Search results for " detector"

showing 10 items of 2719 documents

"Table 1" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

2012

pT-differential production cross section of muons from heavy flavour decays, in the rapidity range 2.5

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology7000.0Muon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringP P --> BOTTOM BOTTOMBAR XHigh Energy Physics::ExperimentDSIG/DPTP P --> MU+ MU- XTransverse Momentum Dependence
researchProduct

"Table 6" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

2012

pT-differential production cross section of muons from heavy flavour decays, in the rapidity range 3.4

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology7000.0Muon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringP P --> BOTTOM BOTTOMBAR XHigh Energy Physics::ExperimentDSIG/DPTP P --> MU+ MU- XTransverse Momentum Dependence
researchProduct

"Table 5" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

2012

pT-differential production cross section of muons from heavy flavour decays, in the rapidity range 3.1

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology7000.0Muon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringP P --> BOTTOM BOTTOMBAR XHigh Energy Physics::ExperimentDSIG/DPTP P --> MU+ MU- XTransverse Momentum Dependence
researchProduct

"Table 4" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

2012

pT-differential production cross section of muons from heavy flavour decays, in the rapidity range 2.8

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyP P --> BOTTOM BOTTOMBAR < MU+ X > X7000.0Muon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringHigh Energy Physics::ExperimentDSIG/DPTP P --> MU+ MU- XTransverse Momentum Dependence
researchProduct

"Table 2" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

2012

y-differential production cross section of muons from heavy flavour decays, in the range 2

Di-Muon ProductionPhysics::Instrumentation and DetectorsHigh Energy Physics::LatticeRapidity DependenceHigh Energy Physics::Phenomenology7000.0DSIG/DYRAPMuon productionInclusiveSingle Differential Cross SectionP P --> CHARM CHARMBAR XProton-Proton ScatteringP P --> BOTTOM BOTTOMBAR XPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentP P --> MU+ MU- X
researchProduct

"Table 2" of "Search for light scalar top quark pair production in final states with two leptons with the ATLAS detector in sqrt(s) = 7 TeV proton-pr…

2012

Distribution of the PT of the leading muon for MU-MU events in the Signal Region, before the application of the leading lepton PT cut.

Di-Muon ProductionProton-Proton ScatteringPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyExclusiveTop7000.0High Energy Physics::ExperimentJet ProductionMuon productionP P --> MU+ MU- JET(S) MM
researchProduct

Measurement of the inelastic proton-proton cross-section at √s = 7 TeV with the ATLAS detector

2011

The dependence of the rate of proton–proton interactions on the centre-of-mass collision energy, √s, is of fundamental importance for both hadron collider physics and particle astrophysics. The dependence cannot yet be calculated from first principles; therefore, experimental measurements are needed. Here we present the first measurement of the inelastic proton–proton interaction cross-section at a centre-of-mass energy, √s, of 7 TeV using the ATLAS detector at the Large Hadron Collider. Events are selected by requiring hits on scintillation counters mounted in the forward region of the detector. An inelastic cross-section of 60.3±2.1 mb is measured for ξ>5×10[superscript −6], where ξ is ca…

DiffractionAtlas detectorNuclear TheoryGeneral Physics and AstronomyPP01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ComputingMilieux_MISCELLANEOUSddc:539PhysicsMultidisciplinaryLarge Hadron Colliderphysical sciences; particle physicsSettore FIS/01 - Fisica SperimentaleSoftATLASDiffraction DissociationPhotoproductionElastic-ScatteringScintillation counterComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCddc:500Particle Physics - ExperimentParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2High-Energies530General Biochemistry Genetics and Molecular BiologyArticleNuclear physicsphysical sciencesinelastic; proton–proton cross-section;ATLAS detector0103 physical sciencesAmplitudesHigh Energy Physicsparticle physics010306 general physicsAstroparticle physicsHardScience & Technology010308 nuclear & particles physicsGeneral ChemistryCollisionExperimental High Energy PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentModel
researchProduct

High-energy X-ray diffraction and topography investigation of CdZnTe

2005

High-energy transmission x-ray diffraction techniques have been applied to investigate the crystal quality of CdZnTe (CZT). CdZnTe has shown excellent performance in hard x-ray and gamma detection; unfortunately, bulk nonuniformities still limit spectroscopic properties of CZT detectors. Collimated high-energy x-rays, produced by a superconducting wiggler at the National Synchrotron Light Source’s X17B1 beamline, allow for a nondestructive characterization of thick CZT samples (2–3 mm). In order to have complete information about the defect distribution and strains in the crystals, two series of experiments have been performed. First, a monochromatic 67 keV x-ray beam with the size of 300×3…

DiffractionMaterials sciencebusiness.industryWigglerSynchrotron radiationCondensed Matter PhysicsCollimated lightElectronic Optical and Magnetic MaterialsCrystalFull width at half maximumOpticsradiation detectorsBeamlineCadmium alloysMaterials ChemistryCadmium tellurideElectrical and Electronic EngineeringRaster scanbusinessJournal of Electronic Materials
researchProduct

Wideband THz time domain spectroscopy based on optical rectification and electro-optic sampling

2013

We present an analytical model describing the full electromagnetic propagation in a THz time-domain spectroscopy (THz-TDS) system, from the THz pulses via Optical Rectification to the detection via Electro Optic-Sampling. While several investigations deal singularly with the many elements that constitute a THz-TDS, in our work we pay particular attention to the modelling of the time-frequency behaviour of all the stages which compose the experimental set-up. Therefore, our model considers the following main aspects: (i) pump beam focusing into the generation crystal; (ii) phase-matching inside both the generation and detection crystals; (iii) chromatic dispersion and absorption inside the c…

DiffractionTA1501Optical rectificationComputer scienceTerahertz radiationTerahertz radiationPhysics::OpticsSettore ING-INF/01 - ElettronicaArticleCrystalElectro-optic samplingOptical rectificationOpticsSampling (signal processing)Dispersion (optics)Thz time domain spectroscopyWidebandSpectroscopyAbsorption (electromagnetic radiation)Multidisciplinarybusiness.industrySettore ING-INF/02 - Campi ElettromagneticiQC0450Terahertz detectorsTerahertz sourcebusinessTelecommunicationsBeam (structure)
researchProduct

Performance of a new real time digital pulse processing system for X-ray and gamma ray semiconductor detectors

2014

New generation spectroscopy systems have advanced towards digital pulse processing (DPP) approaches. DPP systems, based on direct digitizing and processing of detector signals, have recently been favoured over analog pulse processing electronics, ensuring better performance. In this work, we present the performance of a new real time DPP system for X-ray and gamma ray semiconductor detectors. The system is based on a commercial digitizer equipped with a custom DPP firmware, developed by our group, for on-line pulse shape and height analysis. X-ray and gamma ray spectra measurements with cadmium telluride (CdTe) and germanium (Ge) detectors, coupled to resistive feedback preamplifiers, will …

Digital Pulse Processing Semiconductor detectors X-ray and gamma ray spectroscopySettore FIS/01 - Fisica SperimentaleSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)
researchProduct