Search results for "Signal processing"

showing 10 items of 2451 documents

AGATA-Advanced GAmma Tracking Array

2012

WOS: 000300864200005

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPulse-shape and gamma-ray tracking algorithmsFOS: Physical sciencesSemiconductor detector performance and simulationsIntegrated circuit[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Tracking (particle physics)gamma-Ray tracking01 natural sciencesPulse-shape and γ-ray tracking algorithmslaw.inventionData acquisitionlaw0103 physical sciencesddc:530[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsγ-Ray spectroscopyNuclear ExperimentInstrumentationDigital signal processingEvent reconstructiongamma-Ray spectroscopyPhysicssezeleSpectrometerSpectrometers010308 nuclear & particles physicsbusiness.industryDetectorAGATA Digital signals HPGe detectors Pulse-shape Ray trackingHPGe detectorsAlgorithms Crystals Germanium Semiconductor detectors Signal processing Spectrometry Tracking (position)γ-Ray trackingInstrumentation and Detectors (physics.ins-det)Digital signal processingAGATAFísica nuclearbusinessAGATAComputer hardware
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High-gradient testing of an $S$-band, normal-conducting low phase velocity accelerating structure

2020

A novel high-gradient accelerating structure with low phase velocity, $v/c=0.38$, has been designed, manufactured and high-power tested. The structure was designed and built using the methodology and technology developed for CLIC $100\text{ }\text{ }\mathrm{MV}/\mathrm{m}$ high-gradient accelerating structures, which have speed of light phase velocity, but adapts them to a structure for nonrelativistic particles. The parameters of the structure were optimized for the compact proton therapy linac project, and specifically to 76 MeV energy protons, but the type of structure opens more generally the possibility of compact low phase velocity linacs. The structure operates in S-band, is backward…

Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Field (physics)[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]cavityType (model theory)01 natural sciencesp: accelerationLinear particle accelerator0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsReview ArticlesPhysics010308 nuclear & particles physicsvelocity: lowPulse durationSurfaces and Interfaceslinear acceleratorgradient: highAccelerators and Storage Ringsvelocity: phasePulse (physics)particle: nonrelativisticDistribution (mathematics)lcsh:QC770-798Atomic physicsPhase velocityEnergy (signal processing)performance
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Measurement of integrated luminosity and center-of-mass energy of data taken by BESIII at

2017

Chinese physics / C 41(11), 113001 (2017). doi:10.1088/1674-1137/41/11/113001

Nuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical Phenomena01 natural sciences530law.inventionNuclear physicslaw0103 physical sciencesddc:530Nuclear Experiment010306 general physicsColliderInstrumentationAstrophysics::Galaxy AstrophysicsBhabha scatteringPhysicsLuminosity (scattering theory)010308 nuclear & particles physicsDetectorAstronomy and AstrophysicsCollisionData setHigh Energy Physics::ExperimentCenter of massAstrophysics::Earth and Planetary AstrophysicsEnergy (signal processing)
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Probing the Merits of Different Event Parameters for the Identification of Light Charged Particles in CHIMERA CsI(Tl Detectors With Digital Pulse Sha…

2013

We investigated the merits of different event parameters in the identification of Light Charged Particles (LCPs) with CsI(Tl) scintillators read out by photodiodes at high incident energy (400 MeV/u). This investigation is made possible by digital signal processing the output signals. As in the conventional analogue case, the digitized signals allow the discrimination of light charged particles by computing the fast and slow components. In addition other identification parameters as the rise time of the output pulses of the CsI(Tl) come out nearly for free. Aim of this paper is the investigation of novel identification plots and the probe of their merits, in particular at relativistic energ…

Nuclear and High Energy PhysicsPhysics::Instrumentation and Detectorsintermediate energy nuclear physicpulse shape analysiScintillatorParticle identificationlaw.inventionOpticslawElectrical and Electronic EngineeringDigital signal processingPhysicsonline digital signal processingSignal processingsezeleCsI(Tl) scintillatorsbusiness.industrypulse shape analysisDetectorCsI(Tl) scintillatorCsI(Tl) scintillators; intermediate energy nuclear physics; online digital signal processing; particle identification; pulse shape analysisCsI(Tl) scintillators; intermediate energy nuclear physics; online digital signal processing; particle identification; pulse shape analysis; Electrical and Electronic Engineering; Nuclear Energy and Engineering; Nuclear and High Energy PhysicsCharged particlePhotodiodeintermediate energy nuclear physicsNuclear Energy and EngineeringRise timeparticle identificationbusinessnuclear physics; heavy-ions; digital signal processing; scintillation detectors
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Sensitivity enhancement in pulse EPR distance measurements

