Search results for "detector"

showing 10 items of 3491 documents

Deployment of the ATLAS High-Level Trigger

2006

The ATLAS combined test beam in the second half of 2004 saw the first deployment of the ATLAS High-Level Trigger (HLT). The next steps are deployment on the pre-series farms in the experimental area during 2005, commissioning and cosmics tests with the full detector in 2006 and collisions in 2007. This paper reviews the experience gained in the test beam, describes the current status and discusses the further enhancements to be made. We address issues related to the dataflow, integration of selection algorithms, testing, software distribution, installation and improvements.

Nuclear and High Energy PhysicsDataflowCluster (spacecraft)01 natural sciencesAtlas (anatomy)testbeam0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]medicineElectrical and Electronic EngineeringSelection algorithmSimulationhigh-level triggersPhysicshigh-energy physics010308 nuclear & particles physicsbusiness.industryDetectorATLASSoftware distributionTriggertriggeringmedicine.anatomical_structureNuclear Energy and EngineeringClustersoftware integrationSoftware deploymentSystems engineeringSystem integrationLHCbusinessIEEE Transactions on Nuclear Science
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Dosimetry for electron Intra-Operative RadioTherapy: Comparison of output factors obtained through alanine/EPR pellets, ionization chamber and Monte …

2015

Abstract In this work a comparison between the response of alanine and Markus ionization chamber was carried out for measurements of the output factors (OF) of electron beams produced by a linear accelerator used for Intra-Operative Radiation Therapy (IORT). Output factors (OF) for conventional high-energy electron beams are normally measured using ionization chamber according to international dosimetry protocols. However, the electron beams used in IORT have characteristics of dose per pulse, energy spectrum and angular distribution quite different from beams usually used in external radiotherapy, so the direct application of international dosimetry protocols may introduce additional uncer…

Nuclear and High Energy PhysicsDosimeterPhysics::Instrumentation and DetectorsChemistryIORTSettore FIS/01 - Fisica SperimentalePhysics::Medical PhysicsMonte Carlo methodDetectorGeant4Dose profileElectronalanine dosimetry Monte Carlo Simulation Geant4Alanine dosimetrySettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Linear particle acceleratorMonte Carlo simulationsComputational physicsNuclear magnetic resonanceIonization chamberDosimetrySettore MED/36 - Diagnostica Per Immagini E RadioterapiaInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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A Time Projection Chamber with GEM-Based Readout

2016

For the International Large Detector concept at the planned International Linear Collider, the use of time projection chambers (TPC) with micro-pattern gas detector readout as the main tracking detector is investigated. In this paper, results from a prototype TPC, placed in a 1 T solenoidal field and read out with three independent GEM-based readout modules, are reported. The TPC was exposed to a 6 GeV electron beam at the DESY II synchrotron. The efficiency for reconstructing hits, the measurement of the drift velocity, the space point resolution and the control of field inhomogeneities are presented.

Nuclear and High Energy PhysicsDrift velocityPhysics - Instrumentation and DetectorsInternational Linear ColliderMicropattern gaseous detectors (MPGD)Physics::Instrumentation and DetectorsFOS: Physical sciencesTracking (particle physics)01 natural scienceslaw.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]Gas electron multipliers (GEM)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]International Large Detector (ILD)electron: irradiationtracking detector[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniques010306 general physicsInstrumentationspatial resolution[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Physicsmagnetic field: spatial distributionInternational Linear Collider (ILC)Time projection chamber010308 nuclear & particles physicsILD detectorDetectordrift velocityDESYInstrumentation and Detectors (physics.ins-det)Synchrotrontime projection chamberefficiencygas electron multiplierGas electron multiplierPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentTime projection chambers (TPC)
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Observation of orbitally excited B mesons

