Search results for " nuclear"

showing 10 items of 11776 documents

Single Event Upsets Induced by Direct Ionization from Low-Energy Protons in Floating Gate Cells

2017

Floating gate cells in advanced NAND Flash memories, with single-level and multi-level cell architecture, were exposed to low-energy proton beams. The first experimental evidence of single event upsets by proton direct ionization in floating gate cells is reported. The dependence of the error rate versus proton energy is analyzed in a wide energy range. Proton direct ionization events are studied and energy loss in the overlayers is discussed. The threshold LET for floating gate errors in multi-level and single-level cell devices is modeled and technology scaling trends are analyzed, also discussing the impact of the particle track size. peerReviewed

protonitNuclear and High Energy PhysicsProtonfloating gate devicesNAND gateFlash memories01 natural sciencesComputer Science::Hardware ArchitectureIonizationFlash memories; floating gate devices; protons; single event effects; Nuclear and High Energy Physics; Nuclear Energy and Engineering; Electrical and Electronic Engineering0103 physical sciencesHardware_ARITHMETICANDLOGICSTRUCTURESElectrical and Electronic Engineeringflash-muistit010302 applied physicsPhysicsRange (particle radiation)ta114ta213protons010308 nuclear & particles physicsbusiness.industryElectrical engineeringsingle event effectsNon-volatile memoryNuclear Energy and EngineeringLogic gateAtomic physicsbusinessEvent (particle physics)Energy (signal processing)IEEE Transactions on Nuclear Science
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High-gradient accelerating structure studies and their application in hadrontherapy

2013

198 páginas. Tesis doctoral del Departamento de Física Atómica, Molecular y Nuclear, de la Universidad de Valencia.

protontherapycarbon ion therapyRF breakdown:FÍSICA::Física atómica y nuclear ::Otras [UNESCO]cyclinacshigh gradientslinacs:FÍSICA::Nucleónica::Aceleradores de partículas [UNESCO]hadrontherapyUNESCO::FÍSICA::Nucleónica::Aceleradores de partículasproton therapyUNESCO::FÍSICA::Física atómica y nuclear ::Otrascarbontherapy
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Poly[[tetramethanolbis[4-oxo-3-(pyridin-4-yl)-1-(2,4,6-trichlorophenyl)-4,5-dihydro-1H-pyrazolo[3,4-d]pyrimidin-6-olato]disodium]–diethyl ether–metha…

2016

In the title compound, [Na2(C16H7Cl3N5O2)2(CH3OH)4]·C4H10O·2CH3OH, the central pyrazolo[3,4-d]pyrimidine system makes dihedral angles of 82.98 (7)° with the trichlorophenyl ring and 13.11 (15)° with the pyridine ring. The sodium ion has an octahedral environment, being coordinated by four methanol molecules and one O and one N atom of two different heterocyclic ring systems.

pyridinecrystal structure246-trichlorophenylPyrimidineStereochemistryCrystal structureDihedral angle010403 inorganic & nuclear chemistryRing (chemistry)01 natural sciencesMedicinal chemistrychemistry.chemical_compoundPyridinelcsh:QD901-999sodiumbiology010405 organic chemistrypyrazolo[34-d]pyrimidin-6-olateGeneral Medicinebiology.organism_classification0104 chemical scienceschemistryTetralcsh:CrystallographyMethanolDiethyl etherIUCrData
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(E)-1-(Pyridin-4-yl)propan-1-one O-tosyl oxime

2017

The title compound, C15H16N2O3S, was obtained by the reaction of (E)-1-(pyridin-4-yl)propan-1-one oxime andpara-toluenesulfonic acid. The pyridine ring makes a dihedral angle of 54.70 (10)° with the benzene ring. In the crystal, molecules are linked by C—H...O hydrogen bonds, forming a chain along thec-axis direction.

pyridinecrystal structureHydrogen bondCrystal structureDihedral angle010402 general chemistry010403 inorganic & nuclear chemistryRing (chemistry)Oximehydrogen bonding01 natural sciences0104 chemical sciencesCrystalchemistry.chemical_compoundCrystallographytosyl oximechemistryTosylPyridinelcsh:QD901-999lcsh:CrystallographyIUCrData
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3-(2,4-Difluorophenyl)-1-(pyridin-4-yl)benzo[4,5]imidazo[1,2-d][1,2,4]triazin-4(3H)-one

2016

In the title compound, C20H11F2N5O, the central 13-membered ring system (r.m.s. deviation = 0.028 Å) makes a dihedral angle of 53.13 (7)° with the difluorophenyl ring and 79.98 (7)° with the pyridine ring. The crystal packing features aromatic π–π interactions between the 13-membered rings [shortest distance between ring centroids = 3.5682 (8) Å].

pyridinecrystal structureShortest distanceStereochemistryChemistryGeneral MedicineCrystal structuredifluorophenylDihedral angle010402 general chemistry010403 inorganic & nuclear chemistryRing (chemistry)01 natural sciences124-triazinone0104 chemical sciencesbenzoimidazoleCrystalCrystallographychemistry.chemical_compoundPyridinelcsh:QD901-999lcsh:CrystallographyIUCrData
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Halogen Bonds in 2,5-Dihalopyridine-Copper(I) Halide Coordination Polymers

