Search results for "Instrumentation"

showing 10 items of 4914 documents

Cyclotron instability in the afterglow mode of minimum-B ECRIS.

2016

It was shown recently that cyclotron instability in non-equilibrium plasma of a minimum-B electron cyclotron resonance ion source (ECRIS) causes perturbation of the extracted ion current and generation of strong bursts of bremsstrahlung emission, which limit the performance of the ion source. The present work is devoted to the dynamic regimes of plasma instability in ECRIS operated in pulsed mode. Instability develops in decaying plasma shortly after heating microwaves are switched off and manifests itself in the form of powerful pulses of electromagnetic emission associated with precipitation of high energy electrons. Time-resolved measurements of microwave emission bursts are presented. I…

010302 applied physicsPhysicsta114ta213Astrophysics::High Energy Astrophysical Phenomenaplasma instabilityCyclotronBremsstrahlungPlasma01 natural sciencesInstabilityIon sourceElectron cyclotron resonance010305 fluids & plasmaslaw.inventionTwo-stream instabilityPhysics::Plasma Physicslaw0103 physical scienceselectron cyclotron resonance ion sourcesAtomic physicsInstrumentationIon cyclotron resonanceThe Review of scientific instruments
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Luminescence of polymorphous SiO2

2016

Abstract The luminescence of self-trapped exciton (STE) was found and systematically studied in tetrahedron structured silica crystals (α-quartz, coesite, cristobalite) and glass. In octahedron structured stishovite only host material defect luminescence was observed. It strongly resembles luminescence of oxygen deficient silica glass and γ or neutron irradiated α-quartz. The energetic yield of STE luminescence for α-quartz and coesite is about 20% of absorbed energy and about 5(7)% for cristobalite. Two types of STE were found in α-quartz. Two overlapping bands of STEs are located at 2.5–2.7 eV. The model of STE is proposed as Si–O bond rupture, relaxation of created non-bridging oxygen (N…

010302 applied physicsRadiationMaterials scienceMineralogy02 engineering and technologyElectronic structureengineering.material021001 nanoscience & nanotechnology01 natural sciencesCristobalitesymbols.namesakeCrystallographyOctahedron0103 physical sciencesCoesitesymbolsengineering0210 nano-technologyRaman spectroscopyLuminescenceInstrumentationStishoviteNatural bond orbitalRadiation Measurements
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Sub-nanosecond excitonic luminescence in ZnO:In nanocrystals

2019

The financial support of research European Union ERA.NET RUS_ST20170-51 . This work was partly supported by Russian Foundation for Basic Research, Russia , project No. 18-52-76002 . The sample preparation was carried out as part of SFERA II project -Transnational Access activities ( European Union 7th Framework Programme Grant Agreement N3126430 ).

010302 applied physicsRadiationMaterials scienceMorphology (linguistics)DopingKineticsAnalytical chemistrychemistry.chemical_elementTime-resolved luminescenceNanosecondVapour deposition01 natural sciences030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineNanocrystalchemistry0103 physical sciences:NATURAL SCIENCES:Physics [Research Subject Categories]In [ZnO]Indium dopingLuminescenceInstrumentationScintillationIndium
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Lead evaporation instabilities and failure mechanisms of the micro oven at the GTS-LHC ECR ion source at CERN

2020

The GTS-LHC ECR ion source (named after the Grenoble Test Source and the Large Hadron Collider) at CERN provides heavy ion beams for the chain of accelerators from Linac3 up to the LHC for high energy collision experiments and to the Super Proton Synchrotron for fixed target experiments. During the standard operation, the oven technique is used to evaporate lead into the source plasma to produce multiple charged lead ion beams. Intensity and stability are key parameters for the beam, and the operational experience is that some of the source instabilities can be linked to the oven performance. Over long operation periods of several weeks, the evaporation is not stable which makes the tuning …

010302 applied physicsRange (particle radiation)Large Hadron ColliderMaterials scienceionitNuclear engineeringEvaporationPlasmahiukkaskiihdyttimetplasmafysiikka01 natural sciencesSuper Proton SynchrotronIon source010305 fluids & plasmasIonComputer Science::OtherPhysics::Popular Physics0103 physical scienceslyijyInstrumentationBeam (structure)
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Microfabricated high temperature sensing platform dedicated to scanning thermal microscopy (SThM)

2018

Abstract The monitoring of heat flux is becoming more and more critical for many materials and structures approaching nanometric dimensions. Scanning Thermal Microscopy (SThM) is one of the tools available for thermal measurement at the nanoscale and requires calibration. Here we report on a micro-hotplate device made of a platinum heater suspended on thin silicon nitride (SiN) membranes integrating specific features for SThM calibration. These heated reference samples can include a localized resistive temperature sensors (RTD) or standalone platinum membranes (typically 10 × 10 μm2) on which the temperature can be measured precisely. This functional area is dedicated to (1) estimate the th…

010302 applied physicsResistive touchscreenMaterials scienceFabricationbusiness.industryThermal resistanceMetals and Alloys02 engineering and technologyScanning thermal microscopy021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesTemperature measurementSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsOperating temperatureThermocouple0103 physical sciencesMicroscopyOptoelectronicsElectrical and Electronic Engineering0210 nano-technologybusinessInstrumentation
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Development of hard x-ray photoelectron SPLEED-based spectrometer applicable for probing of buried magnetic layer valence states