1995

Experimental evidence for the existence of orbitally excited B meson states is presented in an analysis of the Bπ and B*π distribution of Q = m(B**) - m(B(*)) - m(π) using Z0decay data taken with the DELPHI detector at LEP. The mean Q-value of the decays B**→ B(*)π is measured to be 284 ± 5 (stat.) ± 15 (syst.) MeV/c2, and the Gaussian width of the signal is 79 ± 5 (stat.) ± 8 (syst.) MeV/c2. This signal can be described as a single resonance of mass m = 5732 ± 5 (stat.) ± 20 (syst.) MeV/c2and full width Γ = 145 ± 28 MeV/c2. The observed shape is also consistent with the production of several broad and narrow states as predicted by the quark model and partly observed in the D-…

Nuclear and High Energy PhysicsE+E ANNIHILATIONLUND MONTE-CARLOElectron–positron annihilationDELPHI; B meson; fragmentation; b-jetB meson01 natural sciencesResonance (particle physics)Full widthPartícules (Física nuclear)JET FRAGMENTATIONDECAYSNuclear physicsPHYSICSfragmentation0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B meson010306 general physicsNuclear ExperimentDetectors de radiacióDELPHIPhysics010308 nuclear & particles physicsQuark modelb-jetLARGE ELECTRON POSITRON COLLIDERExcited statePARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSHigh Energy Physics::ExperimentLUND MONTE-CARLO; JET FRAGMENTATION; E+E ANNIHILATION; DECAYS; PHYSICSParticle Physics - ExperimentProduction ratePhysics Letters B
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Lateral distribution of muons in IceCube cosmic ray events

2013

In cosmic ray air showers, the muon lateral separation from the center of the shower is a measure of the transverse momentum that the muon parent acquired in the cosmic ray interaction. IceCube has observed cosmic ray interactions that produce muons laterally separated by up to 400 m from the shower core, a factor of 6 larger distance than previous measurements. These muons originate in high pT (>2  GeV/c) interactions from the incident cosmic ray, or high-energy secondary interactions. The separation distribution shows a transition to a power law at large values, indicating the presence of a hard pT component that can be described by perturbative quantum chromodynamics. However, the ra…

Nuclear and High Energy PhysicsENERGIESPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesCosmic rayAstrophysicsddc:500.201 natural sciences7. Clean energyPower lawIceCubeHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)0103 physical sciencescosmic radiation : interactionddc:530Charm (quantum number)Ultra-high-energy cosmic ray010306 general physicsZenithPhysicsQuantum chromodynamicsHigh Energy Astrophysical Phenomena (astro-ph.HE)Muon010308 nuclear & particles physicsAstrophysics::Instrumentation and Methods for AstrophysicsGluonMODELPhysics and Astronomy13. Climate actionTEVHigh Energy Physics::ExperimentGLUONAstrophysics - High Energy Astrophysical Phenomena
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Angular distributions in the decay B -> K*l(+)l(-)

2009

We use a sample of 384 million BBbar events collected with the Babar detector at the PEP-II e+e- collider to study angular distributions in the rare decays B -> K* l+l-, where l+l- is either e+e- or mu+mu-. For low dilepton invariant masses, m(l+l-)3.2$ GeV/c^2, we measure AFB=0.76 (+0.52,-0.32) +/- 0.07 FL=0.71 (+0.20,-0.22) +/- 0.04.

Nuclear and High Energy PhysicsElectron–positron annihilationBABAReducationPARTICLE PHYSICS; PEP2; BABAR01 natural sciencesbehavioral disciplines and activitiesHigh Energy Physics - ExperimentNuclear physicsParticle decayAngular distribution0103 physical sciencesPEP2[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B meson010306 general physicsPhysics010308 nuclear & particles physicsParticle physicsBABAR detectorHEPPair production13.20.HeBaBarPARTICLE PHYSICSFísica de partículesExperiments
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Auto-Adaptive Trigger and Pulse Extraction for Digital Processing in Nuclear Instrumentation