2019

Two series of 2,5-dihalopyridine-Cu(I)A (A = I, Br) complexes based on 2-X-5-iodopyridine and 2-X-5-bromopyridine (X = F, Cl, Br and I) are characterized by using single-crystal X-ray diffraction analysis to examine the nature of C2&minus

pyridinedihalopyridineSupramolecular chemistrychemistry.chemical_elementHalidekupari010402 general chemistry01 natural scienceslcsh:TechnologyArticlechemistry.chemical_compoundkemialliset sidoksetPyridineGeneral Materials Sciencelcsh:Microscopypolymeeritlcsh:QC120-168.85chemistry.chemical_classificationHalogen bondlcsh:QH201-278.5010405 organic chemistrylcsh:TPolymerkompleksiyhdisteetCopper3. Good health0104 chemical sciencesCrystallographyhalopyridineschemistrylcsh:TA1-2040copperHalogenFluorinehalogeenisidoksetlcsh:Descriptive and experimental mechanicshalogen bondlcsh:Electrical engineering. Electronics. Nuclear engineeringlcsh:Engineering (General). Civil engineering (General)lcsh:TK1-9971
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Highly occupied gauge theories in 2 + 1 dimensions : a self-similar attractor

2019

Motivated by the boost-invariant Glasma state in the initial stages in heavy-ion collisions, we perform classical-statistical simulations of SU(2) gauge theory in 2+1 dimensional space-time both with and without a scalar field in the adjoint representation. We show that irrespective of the details of the initial condition, the far-from-equilibrium evolution of these highly occupied systems approaches a unique universal attractor at high momenta that is the same for the gauge and scalar sectors. We extract the scaling exponents and the form of the distribution function close to this non-thermal fixed point. We find that the dynamics are governed by an energy cascade to higher momenta with sc…

quark-gluon plasmaScalar (mathematics)Adjoint representationhep-latFOS: Physical scienceshiukkasfysiikka114 Physical sciences01 natural sciencesComputer Science::Digital Librariessymbols.namesakeHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Correlation functionfysikk0103 physical sciencesAttractorquantum chromodynamicsGauge theory010306 general physicsUNIVERSAL DYNAMICSParticle Physics - PhenomenologyMathematical physicsDebyePhysics:Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP]010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)finite temperature field theoryParticle Physics - Latticehep-ph115 Astronomy Space scienceHigh Energy Physics - PhenomenologyDistribution functionsymbolsScalar fieldrelativistic heavy-ion collisions
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High Bias Voltage CZT Detectors for High-flux Measurements

2017

In this work, we present the performance of new travelling heater method (THM) grown CZT detectors, recently developed at IMEM-CNR Parma, Italy. Thick planar detectors (3 mm thick) with gold electroless contacts on CZT crystals grown by Redlen Technologies (Victoria BC, Canada) were realized, with a planar cathode covering the detector surface (4.1 x 4.1 mm(2)) and a central anode (2 x 2 mm(2)) surrounded by a guard ring electrode. The detectors, characterized by low leakage currents at room temperature (4.7 nA/cm(2) at 1000 V/cm), allow good room temperature operation even at high bias voltages (> 7000 V/cm). At low rates, the detectors exhibit an energy resolution around 4 % FWIEM at 59.5…

radiation detectorRadiology Nuclear Medicine and ImagingMaterials sciencePreamplifier02 engineering and technology01 natural scienceslaw.inventionlawpixel0103 physical sciencesInstrumentationNuclear and High Energy Physic010308 nuclear & particles physicsbusiness.industryDetectorSettore FIS/01 - Fisica SperimentaleElectrical engineeringBiasing021001 nanoscience & nanotechnologyPhoton countingCathodeSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)AnodeElectronic Optical and Magnetic MaterialsCZTFull width at half maximumHigh Fluxhigh bias voltageOptoelectronicssemiconductor detector0210 nano-technologybusinessVoltage
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Microscale X-ray mapping of CZT arrays: Spatial dependence of amplitude, shape and multiplicity of detector pulses

2018

In this work, we present the results of a microscale X-ray mapping of a 2 mm thick CZT pixel detector, with pixel pitches of 500 μm and 250 μm, using collimated synchrotron X-ray sources at the Diamond Light source (U. K.). The detector is dc coupled to a fast and low noise ASIC (PIXIE ASIC), characterized only by the preamplifier stage. A custom 16-channel digital readout electronics was used, able to perform online fast pulse shape and height analysis (PSHA), with low dead time and reasonable energy resolution at both low and high fluxes. The detector allows high bias voltage operation (> 5000 V/cm) and good energy resolution at room temperature (5.3 %, 2.3 % and 2.1 % FWHM at 22.1, 59…

radiation detectorRadiology Nuclear Medicine and ImagingNuclear and High Energy PhysicsMaterials sciencePreamplifier01 natural sciencesCollimated light030218 nuclear medicine & medical imagingCharge sharinglaw.invention03 medical and health sciences0302 clinical medicineOpticslaw0103 physical scienceshigh fluxmappingInstrumentation010308 nuclear & particles physicsbusiness.industryASICDetectorBiasingDead timeSynchrotronSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)CZTFull width at half maximumsinchrotron radiationbusiness
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THERP and HEART integrated methodology for human error assessment

2014

Medical errors are one of the leading causes of death and injury in radiation therapy administration as reported in the literature. This point out an overall deficiency in management allowing patient treatment in the absence of suitable quality assurance processes. Clinical records of major accidental exposure events in radiotherapy show that there is a combination of factors contributing to the accident such as deficient staff training, lack of independent checks, lack of quality control procedures, and absence of overall supervision. Another finding is that training generally addresses only normal situations and does not prepare radiotherapy staff for unusual situations, resulting in a la…

radiation therapy patient safety human errors fuzzy THERP.Settore ING-IND/20 - Misure E Strumentazione NucleariSettore ING-IND/19 - Impianti Nucleari
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