Search results for "detectors"

showing 10 items of 2229 documents

Radiation-hard semiconductor detectors for SuperLHC

2005

An option of increasing the luminosity of the Large Hadron Collider (LHC) at CERN to 10^35 cm^(- 2) s(- 1) has been envisaged to extend the physics reach of the machine. An efficient tracking down to a few centimetres from the interaction point will be required to exploit the physics potential of the upgraded LHC. As a consequence, the semiconductor detectors close to the interaction region will receive severe doses of fast hadron irradiation and the inner tracker detectors will need to survive fast hadron fluences of up to above 1016 cm 2. The CERN-RD50 project ''Development of Radiation Hard Semiconductor Devices for Very High Luminosity Colliders'' has been established in 2002 to explore…

Nuclear and High Energy Physicsradiation hard semiconductorsPhysics::Instrumentation and DetectorsSemiconductor detectorsRadiation Detector; LHCradiation hardness01 natural sciencesDefect engineeringSuper-LHCRadiation damageradiation detectorssilicon detectors0103 physical sciencesRadiation damageSuperLHCSilicon detectors; LHC; RD50 collaboration; radiation hardnessInstrumentationRadiation hardeningRadiation hardness010302 applied physicsPhysicsRadiation damage; Semiconductor detectors; Silicon particle detectors; Defect engineering; SLHC; Super-LHCLuminosity (scattering theory)Large Hadron ColliderRadiation DetectorInteraction pointRD50 collaboration010308 nuclear & particles physicsbusiness.industrySLHCDetectorRadiation hardness; silicon detectorsSemiconductor deviceSemiconductor detectorSilicon particle detectorsOptoelectronicsSilicon detectorsHigh Energy Physics::ExperimentLHCbusiness
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First Offline Results from the S3 Low-Energy Branch

2022

International audience; We present the first results obtained from the S3 Low-Energy Branch , the gas cell setup at SPIRAL2-GANIL, which will be installed behind the S3 spectrometer for atomic and nuclear spectroscopy studies of exotic nuclei. The installation is currently being commissioned offline, with the aim to establish optimum conditions for the operation of the radio frequency quadrupole ion guides, mass separation and ion bunching, providing high-efficiency and low-energy spatial spread for the isotopes of interest. Transmission and mass-resolving power measurements are presented for the different components of the S3-LEB setup. In addition, a single-longitudinal-mode, injection-lo…

Nuclear and High Energy Physicsresonance ionization laser spectroscopy; gas cell; hypersonic gas jets; radio frequency quadrupoles; nuclear ground state properties; isotope shift; hyperfine structurehyperfine structurespektroskopiatutkimuslaitteet[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Physics Atomic Molecular & Chemicalatomifysiikka[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]radio frequency quadrupolesScience & TechnologySPECTROSCOPY[PHYS.PHYS.PHYS-ATOM-PH]Physics [physics]/Physics [physics]/Atomic Physics [physics.atom-ph]Physicsgas cellLASER ION-SOURCECondensed Matter PhysicslasertekniikkaAtomic and Molecular Physics and Opticsresonance ionization laser spectroscopyisotope shiftnuclear ground state propertiesPhysical Scienceshypersonic gas jetsIONIZATIONydinfysiikkaSYSTEMAtoms
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Measurement of proton and nitrogen polarization in ammonia and a test of equal spin temperature

1998

The 1996 data taking of the SMC experiment used polarized protons to measure the spin-dependent structure function g(1) of the proton. Three liters of solid granular ammonia were irradiated at the Bonn electron linac in order to create the paramagnetic radicals which are needed for polarizing the protons. Proton polarizations of +/- (90 +/- 2.5)% were routinely reached. An analysis based on a theoretical line shape for spin-1. systems with large quadrupolar broadening was developed which allowed the nitrogen polarization in the ammonia to be determined with a 10% relative error. The measured quadrupolar coupling constant of N-14 agrees well with earlier extrapolated values. The polarization…

Nuclear and High Energy Physicsspin resonanceProtonp polarized targetNuclear Theorychemistry.chemical_elementAmmoniachemistry.chemical_compoundParamagnetismIrradiationDetectors and Experimental TechniquesNuclear ExperimentInstrumentationPhysicsCoupling constantpolarizationquadrupolar interactionsPolarization (waves)Nitrogennitrogen polarized targetdynamic nuclearnuclear magnetic resonancechemistryDeuteriump polarized target; nitrogen polarized target; spin resonanceAtomic physics
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The COMPASS experiment at CERN

2007

The COMPASS experiment makes use of the CERN SPS high-intensitymuon and hadron beams for the investigation of the nucleon spin structure and the spectroscopy of hadrons. One or more outgoing particles are detected in coincidence with the incoming muon or hadron. A large polarized target inside a superconducting solenoid is used for the measurements with the muon beam. Outgoing particles are detected by a two-stage, large angle and large momentum range spectrometer. The setup is built using several types of tracking detectors, according to the expected incident rate, required space resolution and the solid angle to be covered. Particle identification is achieved using a RICH counter and both…

