Search results for " Resolution"

showing 10 items of 1159 documents

Scintillating fiber detectors for the HypHI project at GSI

2009

WOS: 000270326800009

PhysicsNuclear and High Energy PhysicsHydrogenProjectileDetectorPhase (waves)chemistry.chemical_elementTracking (particle physics)Charged particleHypernuclear spectroscopyNuclear physicsTracking detectorschemistryScintillating fiber detectorsDeposition (phase transition)InstrumentationImage resolution
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High-resolution study of Gamow-Teller transitions in the47Ti(3He,t)47V reaction

2013

In this work we have studied ${T}_{z}=+2\ensuremath{\rightarrow}+1$, Gamow-Teller (GT) transitions in the $^{48}\mathrm{Ti}(^{3}\mathrm{He},t)^{48}\mathrm{V}$ charge-exchange reaction at 140 MeV/nucleon and ${0}^{\ensuremath{\circ}}$ at the Research Center for Nuclear Physics, Osaka. From the high-resolution facility, consisting of a high-dispersion beamline and the Grand Raiden spectrometer, the spectrum had an energy resolution of 21 keV, among the best achieved. Individual GT transitions were observed and GT strength was derived for each state populated up to an excitation energy of 12 MeV. The total sum of the $B$(GT) strength observed in discrete states was 4.0, which is 33% of the sum…

PhysicsNuclear and High Energy PhysicsIsospinSHELL modelHigh resolutionAtomic physicsNuclear ExperimentNucleonEnergy (signal processing)ExcitationPhysical Review C
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Performance of the ATLAS silicon strip detector modules

1998

Abstract The performance of the silicon strip detector prototypes developed for use in ATLAS at the LHC is reported. Baseline detector assemblies (“modules”) of 12 cm length were read out with binary electronics at 40 MHz clock speed. For both irradiated and unirradiated modules, the tracking efficiency, noise occupancy, and position resolution were measured as a function of bias voltage, binary hit threshold, and detector rotation angle in a 1.56 T magnetic field. Measurements were also performed at a particle flux comparable to the one expected at the LHC.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderPhysics::Instrumentation and Detectorsbusiness.industryClock rateDetectorBiasingTracking (particle physics)Noise (electronics)Nuclear magnetic resonanceOpticsmedicine.anatomical_structureAtlas (anatomy)medicinebusinessInstrumentationImage resolutionNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Silicon detectors for forward tracking in ATLAS

1996

Abstract A 12 cm long silicon microstrip detector module with a fan geometry has been designed and constructed. The performance of the detector has been studied in a test beam at CERN. Results are presented on the hit efficiency and the position resolution as a function of position along the strips. With a hit efficiency of 99.5% and a spatial resolution of typically 35 μm the performance of these detectors exceeds that of other candidate technologies for the precision forward tracker of the ATLAS inner detector.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderSiliconPhysics::Instrumentation and Detectorsbusiness.industryDetectorchemistry.chemical_elementSTRIPSTracking (particle physics)law.inventionmedicine.anatomical_structureOpticschemistryAtlas (anatomy)Position (vector)lawmedicineHigh Energy Physics::ExperimentDetectors and Experimental TechniquesbusinessInstrumentationImage resolution
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High-resolution study of Gamow-Teller excitations in theCa42(He3,t)Sc42reaction and the observation of a “low-energy super-Gamow-Teller state”

2015

Y. Fujita et al.; 15 pags.; 6 figs.; 7 tabs.; PACS number(s): 21.10.Hw, 25.55.Kr, 27.40.+z, 25.40.Ep

PhysicsNuclear and High Energy PhysicsLow energyFujita scaleHigh resolutionState (functional analysis)Atomic physicsPhysical Review C
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Time-of-flight photoelectron emission microscopy TOF-PEEM: first results

1998

The time structure of the synchrotron radiation at BESSY (Berlin) is used to operate a photoemission electron microscope in a time-of-flight (TOF) mode. The electrons which are emitted from the sample surface with different energies are dispersed in a drift tube subsequent to the imaging optics. The screen of the microscope was replaced by a fast scintillator (tau = 1.4 ns) and the light is detected by an ultra fast gated intensified CCD camera (800 ps gate 1 MHz repetition rate). The resolving power in the energy domain is demonstrated and possible implications on the spatial resolution (chromatic correction) are discussed. Additionally, an improved contrast at very low emission energies i…