2015

International audience; This paper presents a novel auto-adaptive method for pulse triggering and extraction. Pulse triggering uses a threshold that must be placed as close as possible to the noise level. We do this by means of an adaptive threshold level based on real-time noise level estimation. A dynamic estimation of the pulse length is also used for pulse selection. The proposed approach is largely insensitive to noise and enables autonomous extraction of pulses regardless of their shape, height or length. The proposed approach can be used with numerous types of detectors from an analog-to-digital converter, and can be used in conjunction with various pulse processing techniques such a…

Nuclear and High Energy PhysicsEngineeringNoise (signal processing)business.industryDetectorPulse durationData acquisitionPulse processingtriggerPulse (physics)NOISEdigital pulse processing (DPP)Nuclear Energy and Engineering[INFO.INFO-TS]Computer Science [cs]/Signal and Image ProcessingElectronic engineeringDETECTORSExtraction (military)Instrumentation (computer programming)[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Electrical and Electronic EngineeringNoise levelbusinessdigital signal processing (DSP)nuclear instrumentation
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A Portable Readout System for Microstrip Silicon Sensors (ALIBAVA)

2009

A readout system for microstrip silicon sensors has been developed. This system is able to measure the collected charge in one or two microstrip silicon sensors by reading out all the channels of the sensor(s), up to 256. The system can operate either with non-irradiated and irradiated sensors as well as with n-type and p-type microstrip silicon sensors. Heavily irradiated sensors will be used at the Super Large Hadron Collider, so this system can be used to research the performance of microstrip silicon sensors in conditions as similar as possible to the Super Large Hadron Collider operating conditions. The system has two main parts: a hardware part and a software part. The hardware part a…

Nuclear and High Energy PhysicsEngineeringanalog processing circuitsMotherboardPhysics::Instrumentation and DetectorsInterface (computing)Analog-digital conversionFPGAshigh energy physics instrumentationUSBMicrostripChargelaw.inventionCharge sensitive amplifiersData acquisitionmicroprocessorslawlogic designElectrical and Electronic Engineeringdetector instrumentationtime to digitalbusiness.industryReading (computer)electronicsDetectorElectrical engineeringConvertersCollectionsfront-end electronicssemiconductor detectorsNuclear Energy and Engineeringdata acquisition systemsdigital integrated circuitsbusinessDaughterboard
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Fast and compact data acquisition for gas-filled detectors with delay line

2004

This article describes the functionality, implementation and performance of a PCI data acquisition board that can be used in conjunction with gas-filled detectors with delay line readout. The board combines a large on-board 256-MByte histogramming memory with a maximum 10-MHz count rate in continuous operation and integrates the time frame generation, histogram building and buffering functionalities in a single PCI board, resulting in a fast, compact and cost-effective data acquisition solution for the Spanish beamline BM16 at ESRF.

Nuclear and High Energy PhysicsEngineeringbusiness.industryContinuous operationDetectorData acquisitionNuclear Energy and EngineeringBeamlineHistogramNuclear electronicsConventional PCIElectronic engineeringElectrical and Electronic EngineeringLine (text file)businessIEEE Transactions on Nuclear Science
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From the Reference SEU Monitor to the Technology Demonstration Module On-Board PROBA-II

2008

The reference SEU Monitor system designed and presented in 2005 (R. H. SOslashrensen, F.-X. Guerre, and A. Roseng ldquoDesign, testing and calibration of a reference SEU monitor system,rdquo in Proc. RADECS, 2005, pp. B3-1-B3-7) has now been used by many researchers at many radiation test sites and has provided valuable calibration data in support of numerous projects. As some of these findings and results give new insight into improved inter-facility calibrations and provide additional inputs into ongoing SEE research, a few of the more interesting cases are presented. Furthermore the dasiadetector elementpsila, the Atmel AT60142F SRAM, now in a hybrid configuration, will form the key dete…

Nuclear and High Energy PhysicsEngineeringbusiness.industryDetectorOn boardRadiation testingNuclear Energy and EngineeringSingle event upsetCalibrationKey (cryptography)Electronic engineeringSatelliteStatic random-access memoryElectrical and Electronic EngineeringbusinessComputer hardwareIEEE Transactions on Nuclear Science
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