Search results for "semiconductor"

showing 10 items of 974 documents

Cooling of the plasma chamber for the AECR-U type electron cyclotron resonance ion source ARTEMIS

2001

Abstract The temperature distribution inside the ECRIS plasma chamber has been studied using finite element analysis. The main goal of these studies was to find out the safest cooling design for the temperature sensitive permanent magnets. In ECR ion sources they are used to provide the hexapole field. Two different designs for the cooling of the magnets were investigated. The temperature distribution on the surface of the plasma electrode was also studied. With the aid of the cooling simulations the most efficient cooling for the new ECR ion source was found. As a result of which, safety and higher reliability of operation can be reached.

Nuclear and High Energy PhysicsReliability (semiconductor)Field (physics)Physics::Plasma PhysicsChemistryMagnetElectrodePlasmaAtomic physicsInstrumentationIon sourceElectron cyclotron resonanceIonNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Silicon detectors for the sLHC

2011

In current particle physics experiments, silicon strip detectors are widely used as part of the inner tracking layers. A foreseeable large-scale application for such detectors consists of the luminosity upgrade of the Large Hadron Collider (LHC), the super-LHC or sLHC, where silicon detectors with extreme radiation hardness are required. The mission statement of the CERN RD50 Collaboration is the development of radiation-hard semiconductor devices for very high luminosity colliders. As a consequence, the aim of the RandD programme presented in this article is to develop silicon particle detectors able to operate at sLHC conditions. Research has progressed in different areas, such as defect …

Nuclear and High Energy PhysicsSiliconPhysics::Instrumentation and DetectorsLHC; High luminosity collider; radiation damageCharge collection efficiencychemistry.chemical_elementHigh luminosity colliderTracking (particle physics)Nuclear physicsRadiation damageSilicon particle detectors; Radiation damage; Irradiation; Charge collection efficiencyInstrumentationRadiation hardeningPhysicsLuminosity (scattering theory)Large Hadron ColliderDetectorSemiconductor deviceEngineering physicsSilicon particle detectorschemistryHigh Energy Physics::ExperimentIrradiationLHCParticle physics experiments
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Stopping power measurement of 48Ca in a broad energy range in solid absorbers

2006

Abstract Stopping power of 48 Ca ions in C, Ni and Au was measured using TOF-E method. The results cover energy range from 0.1 to 5.3 MeV/u (5–250 MeV). The reliability of our experimental method was verified and confirmed by TOF–TOF measurements. The results are compared with theoretical (PASS) and semi empirical (SRIM2003) predictions.

Nuclear and High Energy PhysicsTime of flightRange (particle radiation)Reliability (semiconductor)ChemistryStopping power (particle radiation)Atomic physicsInstrumentationEnergy (signal processing)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Determination of absolute internal conversion coefficients using the SAGE spectrometer

2016

Abstract A non-reference based method to determine internal conversion coefficients using the SAGE spectrometer is carried out for transitions in the nuclei of 154 Sm, 152 Sm and 166 Yb. The Normalised-Peak-to-Gamma method is in general an efficient tool to extract internal conversion coefficients. However, in many cases the required well-known reference transitions are not available. The data analysis steps required to determine absolute internal conversion coefficients with the SAGE spectrometer are presented. In addition, several background suppression methods are introduced and an example of how ancillary detectors can be used to select specific reaction products is given. The results o…

Nuclear and High Energy Physicselectron spectroscopy01 natural sciencesParticle detectorInternal conversionOptics0103 physical sciences010306 general physicsInternal conversion coefficientInstrumentationsilicon detectorbackground subtractionenergy reconstructionPhysicsBackground subtractionSpectrometerta114010308 nuclear & particles physicsbusiness.industry3. Good healthComputational physicsSemiconductor detectorMeasuring instrumentbusinessRadioactive decayinternal conversion coefficientNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Efficiency and timing performance of the MuPix7 high-voltage monolithic active pixel sensor

2018

The MuPix7 is a prototype high voltage monolithic active pixel sensor with 103 times 80 um2 pixels thinned to 64 um and incorporating the complete read-out circuitry including a 1.25 Gbit/s differential data link. Using data taken at the DESY electron test beam, we demonstrate an efficiency of 99.3% and a time resolution of 14 ns. The efficiency and time resolution are studied with sub-pixel resolution and reproduced in simulations.