PhysicsNuclear and High Energy PhysicsMicroscopebusiness.industryPhysics::Instrumentation and DetectorsSynchrotron radiationElectronScintillatorlaw.inventionTime of flightOpticslawChromatic scaleElectron microscopebusinessInstrumentationImage resolution
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UTSW Small Animal Positron Emission Imager

2006

A Small Animal Imager (SAI) for PET has been designed, built, tested in phantoms, and applied to investigations in mice and rats. The device uses principles based on gamma-ray induced scintillation in crossed fiber optic detectors connected to Position Sensitive Photomultiplier Tubes (PSPMT). Each detector consists of an epoxied stack of 28 layers of 135 round 1 mm BCF-10 scintillating plastic fibers. The overlap region forms a 13.5times13.5times2.8 cm3 detector volume. Scintillating light from the fibers is detected by two (X and Y directions) Hamamatsu R-2486 PSPMTs with 16 anode wires in each of two orthogonal directions. A centroid-finding algorithm gives the position of a light cluster…

PhysicsNuclear and High Energy PhysicsPhotomultiplierScintillationOptical fiberPhotonbusiness.industryDetectorIterative reconstructionPhotocathodelaw.inventionOpticsNuclear Energy and EngineeringlawElectrical and Electronic EngineeringbusinessImage resolutionIEEE Transactions on Nuclear Science
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A scintillator based time-of-flight hodoscope with a new type of emitter follower divider

2004

A high precision, time-of-flight hodoscope has been constructed to analyse the secondary pion beam at GSI, Darmstadt. The hodoscope comprises three scintillator planes with the individual scintillator rods read out by photomultipliers in both ends. A new active base of the emitter follower type has been developed for stabilization of voltages at the last dynodes of the photomultiplier. The time resolution of this system was found to be sigma less than or equal to 150 ps for counting rates up to 2 MHz.

PhysicsNuclear and High Energy PhysicsPhotomultiplierbusiness.industryPhysics::Instrumentation and Detectors25.80.Ls; 29.70.Eg; 25.75.Dw; 29.27.-tCommon collectorTime resolutionScintillatorRodTime of flightOpticsTime-of-flight measurementsHodoscopePhysics::Accelerator Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]businessNuclear ExperimentInstrumentationVoltage
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AX-PET: A novel PET concept with G-APD readout

2012

Abstract The AX-PET collaboration has developed a novel concept for high resolution PET imaging to overcome some of the performance limitations of classical PET cameras, in particular the compromise between spatial resolution and sensitivity introduced by the parallax error. The detector consists of an arrangement of long LYSO scintillating crystals axially oriented around the field of view together with arrays of wave length shifter strips orthogonal to the crystals. This matrix allows a precise 3D measurement of the photon interaction point. This is valid both for photoelectric absorption at 511 keV and for Compton scattering down to deposited energies of about 100 keV. Crystals and WLS s…

PhysicsNuclear and High Energy PhysicsPhotonPhysics::Instrumentation and Detectorsbusiness.industryPhysics::Medical PhysicsDetectorCompton scatteringField of viewLyso-030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineOpticsSilicon photomultiplier030220 oncology & carcinogenesisTomographybusinessInstrumentationImage resolutionNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Performance of production modules of the Belle II pixel detector in a high-energy particle beam

2021

The Belle II experiment at the Super B factory SuperKEKB, an asymmetric $e^+e^-$ collider located in Tsukuba, Japan, is tailored to perform precision B physics measurements. The centre of mass energy of the collisions is equal to the rest mass of the $\Upsilon(4S)$ resonance of $m_{\Upsilon(4S)} = 10.58\,\rm GeV$. A high vertex resolution is essential for measuring the decay vertices of B mesons. Typical momenta of the decay products are ranging from a few tens of MeV to a few GeV and multiple scattering has a significant impact on the vertex resolution. The VerteX Detector (VXD) for Belle II is therefore designed to have as little material as possible inside the acceptance region. Especial…

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and Detectors010308 nuclear & particles physicsDetectorFOS: Physical sciencesDESYInstrumentation and Detectors (physics.ins-det)01 natural sciences7. Clean energyCharge sharinglaw.inventionB-factoryHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciencesInvariant massHigh Energy Physics::Experiment010306 general physicsColliderInstrumentationImage resolutionBeam (structure)
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