Search results for "RAPIDITY"
showing 10 items of 810 documents
"Table 7" of "K^0_S and {\Lambda} production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"
2016
pT spectra of K0Short in the rapidity range -0.5
"Table 6" of "K^0_S and {\Lambda} production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"
2016
pT spectra of K0Short in the rapidity range -0.5
"Table 4" of "K^0_S and {\Lambda} production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"
2016
pT spectra of K0Short in the rapidity range -0.5
"Table 5" of "K^0_S and {\Lambda} production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"
2016
pT spectra of K0Short in the rapidity range -0.5
"Table 3" of "K^0_S and {\Lambda} production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"
2016
pT spectra of K0Short in the rapidity range -0.5
"Table 1" of "K^0_S and {\Lambda} production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"
2016
pT spectra of K0Short in the rapidity range -0.5
"Table 2" of "K^0_S and {\Lambda} production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"
2016
pT spectra of K0Short in the rapidity range -0.5
The ATLAS Level-1 Calorimeter Trigger: PreProcessor implementation and performance
2012
The PreProcessor system of the ATLAS Level-1 Calorimeter Trigger (L1Calo) receives about 7200 analogue signals from the electromagnetic and hadronic components of the calorimetric detector system. Lateral division results in cells which are pre-summed to so-called Trigger Towers of size 0.1 × 0.1 along azimuth (phi) and pseudorapidity (η). The received calorimeter signals represent deposits of transverse energy. The system consists of 124 individual PreProcessor modules that digitise the input signals for each LHC collision, and provide energy and timing information to the digital processors of the L1Calo system, which identify physics objects forming much of the basis for the full ATLAS fi…
Multiplicity dependence of light (anti-)nuclei production in p–Pb collisions at sNN=5.02 TeV
2020
The measurement of the deuteron and anti- deuteron production in the rapidity range −1 < y < 0 as a function of transverse momentum and event multiplicity in p–Pb collisions at √sNN= 5.02 TeV is presented. (Anti-)deuterons are identified via their specific energy loss dE/dxand via their time-of-flight. Their production in p–Pb collisions is compared to pp and Pb–Pb collisions and is discussed within the context of thermal and coalescence models. The ratio of integrated yields of deuterons to protons (d/p) shows a significant increase as a function of the charged-particle multiplicity of the event starting from values similar to those observed in pp collisions at low multiplicities and appro…
Effects of shadowing on Drell-Yan dilepton production in high energy nuclear collisions
2001
We compute cross sections for the Drell-Yan process in nuclear collisions at next-to-leading order (NLO) in ��_s. The effects of shadowing on the normalization and on the mass and rapidity dependence of these cross sections are presented. An estimate of higher order corrections is obtained from next-to-next-to-leading order (NNLO) calculation of the rapidity-integrated mass distribution. Variations in these predictions resulting from choices of parton distribution sets are discussed. Numerical results for mass distributions at NLO are presented for RHIC and LHC energies, using appropriate rapidity intervals. The shadowing factors in the dilepton mass range 2 < M < 10 GeV are predicted…