Nuclear and High Energy Physicsirradiation [electron]Physics - Instrumentation and DetectorsFOS: Physical sciencesElectron01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesddc:530DESY Lab010306 general physicsnumerical calculationsInstrumentationtime resolutionPhysicspixel [semiconductor detector]CMOS sensorPixel010308 nuclear & particles physicsbusiness.industryResolution (electron density)High voltageDESYTime resolutionInstrumentation and Detectors (physics.ins-det)Test beamefficiencyOptoelectronicsbusinessperformance
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High performance detector head for PET and PET/MR with continuous crystals and SiPMs

2012

International audience; A high resolution PET detector head for small animal PET applications has been developed. The detector is composed of a 12 mm x 12 mm source continuous LYSO crystal coupled to a 64-channel monolithic SiPM matrix from FBK-irst. Crystal thicknesses of 5 mm and 10 mm have been tested, both yielding an intrinsic spatial resolution around 0.7 mm FWHM with a position determination algorithm that can also provide depth-of-interaction information. The detectors have been tested in a rotating system that makes it possible to acquire tomographic data and reconstruct images of 22Na sources. An image reconstruction method specifically adapted for continuous crystals has been emp…

Nuclear and High Energy Physicsmedicine.medical_specialtySiPMIterative reconstruction01 natural sciencesParticle detectorLyso-030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineOpticsSilicon photomultiplier0103 physical sciencesmedicineMedical physicsHigh resolution[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/MicroelectronicsInstrumentationImage resolutionPhysics010308 nuclear & particles physicsbusiness.industryDetectorPosition determinationSemiconductor detectorFull width at half maximumMG-APDPETMonolithic crystalsbusiness
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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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Hypernuclear physics at $\overline{\mbox{P}}$ ANDA

2012

Hypernuclear research will be one of the main topics addressed by the \(\overline{\mbox{P}}\) anda experiment at the planned Facility for Anti-proton and Ion Research FAIR at Darmstadt, Germany. A copious production of Ξ-hyperons at a dedicated internal target in the stored anti-proton beam is expected, which will enable the high-precision γ-spectroscopy of double strange systems for the first time. In addition to the general purpose \(\overline{\mbox{P}}\) anda setup, the hypernuclear experiments require an active secondary target of silicon layers and absorber material as well as high purity germanium (HPGe) crystals as γ-detectors. The design of the setup and the development of these det…

Nuclear physicsPhysicsParticle physicsPionSiliconchemistryDetectorMonte Carlo methodchemistry.chemical_elementProduction (computer science)StrangenessBeam (structure)Semiconductor detector
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Heavy ion and proton test site at JYFL-accelerator laboratory

1999

Abstract A radiation effects facility (RADEF) has been installed in the Accelerator Laboratory of the Department of Physics, University of Jyvaskyla (JYFL). The facility includes a special beam line dedicated to irradiation studies of semiconductor components and devices. It consists of a vacuum chamber including component movement apparatus and the necessary diagnostic equipment required for beam quality and intensity analysis. Construction of the station began in the summer of 1996, and in August 1997 the suitability of the station for space applications was evaluated. In this paper we introduce the accelerator laboratory along with the test station and its properties. We also describe th…

Nuclear physicsPhysicsProton (rocket family)Nuclear and High Energy PhysicsTest siteBeamlineNuclear engineeringHeavy ionVacuum chamberLaser beam qualityInstrumentationElectron cyclotron resonanceSemiconductor componentsNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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10Li low-lying resonances populated by one-neutron transfer

2015

The 9Li + 2H → 10Li + 1H one-neutron transfer reaction has been performed at 100 MeV incident energy at TRIUMF using a 9Li beam delivered by the ISAC-II facility. A setup based on double-sided silicon strip detectors has been used in order to detect and identify the outgoing 9Li produced by the 10Li breakup at forward angles and the recoil protons emitted at backward angles. The 10Li low-lying resonances, whose energies, widths and configurations are still unclear, have been populated with significant statistics.

Nuclear reactionChemistryNuclear TheoryHadronParticle detectorSemiconductor detectorNuclear physicsRecoilPhysics::Accelerator PhysicsNeutronAtomic physicsNuclear ExperimentNucleonBeam (structure)
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