Search results for "TRACK"

showing 10 items of 975 documents

LiF crystals irradiated with 150MeV Kr ions: Peculiarities of color center creation and thermal annealing

2013

Abstract Color centers in LiF crystals are studied under irradiation at room temperature with 150 MeV Kr ions in the fluence (Φ) range of 1010–1014 ions/cm2 with a beam current density of 10, 50, and 100 nA/cm2, corresponding to flux of 4.46 × 109, 2.23 × 1010 and 4.46 × 1010 ions/(cm2 × s), respectively. At Φ ⩾ 3 × 1012 ions/cm2 besides F and Fn centers also charged F 3 + centers are created. Thermal annealing of irradiated LiF crystals with Φ ⩾ 1013 ions/cm2 at 400 K leads to a decrease of F centers (due to annihilation with H centers) and an enhancement of complex Fn color centers (neutral and charged) due to interaction with thermally activated anion vacancies. Annealing LiF crystals at…

Nuclear and High Energy PhysicsColloidRange (particle radiation)Absorption spectroscopyAnnealing (metallurgy)ChemistryIon trackAnalytical chemistryIrradiationAtomic physicsInstrumentationFluenceIonNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The DAMPE silicon–tungsten tracker

2016

Abstract The DArk Matter Particle Explorer (DAMPE) is a spaceborne astroparticle physics experiment, launched on 17 December 2015. DAMPE will identify possible dark matter signatures by detecting electrons and photons in the 5 GeV–10 TeV energy range. It will also measure the flux of nuclei up to 100 TeV, for the study of the high energy cosmic ray origin and propagation mechanisms. DAMPE is composed of four sub-detectors: a plastic strip scintillator, a silicon–tungsten tracker–converter (STK), a BGO imaging calorimeter and a neutron detector. The STK is composed of six tracking planes of 2 orthogonal layers of single-sided micro-strip detectors, for a total detector surface of ca. 7 m2. T…

Nuclear and High Energy PhysicsCosmic rays; Dark matter; Silicon tracker; Spaceborne experiment; Nuclear and High Energy Physics; InstrumentationPhysics::Instrumentation and DetectorsCosmic rayParticle detectorsTracking (particle physics)01 natural sciencesParticle detectorOpticscosmic rays0103 physical sciencesDark matterNeutron detection010303 astronomy & astrophysicsInstrumentationAstroparticle physicsPhysicsLarge Hadron ColliderCalorimeter (particle physics)010308 nuclear & particles physicsbusiness.industryDetectorSettore FIS/01 - Fisica SperimentaleParticle detectors cosmic raysSpaceborne experimentSilicon trackerHigh Energy Physics::Experimentbusiness
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Color centers and nanodefects in LiF crystals irradiated with 150MeV Kr ions

2012

Abstract The modifications of structure, optical and nano-mechanical properties of LiF crystals after irradiation with 150-MeV Kr +14 ions at a fluence of 6 × 10 12  ions cm −2 have been studied using optical absorption spectroscopy, scanning electron and atomic force microscopy, and nanoindentation. Optical spectroscopy shows the saturation of F centers and a comparatively high number of F n centers. AFM and SEM imaging reveals a nanostructured region with columnar nanocrystallites (size 30–90 nm). Nanostructuring occurs in depths up to 10 μm, where the ion energy loss surpasses a critical threshold of about 10 keV/nm. At a lower energy loss a zone enriched with dislocations is observed. S…

Nuclear and High Energy PhysicsCrystallographyMaterials scienceAbsorption spectroscopyScanning electron microscopeAnnealing (metallurgy)Ion trackAnalytical chemistryIrradiationNanoindentationSpectroscopyInstrumentationIonNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Investigation of heavy ion tracks in LiF crystals by dislocation mobility method

2008

Abstract The track damage created in LiF by swift heavy ions was studied using methods of dislocation mobility and track etching. The crystals were irradiated with Bi and Pb ions of a specific energy of 11 MeV/u at fluences between 10 7 and 10 10  cm −2 . The measurements on cross-sections cleaved parallel to the irradiated surface showed continuity of the track etching for the depth up to 70% of the ion range. In deeper layers, numerous etch pits had a flat-bottomed shape indicating the discontinuities of the track structure. At this stage, a decrease of the ion-induced effect in dislocation mobility was observed. The observed reduction of the efficiency of ion tracks as obstacles for disl…

Nuclear and High Energy PhysicsCrystallographyRange (particle radiation)Materials scienceEtching (microfabrication)Ion trackTrack (disk drive)Specific energyIrradiationDislocationInstrumentationMolecular physicsIonNuclear 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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Interaction position resolution simulations and in-beam measurements of the AGATA HPGe detectors

