Search results for "Semiconductor device"

showing 10 items of 60 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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Unified model of fractal conductance fluctuations for diffusive and ballistic semiconductor devices

2006

We present an experimental comparison of magnetoconductance fluctuations measured in the ballistic, quasiballistic, and diffusive scattering regimes of semiconductor devices. In contradiction to expectations, we show that the spectral content of the magnetoconductance fluctuations exhibits an identical fractal behavior for these scattering regimes and that this behavior is remarkably insensitive to device boundary properties. We propose a unified model of fractal conductance fluctuations in the ballistic, quasiballistic, and diffusive transport regimes, in which the generic fractal behavior is generated by a subtle interplay between boundary and material-induced chaotic scattering events.

PhysicsCondensed matter physicsScatteringConductanceBoundary (topology)Semiconductor deviceUnified ModelCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsElectronic Optical and Magnetic Materials[SPI]Engineering Sciences [physics]FractalQuantum dotChaotic scatteringStatistical physicsPhysical Review B
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Stationary semiconductor equations

1996

The behaviour of a semiconductor device is usually modelled by three coupled nonlinear partial differential equations of elliptic type. Such a system for the transport of mobile charge carriers was first introduced by Van Roosbroeck [Van Roosbroeck] in 1950. Nowadays there are many models which differ in their choice of unknowns, scales, various types of nonlinearities etc. (see, e.g., [Brezzi], [Groger], [Markowich], [Markowich, Ringhofer, Schmeiser], [Mock, 1972], [Polak, den Heijer, Schilders, Markowich], [Pospisek], [Pospisek, Segeth, Silhan], [Selberherr], [Sze], [Zlamal, 1986]).

PhysicsNonlinear systemPartial differential equationElliptic typeMathematical analysisMobile chargeSemiconductor equationsSemiconductor device
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A comparison of the performance of irradiated p-in-n and n-in-n silicon microstrip detectors read out with fast binary electronics

2000

Abstract Both n-strip on n-bulk and p-strip on n-bulk silicon microstrip detectors have been irradiated at the CERN PS to a fluence of 3×10 14 p cm −2 and their post-irradiation performance compared using fast binary readout electronics. Results are presented for test beam measurements of the efficiency and resolution as a function of bias voltage made at the CERN SPS, and for noise measurements giving detector strip quality. The detectors come from four different manufacturers and were made as prototypes for the SemiConductor Tracker of the ATLAS experiment at the CERN LHC.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderPhysics::Instrumentation and Detectorsbusiness.industryATLAS experimentDetectorBiasingSemiconductor deviceParticle detectorMicrostripSemiconductor detectorOptoelectronicsHigh Energy Physics::ExperimentbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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High Voltage Monolithic Active Pixel Sensors

2018

Ever higher demands on resolution and rate capability drive the development of particle tracking detectors. Especially at low momenta, multiple Coulomb scattering in the material of the detector is also strongly affecting the resolution of momentum measurements. While gas-based detectors such as drift chambers and time projection chambers can be built with very small amounts of material, their rate capability is limited by ageing and space charge effects. Hybrid semiconductor detectors on the other hand combine a depleted (silicon) sensor with a custom amplifier and readout chip. Pixelated devices especially can operate efficiently in very harsh rate and radiation environments such as the i…

PhysicsNuclear and High Energy PhysicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsbusiness.industryAmplifierDetectorHigh voltageSemiconductor deviceTracking (particle physics)Chip01 natural sciencesSpace charge030218 nuclear medicine & medical imagingSemiconductor detector03 medical and health sciences0302 clinical medicine0103 physical sciencesOptoelectronicsbusinessNuclear Physics News
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2.45 GHz synchronised polarised electron injection at MAMI

1998

Abstract A semiconductor modelocked diode laser has been used to produce picosecond spin-polarised electron bunches from strained GaAsP photocathodes and inject them into MAMI, synchronised to the 2.45 GHz accelerating field. The laser meets the operational requirements of MAMI producing stable electron beams, with a polarisation purity of 72% and a transmission efficiency of 52% at an accelerated beam current of 10.1 μA.