Nuclear and High Energy Physicsstraw tube detectorPhysics::Instrumentation and DetectorsProject commissioningFOS: Physical sciencesfixed-target experimentRICH detectorhadron structureHigh Energy Physics - ExperimenttargetMWPCNuclear physicsHigh Energy Physics - Experiment (hep-ex)CompassHadron spectroscopyCOMPASS experimentscintillating fibre detectorNuclear Experimentsilicon microstrip detectorsInstrumentationSilicon microstrip detectorsPhysicsLarge Hadron ColliderStructure functionMicroMegas detectorfront-end electronicsDAQmicromegas detectordrift chamberPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentpolarisedGEM detectorcalorimetryParticle Physics - Experimentpolarised DISNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A gas ionisation Direct-STIM detector for MeV ion microscopy

2015

Abstract Direct-Scanning Transmission Ion Microscopy (Direct-STIM) is a powerful technique that yields structural information in sub-cellular whole cell imaging. Usually, a Si p-i-n diode is used in Direct-STIM measurements as a detector. In order to overcome the detrimental effects of radiation damage which appears as a broadening in the energy resolution, we have developed a gas ionisation detector for use with a focused ion beam. The design is based on the ETH Frisch grid-less off-axis Geiger–Muller geometry. It is developed for use in a MeV ion microscope with a standard Oxford Microbeams triplet lens and scanning system. The design has a large available solid angle for other detectors …

Nuclear and High Energy Physicsta114Physics::Instrumentation and Detectorsbusiness.industryChemistryResolution (electron density)DetectorTriplet lensMeV ion microscopeFocused ion beamionisation detectorOpticsIonizationRadiation damagedirect-STIMAtomic physicsbioimagingbusinessInstrumentationField ion microscopeReNcells VMDiodeNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Underground multi-muon experiment EMMA

2011

EMMA is a new experiment designed for cosmic- ray composition studies around the knee energy operating at the shallow depth underground in the Pyh¨ asalmi mine, Fin- land. The array has sufficient coverage and resolution to de- termine the multiplicity, the lateral density distribution and the arrival direction of high-energy muons on an event by event basis. Preliminary results on the muon multiplicity ex- tracted using one detector station of the array are presented.

Nuclear physicsPhysicsCOSMIC cancer databaseMuonPhysics and Astronomy (miscellaneous)Density distributionPhysics::Instrumentation and DetectorsDetectorHigh Energy Physics::ExperimentAstronomy and AstrophysicsAstrophysics and Space Sciences Transactions
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The “Physics Beyond Colliders” Projects for the CERN M2 Beam

2019

Abstract Physics Beyond Colliders is an exploratory study aimed at exploiting the full scientific potential of CERN’s accelerator complex up to 2040 and its scientific infrastructure through projects complementary to the existing and possible future colliders. Within the Conventional Beam Working Group (CBWG), several projects for the M2 beam line in the CERN North Area were proposed, such as a successor for the COMPASS experiment, a muon programme for NA64 dark sector physics, and the MuonE proposal aiming at investigating the hadronic contribution to the vacuum polarisation. We present integration and beam optics studies for 100 – 160 GeV/c muon beams as well as an outlook for improvement…

Nuclear physicsPhysicsHistoryLarge Hadron ColliderPhysics::Instrumentation and DetectorsPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentBeam (structure)Computer Science ApplicationsEducationJournal of Physics: Conference Series
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Calculation of total muon flux observed by Muon Monitor experiment

2017

An approach to calculate the flux of cosmicgenic muons detected by Muon Monitor experiment in lab LAB2400 of the Underground Laboratory in Canfranc (LSC) is described. The measuring apparatus consists of three layers of SC16 scintillation matrix detectors. The hardware function of the detector assembly was determined using computer simulation. Obtained value of the total muon ux turned out to be equal to (4.35 ± 0.2) × 10−3 m −2 s −1.

Nuclear physicsPhysicsHistoryScintillationMuonPhysics::Instrumentation and DetectorsMuon fluxDetectorUnderground laboratoryFluxHigh Energy Physics::ExperimentComputer Science ApplicationsEducationJournal of Physics: Conference Series
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Heavy flavour production and fragmentation

2001

We review theoretical and experimental results relevant to charm and bottom physics. In particular, we consider charmonium and open heavy-flavour production at Tevatron, LEP and HERA colliders, and in heavy-ion scattering. We study the prospect of future b-physics measurement at the LHC with the ATLAS and CMS detectors.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFlavourTevatronHigh Energy Physics::ExperimentHERANuclear ExperimentJournal of Physics G: Nuclear and Particle Physics
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Measurement of the mass and width of the charmed meson D∗+ (2010)

1992

Abstract Using a high-resolution silicon vertex detector we have observed a very clean signal of 127 D∗+. After a careful study of the experimental resolution of our apparatus we have measured m( D ∗++ )−m( D 0 ) = 145.39±0.06±0.03 MeV . We have also obtained a 90% CL upper limit to γ(D∗+) of 131 keV.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsMesonPhysics::Instrumentation and DetectorsResolution (electron density)High Energy Physics::ExperimentLimit (mathematics)SignalParticle Physics - ExperimentSilicon vertex detectorPhysics Letters B
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