Search results for "microchannel"

showing 10 items of 35 documents

Performance of the cost-effective Planacon ® MCP-PMTs in strong magnetic fields

2020

Abstract We present the behavior of the cost-effective Planacon MCP-PMTs with 25 μ m pore diameter in the presence of axial magnetic fields up to 0.5 T. Having a batch of 62 devices of the same type, two MCP-PMTs were selected and their gain variation measured in different magnetic fields. These two otherwise identical devices satisfied the selection criteria by requiring the lowest (1.15 kV) and one of the highest (1.4 kV) bias voltage values to achieve a given gain. Both MCP-PMTs have a nearly identical tolerance of the strong magnetic field despite the significant difference in the bias voltage. This clarifies the mechanism of the B-field influence on the MCP-PMT gain, emphasizing the im…

PhysicsNuclear and High Energy PhysicsPore diameter010308 nuclear & particles physicsSignificant differenceBiasing01 natural sciences030218 nuclear medicine & medical imagingComputational physicsLarge poreMagnetic field03 medical and health sciences0302 clinical medicine0103 physical sciencesMicrochannel plate detectorInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The PANDA DIRC detectors

2020

Abstract The PANDA experiment at the future Facility for Antiproton and Ion Research (FAIR) will address fundamental questions of hadron physics with unprecedented precision. To reach this goal excellent Particle Identification (PID) is essential over a large range of particle momenta and solid angles. Most of the phase space will be covered by two innovative DIRC (Detection of Internally Reflected Cherenkov light) detectors. The Endcap Disc DIRC and Barrel DIRC will cover the polar angle range from 5 to 22°and 22 to 140°, respectively. Both detectors rely on high precision optical components, lifetime-enhanced Microchannel Plate PMTs (MCP-PMTs), and fast readout electronics.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Physics::Instrumentation and Detectors010308 nuclear & particles physicsCherenkov detectorbusiness.industryDetectorSolid angle01 natural sciencesParticle identificationlaw.inventionOpticslawDetection of internally reflected Cherenkov light0103 physical sciencesFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentMicrochannel plate detector010306 general physicsbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Time response of TOF spectrometer to light and heavy particles

2002

Comparing time of flight (TOF) values for α particles and fission fragments measured at different distances between the start- and stop detector we have obtained 60 ps as the upper limit for the TOF error resulting from the assumption of equal and linear time calibrations for both types of particles. While the 60 ps limit relates only to the specific spectrometer, the problem and the suggested verification technique are of general interest.

PhysicsNuclear and High Energy PhysicsSpectrometerPhysics::Instrumentation and DetectorsFissionDetectorAnalytical chemistryAlpha particleTime of flightTime responseMicrochannel plate detectorLimit (mathematics)Nuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The large-area micro-channel plate entrance detector of the heavy-ion magnetic spectrometer PRISMA

2005

This paper describes the entrance detector of the magnetic spectrometer PRISMA recently installed at Legnaro. The detector is based on rectangular (80 x 100 mm(2)) Micro-Channel Plates (MCP). It provides a fast time signal and its position-sensitive anode allows to extract the X and Y information. It exploits an electrostatic field for the acceleration of secondary electrons from a thin Carbon foil (similar or equal to 20 mu g/cm(2)) onto the MCP assembly. The electrons are guided by a parallel magnetic field. Good performances were obtained in the laboratory tests. The detector is presently installed at the entrance of PRISMA and gives resolutions <= 400 ps in time, and 1 mm in both X and …

PhysicsNuclear and High Energy PhysicsSpectrometerbusiness.industryDetectordetectors for heavy ions ; micro-channel plates ; magnetic spectrometers ; low-energy heavy-ion reactionsParticle detectorSecondary electronsCharged particleMagnetic fieldNuclear physicsOpticsElectric fieldMicrochannel plate detectorbusinessInstrumentation
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Tests of Lobster Eye Optics for Small Space X-ray Telescope

2011

Abstract The Lobster eye design for a grazing incidence X-ray optics provides wide field of view of the order of many degrees, for this reason it can be a convenient approach for the construction of space all-sky X-ray monitors. We present preliminary results of tests of prototype lobster eye X-ray optics in quasi parallel beam full imaging mode conducted using the 35 m long X-ray beam-line of INAF-OAPA in Palermo (Italy). X-ray images at the focal plane have been taken with a microchannel plate (MCP) detector at several energy values from 0.3 to 8 keV. The gain, the field of view and the angular resolution have been measured and compared with theoretical values.

