarkonium production in proton-lead and proton-proton collisions at 5.02 TeV with the ATLAS detector
... quarkonium production were performed with p+Pb data collected in 2013 at the LHC at a centre-of-mass energy per nucleon pair √ s NN = 5 ...J/ψ production is observed at small rapidi- ties and high ... See full document
25
Reconstruction of primary vertices at the ATLAS experiment in Run 1 proton-proton collisions at the LHC
... 11 Efficiency to reconstruct and then select the hard-scatter primary vertex as a function of the average number of pp interactions per bunch crossing, μ, for different physics processes[r] ... See full document
22
Measurement of quarkonium production in proton-lead and proton-proton collisions at 5.02 TeV with the ATLAS detector
... quarkonium production were performed with p +Pb data col- lected in 2013 at the LHC at a centre-of-mass energy per nucleon pair √ s NN = ...J/ψ production is observed at small rapidities and high transverse ... See full document
6
Neural Networks Search for Charged Higgs Boson in Two Doublet Higgs Model at the Hadrons Colliders
... the production and decay of top quark ...the production cross section at different energies, decay width, branching ration and different ki- nematics distribution for charged Higgs boson and for the final ... See full document
12
Search for Stop Pair Production at the LHC using the CMS Detector
... signal production cross section at 95% confidence level us- ing the SR with the best expected sensitivity at that point. Exclusion regions are defined by comparing these cross section upper limits to the ... See full document
39
Eta Meson Production in Proton-Deuteron Collisions
... Abstract. Since many years the strong final state interaction between η-mesons and light nuclei and the discussed possibility for the formation of η-mesic nuclei has attracted broad experimental and theoretical ... See full document
37
Observation of Y(1S) pair production in proton-proton collisions at √s=8 TeV
... The central feature of the CMS apparatus is a 13 m long superconducting solenoid of 6 m internal diameter, providing a magnetic field of 3.8 T. Within the solenoid volume are a silicon pixel and strip tracker, a ... See full document
10
Optimization techniques in elastic proton proton collisions
... w here is th e center-of-m ass energy and sq is a c o n sta n t. Since th e resu lt of F ro issart m any developm ents of th e m e th o d of o b ta in in g b o u n d s on s c a tte r ing a m p litu d es have b een m ade ... See full document
139
Evidence for the Higgs boson in the H->WW->lnulnu decay channel
... ATLAS has a toroidal magentic field [56] that bend charged particles inside the inner detector (ID), which will be discussed in Section 3.4. The ID extends to 1.2 m from the proton beam. The magnetic field ... See full document
8
Spin Dependence of η Meson Production in Proton-Proton Collisions Close to Threshold
... polarized proton beam was circulating through the vertical stream of the hydrogen pellets, leading to the pp ⃗ → ppη reaction in the center of the WASA-at-COSY ...the proton beam polarization was flipped ... See full document
10
Current status of the LHCf experiment and future plan
... LHCf experiment has successfully measured the energy spectra of photon emitted in the very forward region of the LHC proton-proton collisions in ... See full document
6
Production of exotic charmonium in heavy ion collisions
... the production mechanism is coalescence, then the production yield of these exotic hadrons at the moment of their formation strongly reflects their internal ...the production yield of the X(3872), at ... See full document
18
Search for the QCD Critical Point with Fluctuations of Conserved Quantities in Relativistic Heavy-Ion Collisions at RHIC
... of STAR is to be upgraded to improve the energy loss resolution and can extend the pseudo-rapidity coverage from |η| < 1 to |η| < ...the STAR TPC to extend the PID capability in the forward region ... See full document
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