2011

WOS: 000290082600015

Nuclear and High Energy PhysicsFusion-evaporation ReactionsPhysics::Instrumentation and Detectorsg-ray trackingAstrophysics::High Energy Astrophysical PhenomenaMonte Carlo methodEvaporationRay tracking[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesParticle detectorNuclear physicsAGATA Fusion-evaporation reactions HPGe detectors Monte Carlo Simulation Ray tracking; Computer simulation Evaporation Monte Carlo methods Phase transitions; DetectorsHPGe Detectors0103 physical sciencesNuclear Experiment010306 general physicsInstrumentationGamma-ray TrackingPhysics010308 nuclear & particles physics4. EducationResolution (electron density)DetectorMonte Carlo SimulationMonte Carlo methodsDetectorsComputer simulationSemiconductor detectorPhase transitionsMonte Carlo SimulationsMeasuring instrumentHigh Energy Physics::ExperimentAGATAAGATABeam (structure)
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Pairing-quadrupole interplay in the neutron-deficient tin nuclei: First lifetime measurements of low-lying states in 106,108Sn

2020

The lifetimes of the low-lying excited states 2(+) and 4(+) have been directly measured in the neutron-deficient Sn-106,Sn-108 isotopes. the nuclei were populated via a deep-inelastic reaction and the lifetime measurement was performed employing a differential plunger device. the emitted gamma rays were detected by the AGATA array, while the reaction products were uniquely identified by the VAMOS++ magnetic spectrometer. Large-Scale Shell-Model calculations with realistic forces indicate that, independently of the pairing content of the interaction, the quadrupole force is dominant in the B(E2; 2(1)(+) -> 0(g.s)(+)) values and it describes well the experimental pattern for Sn104-114 ; the B…

Nuclear and High Energy PhysicsLight Snchemistry.chemical_elementFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex01 natural sciencesSubatomär fysikLifetime; Light Sn; Multi-nucleon transfer; Nuclear structure; Tracking array0103 physical sciencesSubatomic PhysicsNeutronTracking arrayNuclear Physics - ExperimentNuclear structureNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsSpectrometerIsotopeLifetime ; Nuclear structure ; Multi-nucleon transfer ; Light Sn ; Tracking array010308 nuclear & particles physicsPhysicsMulti-nucleon transferlcsh:QC1-999chemistryPairingExcited stateQuadrupoleAGATAAtomic physicsTinlcsh:PhysicsLifetime
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Ion track template technique for fabrication of ZnSe2O5 nanocrystals

2020

The work was performed under the grant of the Ministry of Education and Science of the Republic of Kazakhstan AP05134367 and Latvian grant lzp

Nuclear and High Energy PhysicsLuminescencePhotoluminescenceMaterials sciencePhysics::Optics02 engineering and technology01 natural sciencesMolecular physicsFluenceIonIon trackCondensed Matter::Materials Science0103 physical sciences:NATURAL SCIENCES:Physics [Research Subject Categories]Instrumentation010302 applied physicsIon track021001 nanoscience & nanotechnologyZnSe2O5Track templateExcited stateAb initioDirect and indirect band gapsOrthorhombic crystal system0210 nano-technologyLuminescenceNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Thin film growth into the ion track structures in polyimide by atomic layer deposition

2017

Abstract High-aspect ratio porous structures with controllable pore diameters and without a stiff substrate can be fabricated using the ion track technique. Atomic layer deposition is an ideal technique for depositing thin films and functional surfaces on complicated 3D structures due to the high conformality of the films. In this work, we studied Al2O3 and TiO2 films grown by ALD on pristine polyimide (Kapton HN) membranes as well as polyimide membranes etched in sodium hypochlorite (NaOCl) and boric acid (BO3) solution by means of RBS, PIXE, SEM-EDX and helium ion microcopy (HIM). The focus was on the first ALD growth cycles. The areal density of Al2O3 film in the 400 cycle sample was det…

Nuclear and High Energy PhysicsMaterials scienceAnalytical chemistry02 engineering and technologySubstrate (electronics)ion trackpolyimide01 natural sciencesAtomic layer depositionEtching (microfabrication)0103 physical sciencesetchingComposite materialThin filmInstrumentation010302 applied physicsIon beam analysista114broad ion beam cuttingIon trackion beam analysis021001 nanoscience & nanotechnologyKaptonatomic layer depositionhelium ion microscopy0210 nano-technologyPolyimideNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Influence of complex impurity centres on radiation damage in wide-gap metal oxides

2016

Different mechanisms of radiation damage of wide-gap metal oxides as well as a dual influence of impurity ions on the efficiency of radiation damage have been considered on the example of binary ionic MgO and complex ionic–covalent $Lu_{3}Al_{5}O_{12}$ single crystals. Particular emphasis has been placed on irradiation with $\sim$2 GeV heavy ions ($^{197}Au, ^{209}Bi, ^{238}U$, fluence of 10$^{12}$ ions/cm$^{2}$) providing extremely high density of electronic excitations within ion tracks. Besides knock-out mechanism for Frenkel pair formation, the additional mechanism through the collapse of mobile discrete breathers at certain lattice places (e.g., complex impurity centres) leads to the c…

Nuclear and High Energy PhysicsMaterials scienceCondensed matter physicsIon trackIonic bonding02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesIonImpurity0103 physical sciencesFrenkel defectddc:530IrradiationAtomic physics010306 general physics0210 nano-technologyInstrumentationRadiation resistanceMagnetic impurity
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