PhysicsNuclear and High Energy Physicsbusiness.industryAstrophysics::High Energy Astrophysical PhenomenaDetectorX-ray opticsField of viewX-ray telescopeCardinal pointOpticsLobster eye X-ray optics X-ray telescope All-sky monitor X-ray imaging X-raySettore FIS/05 - Astronomia E AstrofisicaAngular resolutionMicrochannel plate detectorbusinessInstrumentationEnergy (signal processing)
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A Disc-DIRC Cherenkov detector with high resolution micro channel plate photomultiplier tubes

2014

The upcoming PANDA Experiment at FAIR in Germany will be equipped with a novel Cherenkov detector type for high-energy particle identification. This very compact Disc-DIRC detector uses a large disc-shaped fused silica plate of 2 cm thickness as its Cherenkov radiator. The internally reflected Cherenkov light is transported to the rim of the disc where it is focused by quartz light guides onto microchannel plate photomultiplier tubes (MCP-PMTs) with high spatial resolution (pitch 0.5 mm) and high time resolution (σ ≈ 100 ps). The device has an active area of about 3 m2 and will be able to identify pions and kaons with a separation power of more than 3σ in the momentum range up to 4 GeV/c. I…

PhysicsPhotomultiplierPhotonPhysics::Instrumentation and DetectorsCherenkov detectorbusiness.industryDetectorRadiationParticle identificationlaw.inventionOpticslawMicrochannel plate detectorbusinessCherenkov radiation2014 IEEE Nuclear Science Symposium and Medical Imaging Conference (NSS/MIC)
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Direct detection of the 229Th nuclear clock transition

2017

Today’s most precise time and frequency measurements are performed with optical atomic clocks. However, it has been proposed that they could potentially be outperformed by a nuclear clock, which employs a nuclear transition instead of an atomic shell transition. There is only one known nuclear state that could serve as a nuclear clock using currently available technology, namely, the isomeric first excited state of 229Th (denoted 229mTh). Here we report the direct detection of this nuclear state, which is further confirmation of the existence of the isomer and lays the foundation for precise studies of its decay parameters. On the basis of this direct detection, the isomeric energy is const…

PhysicsQuantum opticsMultidisciplinaryPhysics - Instrumentation and Detectors010308 nuclear & particles physicsNuclear TheoryElectronvoltFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)Frequency standardLaser01 natural sciencesAtomic clockComputational physicslaw.inventionlawExcited state0103 physical sciencesMicrochannel plate detectorNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentExcitation
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Energy loss measurement of protons in liquid water

2011

The proton stopping power of liquid water was, for the first time, measured in the energy range 4.7-15.2 MeV. The proton energies were determined by the time-of-flight transmission technique with the microchannel plate detectors, which were especially developed for timing applications. The results are compared to the literature values (from ICRU Report 49 (1993) and Janni's tabulation (1982 At. Data Nucl. Data Tables 27 147-339)) which are based on Bethe's formula and an agreement is found within the experimental uncertainty of 4.6%. Thus, earlier reported discrepancy between the experimental and literature stopping power values at lower energies was not observed at the energies considered …

PhysicsRange (particle radiation)Energy lossTime FactorsRadiological and Ultrasound TechnologyProtonLiquid waterDetectorWaterNuclear physicsExperimental uncertainty analysisSolventsStopping power (particle radiation)Computer SimulationLinear Energy TransferRadiology Nuclear Medicine and imagingMicrochannel plate detectorProtonsAtomic physicsRadiometryPhysics in Medicine and Biology
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Secondary electron flight times and tracks in the carbon foil time pick-up detector

2014

Carbon foil time pick-up detectors used in the time-of-flight measurements of MeV energy ions have been studied in connection to time-of-flight-energy spectrometer used for heavy ion elastic recoil detection analysis. In experimental coincident TOF-E data characteristic halos are observed around light element isobars, and the origin of these halos were studied. The experimental data indicated that these halos originate from single electron events occurring before the electron multiplication in the microchannel plate. By means of electron trajectory simulations, this halo effect is explained to originate from single electron, emitted from the carbon foil, hitting the non-active area of the m…

PhysicsToF-ERDANuclear and High Energy Physicstiming gateta114business.industryPhysics::Instrumentation and DetectorsDetectorElectrontime-of-flightSecondary electronsElastic recoil detectionTime of flightOpticsCoincidentMicrochannel plate detectorspectrometerAtomic physicsbusinesscarbon foil time pick-up detectorInstrumentationFOIL methodNuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
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Light weight, thin plastic foil, X-ray telescopes

2002

We present results from a program to develop an X-ray telescope made from thin plastic shells. Our initial results have been obtained from multi-shell cylindrical lenses that are used in a point-to-point configuration to image the small focal spot of a an X-ray tube on a microchannel plate detector. We describe the steps that led up to the present design and present data from the tests that have been used to identify the properties of the plastic material that make it a suitable X-ray reflector. We discuss two applications of our technology to X-ray missions that are designed to address some of the scientific priorities set forth in NASA's long term plans for high energy astrophysics. One m…

PhysicsX-ray astronomyHigh-energy astronomybusiness.industryAstrophysics::High Energy Astrophysical PhenomenaAstrophysics::Instrumentation and Methods for AstrophysicsX-ray opticsReflector (antenna)X-ray telescopeCondensed Matter Physicslaw.inventionTelescopeOpticslawMicrochannel plate detectorTube (container)Electrical and Electronic Engineeringbusiness
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