PhysicsNuclear and High Energy Physicsbusiness.industryCyclotronSemiconductor deviceLaserCathodelaw.inventionSemiconductor laser theorySemiconductorOpticslawPicosecondOptoelectronicsbusinessInstrumentationDiodeNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Multi-Scale Modeling of Quantum Semiconductor Devices

2006

This review is concerned with three classes of quantum semiconductor equations: Schrodinger models, Wigner models, and fluid-type models. For each of these classes, some phenomena on various time and length scales are presented and the connections between micro-scale and macro-scale models are explained. We discuss Schrodinger-Poisson systems for the simulation of quantum waveguides and illustrate the importance of using open boundary conditions. We present Wigner-based semiconductor models and sketch their mathematical analysis. In particular we discuss the Wigner-Poisson-Focker-Planck system, which is the starting point of deriving subsequently the viscous quantum hydrodynamic model. Furt…

PhysicsOpen quantum systemsymbols.namesakeSemiconductor device modelingInelastic collisionsymbolsWigner distribution functionBoundary value problemStatistical physicsSemiconductor process simulationQuantumSchrödinger's cat
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MuPix7 - A fast monolithic HV-CMOS pixel chip for Mu3e

2016

The MuPix7 chip is a monolithic HV-CMOS pixel chip, thinned down to 50 \mu m. It provides continuous self-triggered, non-shuttered readout at rates up to 30 Mhits/chip of 3x3 mm^2 active area and a pixel size of 103x80 \mu m^2. The hit efficiency depends on the chosen working point. Settings with a power consumption of 300 mW/cm^2 allow for a hit efficiency >99.5%. A time resolution of 14.2 ns (Gaussian sigma) is achieved. Latest results from 2016 test beam campaigns are shown.

PhysicsPhysics - Instrumentation and DetectorsPixel010308 nuclear & particles physicsbusiness.industryGaussianFOS: Physical sciencesTime resolutionInstrumentation and Detectors (physics.ins-det)Semiconductor deviceChip01 natural sciencessymbols.namesakeCMOSTest beam0103 physical sciencessymbolsOptoelectronicsddc:610010306 general physicsbusinessInstrumentationGaussian processMathematical Physics
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Monte Carlo Analysis of Voltage-Current Characteristic Nonlinearity and Harmonic Generation in Submicron Semiconductor Structures

2006

Using a multiparticles Monte Carlo technique, we investigate the dependence of the nonlinear carrier dynamics in GaAs n+nn+ structures operating under very intense sub-terahertz signals from some process parameters as: i) the frequency and the intensity of the excitation signal and ii) the length of the n region

Physicsbusiness.industryMonte Carlo methodSemiconductor deviceComputational physicsGallium arsenideNonlinear systemchemistry.chemical_compoundSemiconductorchemistryHigh harmonic generationOptoelectronicsbusinessIntensity (heat transfer)Voltage2006 25th International Conference on Microelectronics
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Size dependent light absorption modulation and enhanced carrier transport in germanium quantum dots devices

2015

Quantum confinement in closely packed arrays of Ge quantum dots (QDs) was studied for energy applications. In this work, we report an efficient tuning mechanism of the light harvesting and detection of Ge QDs. Thin films of SiGeO alloys, produced by rf-magnetron sputtering, were annealed at 600 degrees C in N-2 to induce precipitation of small amorphous Ge QDs into the oxide matrix. Varying the Ge content, the QD size was tailored between 2 and 4 nm, as measured by high resolution transmission electron microscopy. X-ray photoelectron spectroscopy (XPS) measurements indicate the formation of pure SiO2, as well as the presence of a sub-stoichiometric Ge oxide shell at the QD interface. Light …

Precipitation (chemical)Materials scienceAmorphous alloyBand gapchemistry.chemical_elementHigh resolution transmission electron microscopyPhotoconductive gainGermaniumNanocrystalMetal-insulator semiconductor deviceSettore ING-INF/01 - ElettronicaSettore FIS/03 - Fisica Della MateriaAbsorption spectroscopyQuantum confinement effectQuantum confinementElectromagnetic wave absorptionLight absorptionThin filmGermanium oxideOxide filmHigh-resolution transmission electron microscopyGermanium quantum dotPotential wellMIS deviceAmorphous filmGermaniumQuantum dotsRenewable Energy Sustainability and the Environmentbusiness.industryPhotoconductivitySolar cellPreferential trappingMIM deviceSemiconductor deviceSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsPhotovoltaicschemistryMetal insulator boundarieQuantum dotrf-Magnetron sputtering Semiconductor quantum dotOptoelectronicsCharge carrierX ray photoelectron spectroscopy Effective mass approximationbusinessQuantum chemistryPhotovoltaicMagnetron sputteringSolar Energy Materials and Solar Cells
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