Search results for "DETECTOR"

showing 10 items of 3491 documents

"Table 16" of "Measurement of the low-energy antideuteron inelastic cross section"

2020

Inelastic interaction cross section of antideuterons on an averaged material element of the ALICE detector (2 sigma constraints).

5020.0Antideuteron inelastic c.s.Physics::Instrumentation and DetectorsP PB --> XHigh Energy Physics::ExperimentNuclear ExperimentSIG_INEL
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"Table 12" of "Measurement of the low-energy antideuteron inelastic cross section"

2020

Inelastic interaction cross section of antiprotons on an averaged material element of the ALICE detector (2 sigma constraints).

5020.0Physics::Instrumentation and DetectorsP PB --> XHigh Energy Physics::ExperimentAntiproton inelastic c.s.Nuclear ExperimentSIG_INEL
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"Table 10" of "Measurement of the low-energy antideuteron inelastic cross section"

2020

Inelastic interaction cross section of antiprotons on an averaged material element of the ALICE detector (2 sigma constraints).

5020.0Physics::Instrumentation and DetectorsP PB --> XHigh Energy Physics::ExperimentAntiproton inelastic c.s.Nuclear ExperimentSIG_INEL
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"Table 11" of "Measurement of the low-energy antideuteron inelastic cross section"

2020

Inelastic interaction cross section of antiprotons on an averaged material element of the ALICE detector (1 sigma constraints).

5020.0Physics::Instrumentation and DetectorsP PB --> XHigh Energy Physics::ExperimentAntiproton inelastic c.s.Nuclear ExperimentSIG_INEL
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"Table 9" of "Measurement of the low-energy antideuteron inelastic cross section"

2020

Inelastic interaction cross section of antiprotons on an averaged material element of the ALICE detector (1 sigma constraints).

5020.0Physics::Instrumentation and DetectorsP PB --> XHigh Energy Physics::ExperimentAntiproton inelastic c.s.Nuclear ExperimentSIG_INEL
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"Table 5" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

2017

pT-differential nuclear modification factor of heavy-flavour decay muons at backward rapidity (Pb-going side)

5020.0p PB --> MUON XPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 3" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

2017

pT-differential nuclear modification factor of heavy-flavour decay muons at backward rapidity (Pb-going side)

5020.0p PB --> MUON XPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentNuclear ExperimentSIG
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"Table 6" of "Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV"

2017

pT-differential forward-to-backward ratio of heavy-flavour decay muons

5020.0p PB --> MUON XPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentSIG
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Implementation of the ROD Crate DAQ Software for the ATLAS Tile Calorimeter and a Search for a MSSM Higgs Boson decaying into Tau pairs

2010

The ATLAS experiment of the LHC at CERN started its operation in 2009. The ROD Crate DAQ (RCD) as a part of the Trigger and Data Acquisition system (TDAQ) is responsible for the operation of the sub-­‐detector specific hardware at the level of the back-­‐end electronics crates. The RCD for the Tile Calorimeter is fully implemented. In first place, the specific Tile hardware and software is described in the configuration database. In second place, the various plug-­‐ins for the RCD that make use of sophisticated programming techniques are characterized. The RCD performance can be evaluated in terms of global DAQ efficiency, which is over 94% for the considered period in 2010 and in terms of …

53Physics::Instrumentation and DetectorsFísicaHigh Energy Physics::ExperimentDetectors and Experimental TechniquesParticle Physics - Experiment
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Sterile neutrinos as dark matter candidates

2021

In these brief lecture notes, we introduce sterile neutrinos as dark matter candidates. We discuss in particular their production via oscillations, their radiative decay, as well as possible observational signatures and constraints.

530 PhysicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::PhenomenologyFOS: Physical scienceshep-ph530 Physik01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsParticle Physics - PhenomenologySciPost Physics Lecture Notes
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