2004

Established pulse EPR approaches to the measurement of small dipole-dipole couplings between electron spins rely on constant-time echo experiments to separate relaxational contributions from dipolar time evolution. This requires a compromise between sensitivity and resolution to be made prior to the measurement, so that optimum data are only obtained if the magnitude of the dipole-dipole coupling is known beforehand to a good approximation. Moreover, the whole dipolar evolution function is measured with relatively low sensitivity. These problems are overcome by a variable-time experiment that achieves suppression of the relaxation contribution by reference deconvolution. Theoretical and exp…

Nuclear and High Energy PhysicsProtein ConformationBiophysicsAnalytical chemistryBiochemistrySensitivity and Specificitylaw.inventionlawspin labelingSensitivity (control systems)protein structurepair correlation functionElectron paramagnetic resonanceCouplingSpinsChemistryPulsed EPRRelaxation (NMR)Time evolutionElectron Spin Resonance SpectroscopyPhotosystem II Protein ComplexReproducibility of ResultsSignal Processing Computer-AssistedELDORCondensed Matter PhysicsComputational physicsDeconvolutionEPRAlgorithms
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Simultaneous wide-range stopping power determination for several ions

2002

A new procedure to extract simultaneously continuous stopping power curves for several ions and several absorbers over a wide energy range and with statistical errors reduced to negligible level is presented. The method combines our novel time-of-flight based method with the capability of our K130 cyclotron and ECR ion-source to produce the so-called ion cocktails. The potential of the method is demonstrated with a 6.0 MeV/u cocktail consisting of 16O4+, 28Si7+ and 40Ar10+ ions. The stopping power in polycarbonate in the energy range of 0.35–5 MeV/u has been determined with absolute uncertainty of less than 2.3% and with relative below 0.2%. The results are compared with literature data and…

Nuclear and High Energy PhysicsRange (particle radiation)ChemistrylawCyclotronStopping power (particle radiation)Atomic physicsInstrumentationEnergy (signal processing)law.inventionIonNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Energy loss of 40Ar in Au: Comparison of TOF-E and TOF–TOF method

2005

Abstract Energy loss of 40Ar ions in Au has been measured using two methods: TOF-E and TOF–TOF. The two methods are compared and discussed. The final results cover energy range 2–445 MeV (0.05–11 MeV/u) and give satisfactory agreement with SRIM 2003 predictions. Statistical error of the data is at the level of 1–2%.

Nuclear and High Energy PhysicsRange (particle radiation)Energy lossChemistryAnalytical chemistryStopping power (particle radiation)Statistical errorAtomic physicsInstrumentationEnergy (signal processing)IonNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Silicon Detector Telescope for proton detection in electron scattering reactions at MAMI

2012

Abstract A new Silicon Detector Telescope has been constructed and installed within the experimental facility of the A1 collaboration at Mainz Microtron, with the goal to detect low-energy protons. It consists of seven silicon layers for energy and angle measurement and a plastic scintillator for triggering purposes. The detector subtends a solid angle up to 88 msr, depending on the distance from the target and covers the proton kinetic energy range of 25–41  MeV with the mean energy resolution σ E = 0.47 MeV , operating at 500 kHz. Digital signal processing methods applied for energy reconstruction have been important for keeping the acceptable energy resolution at high counting rates. The…

Nuclear and High Energy PhysicsSiliconPhysics::Instrumentation and Detectorschemistry.chemical_elementScintillator01 natural scienceslaw.inventionNuclear physicsTelescopeOpticslaw0103 physical sciencessilicon detector; digital signal processing; electron scatteringNuclear Experiment010306 general physicsInstrumentationMicrotronPhysicsRange (particle radiation)Spectrometer010308 nuclear & particles physicsbusiness.industryDetectorSolid anglechemistryPhysics::Accelerator PhysicsbusinessNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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Measurements of the top-quark mass using charged particle tracking

2010

21 páginas, 13 figuras, 6 tablas.-- PACS numbers: 12.15.-y, 13.85.-t, 14.60.-z, 14.65.Fy.-- CDF Collaboration: et al.

Nuclear and High Energy PhysicsTop quarkParticle physicsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesElementary particleElectronddc:500.201 natural sciences7. Clean energy114 Physical sciencesTOP QUARKHigh Energy Physics - ExperimentPHYSICSNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences010306 general physicsTEVATRONNuclear ExperimentPhysicsMuon010308 nuclear & particles physicshep-exPhysicsHigh Energy Physics::PhenomenologyFermionCharged particleCDFHigh Energy Physics::ExperimentEnergy (signal processing)Lepton
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