2016

Abstract A novel design of high-voltage compatible polarimeter for spin-resolved hard X-ray photoelectron spectroscopy (Spin-HAXPES) went into operation at beamline BL09XU of SPring-8 in Hyogo, Japan. The detector is based on the well-established principle of electron diffraction from a W(001) single-crystal at a scattering energy of 103.5 eV. It's special feature is that it can be operated at a high negative bias potential up to 10 kV, necessary to access the HAXPES range. The polarimeter is operated behind a large hemispherical analyzer (Scienta R-4000). It was optimized for high transmission of the transfer optics. A delay-line detector (20 mm dia.) is positioned at the exit plane of the…

010302 applied physicsSpectrum analyzerRadiationPhysics - Instrumentation and DetectorsSpin polarizationSpectrometerScatteringbusiness.industryChemistryFOS: Physical sciencesPolarimeterInstrumentation and Detectors (physics.ins-det)Condensed Matter Physics01 natural sciencesAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsOpticsX-ray photoelectron spectroscopyElectron diffraction0103 physical sciencesPhysical and Theoretical Chemistry010306 general physicsSpectroscopybusinessSpectroscopy
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Simplified feedback control system for scanning tunneling microscopy

2021

A Scanning Tunneling Microscope (STM) is one of the most important scanning probe tools available to study and manipulate matter at the nanoscale. In a STM, a tip is scanned on top of a surface with a separation of a few \AA. Often, the tunneling current between tip and sample is maintained constant by modifying the distance between the tip apex and the surface through a feedback mechanism acting on a piezoelectric transducer. This produces very detailed images of the electronic properties of the surface. The feedback mechanism is nearly always made using a digital processing circuit separate from the user computer. Here we discuss another approach, using a computer and data acquisition thr…

010302 applied physicsSuperconductivityPhysics - Instrumentation and DetectorsMaterials sciencebusiness.industrySerial communicationFOS: Physical sciencesWeyl semimetalPort (circuit theory)Instrumentation and Detectors (physics.ins-det)01 natural sciencesPiezoelectricityNoise (electronics)law.inventionCondensed Matter - Other Condensed MatterData acquisitionlawCondensed Matter::Superconductivity0103 physical sciencesOptoelectronicsScanning tunneling microscope010306 general physicsbusinessInstrumentationOther Condensed Matter (cond-mat.other)Review of Scientific Instruments
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Gasdynamic ECR ion source for negative ion production

2018

H− ion sources are needed in various areas of accelerator technology, such as beam injection into cyclotrons and storage rings and as a part of neutral beam injectors for plasma heating in experimental facilities studying thermonuclear fusion. It was recently demonstrated that gasdynamic ion source based on ECR discharge in a simple mirror trap is very efficient for proton beam production [1]. Here we use the gasdynamic plasma source as the first stage driver of volumetric negative ion production through dissociative electron attachment (DEA) [2]. Experiments were performed with a pulsed 37 GHz / up to 100 kW gyrotron radiation in a dual-trap magnetic system, which consists of two identical…

010302 applied physicsThermonuclear fusionMaterials scienceCyclotronElectronPlasma01 natural sciencesIon sourcelaw.inventionIonPhysics::Plasma PhysicslawGyrotron0103 physical sciencesPhysics::Accelerator PhysicsAtomic physics010306 general physicsInstrumentationMathematical PhysicsBeam (structure)Journal of Instrumentation
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Oxy-nitrides characterization with a new ERD-TOF system

2017

Abstract A new time-of-flight (TOF) camera was installed on Elastic Recoil Detection (ERD) measurement setup on the Tandem Accelerator at Universite de Montreal. The camera consists of two timing detectors, developed and built by the Jyvaskyla group, that use a thin carbon foil and microchannel plates (MCP) to produce the start and stop signals. The position of the first detector is fixed at 18 cm from the target, while the position of the second detector can be varied between 50 and 90 cm from the first detector. This allows to increase time resolution by increasing the distance between the time-of-flight detectors or to increase solid angle by decreasing the distance. Moving the detector …

010302 applied physicsToF-ERDANuclear and High Energy PhysicsIon beam analysisMicrochannelMaterials scienceta114Physics::Instrumentation and Detectorsbusiness.industryDetectorSolid angleion beam analysis02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesSignalelastic recoil detectionElastic recoil detectionOpticsPosition (vector)0103 physical sciences0210 nano-technologybusinessInstrumentationEnergy (signal processing)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Positron trapping defects in free-volume investigation of Ge–Ga–S–CsCl glasses

2016

Abstract Evolution of free-volume positron trapping defects caused by crystallization process in (80GeS 2 –20Ga 2 S 3 ) 100−х (СsCl) x , 0 ≤ x ≤ 15 chalcogenide-chalcohalide glasses was studied by positron annihilation lifetime technique. It is established that CsCl additives in Ge–Ga–S glassy matrix transform defect-related component spectra, indicating that the agglomeration of free-volume voids occurs in initial and crystallized (80GeS 2 –20Ga 2 S 3 ) 100−х (СsCl) x , 0 ≤ x ≤ 10 glasses. Void fragmentation in (80GeS 2 –20Ga 2 S 3 ) 85 (СsCl) 15 glass can be associated with loosing of their inner structure. Full crystallization in each of these glasses corresponds to the formation of defe…

010302 applied physicsVoid (astronomy)RadiationMaterials scienceAnalytical chemistryChalcogenide glassMineralogy02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesPositron trappingSpectral linelaw.inventionAbsorption edgeFragmentation (mass spectrometry)law0103 physical sciencesCrystallization0210 nano-technologyInstrumentationPositron annihilationRadiation Measurements
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