Search results for "Ford"

showing 10 items of 785 documents

Characterization of alpha sources prepared by direct evaporation using Rutherford backscattering spectrometry

1997

Abstract Standardization of solutions containing alpha emitting nuclides by direct evaporation onto metal supports is a widely used technique due to its simplicity in providing good quantitative results. In order to avoid inhomogeneity in the deposition surface, polished stainless steel disks and a spreading agent are generally used. These sources are usually measured by alpha spectrometry using passivated implanted silicon detectors. The resolution of the source is a measure of the thickness and homogeneity of the evaporated layer. Rutherford backscattering of He+ and H+ was here used to measure directly this thickness and homogeneity. The results were in agreement with semiconductor detec…

Nuclear and High Energy PhysicsMaterials scienceSiliconAlpha spectrometryPhysics::Instrumentation and DetectorsDetectorAnalytical chemistrychemistry.chemical_elementRutherford backscattering spectrometrySemiconductor detectorMetalchemistryvisual_artHomogeneity (physics)visual_art.visual_art_mediumNuclideInstrumentation
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Synthesis and characterization of cobalt silicide films on silicon

2006

Cobalt silicide has emerged as a leading contact material in silicon technology due to its low resistivity, high stability and small lattice mismatch. In this study, 0.2-0.4 mu m thick Co films were deposited on Si(100) wafers by RF magnetron sputtering at room temperature, and annealed at temperatures from 600 to 900 degrees C in vacuum. As-deposited and annealed samples were characterized by Rutherford backscattering spectrometry (RBS), nuclear reaction analysis (NRA), X-ray diffraction (XRD) and scanning electron microscopy (SEM). Although the Si substrates were sputter cleaned before the deposition, all the samples showed a thin oxide layer at the Si/Co interfaces. Annealing up to 700 d…

Nuclear and High Energy PhysicsMaterials scienceSiliconScanning electron microscopeAnnealing (metallurgy)Analytical chemistrychemistry.chemical_elementSputter depositionRutherford backscattering spectrometrychemistrySputteringElectrical resistivity and conductivityNuclear reaction analysisInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Global analysis of fragmentation functions for eta mesons

2011

Fragmentation functions for eta mesons are extracted at next-to-leading order accuracy of QCD in a global analysis of data taken in electron-positron annihilation and proton-proton scattering experiments. The obtained parametrization is in good agreement with all data sets analyzed and can be utilized, for instance, in future studies of double-spin asymmetries for single-inclusive eta production. The Lagrange multiplier technique is used to estimate the uncertainties of the fragmentation functions and to assess the role of the different data sets in constraining them.

Nuclear and High Energy PhysicsParticle physicsMesonCiencias FísicasElectron–positron annihilationHadronFOS: Physical sciencesElementary particle//purl.org/becyt/ford/1 [https]symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Fragmentation FunctionsNuclear ExperimentQuantum chromodynamicsPhysicsAnnihilation//purl.org/becyt/ford/1.3 [https]QcdEtaAstronomíaHigh Energy Physics - PhenomenologyLagrange multiplierData analysissymbolsHigh Energy Physics::ExperimentCIENCIAS NATURALES Y EXACTASHadronization
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Observation of charmonium pairs produced exclusively in $pp$ collisions

2014

A search is performed for the central exclusive production of pairs of charmonia produced in proton-proton collisions. Using data corresponding to an integrated luminosity of $3{\rm\ fb}^{-1}$ collected at centre-of-mass energies of 7 and 8 TeV, $J/\psi J/\psi$ and $J/\psi\psi(2S)$ pairs are observed, which have been produced in the absence of any other activity inside the LHCb acceptance that is sensitive to charged particles in the pseudorapidity ranges $(-3.5,-1.5)$ and $(1.5,5.0)$. Searches are also performed for pairs of P-wave charmonia and limits are set on their production. The cross-sections for these processes, where the dimeson system has a rapidity between 2.0 and 4.5, are measu…

Nuclear and High Energy PhysicsParticle physicsNuclear TheorydiffractionFOS: Physical sciencesLHCb - Abteilung HofmannHEAVY-ION COLLISIONSQCD diffraction charmoniaNOHigh Energy Physics - ExperimentLuminosityHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Quantum chromodynamiccharmonia; diffraction; QCDcharmonia; diffraction; QCD; Nuclear and High Energy PhysicsRapiditySDG 7 - Affordable and Clean EnergyNuclear ExperimentQCPhysics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyhep-ex12.38.-tParticle physicsHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronHEAVY-ION COLLISIONS; 450 GEV/C; DIFFRACTION; LHCQCDCromodinàmica quànticaLHCbDifracció450 GEV/CPseudorapidityPhysics::Accelerator PhysicscharmoniaFísica nuclearHigh Energy Physics::ExperimentProduction (computer science)LHCHEAVYFísica de partículesExperiments13.85.NiDiffractionQuantum chromodynamicsParticle Physics - ExperimentJournal of Physics G: Nuclear and Particle Physics
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Measurement of the semileptonic branching fraction of the B_{s} meson

2012

We report a measurement of the inclusive semileptonic branching fraction of the B_s meson using data collected with the BaBar detector in the center-of-mass (CM) energy region above the Upsilon(4S) resonance. We use the inclusive yield of phi mesons and the phi yield in association with a high-momentum lepton to perform a simultaneous measurement of the semileptonic branching fraction and the production rate of B_s mesons relative to all B mesons as a function of CM energy. The inclusive semileptonic branching fraction of the B_s meson is determined to be B(B_s to l nu X)=9.5 (+2.5/-2.0)(stat)(+1.1/-1.9)(syst)%, where l indicates the average of e and mu.

Nuclear and High Energy PhysicsParticle physicssemileptonic branching fractionMesonHigh Energy Physics::Latticesemileptonic branching fraction B_s mesonFOS: Physical sciences01 natural sciencesResonance (particle physics)semileptonic Bs-meson decaysHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Mesons (Nuclear physics)B mesonSDG 7 - Affordable and Clean EnergyMesons (Física nuclear)010306 general physicsNuclear Experiment14.40.Nd 13.20.HePhysics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energy010308 nuclear & particles physicsBranching fractionLeptons (Física nuclear)High Energy Physics::PhenomenologyBABAR detectorbranching fraction measurementHEPPACS: 14.40.Nd 13.20.HeBaBar detector at SLAC; semileptonic Bs-meson decays; branching fraction measurementLeptons (Nuclear physics)Yield (chemistry)BaBarB_s mesonHigh Energy Physics::ExperimentBaBar detector at SLACsemileptonic Bs-meson decayLeptonProduction rate
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Characterization of 233U alpha recoil sources for 229()Th beam production

2019

Radioactive $^{233}$U alpha recoil sources are being considered for the production of a thorium ion source to study the low-energy isomer in $^{229}$Th with high-resolution collinear laser spectroscopy at the IGISOL facility of the University of Jyv\"askyl\"a. In this work two different $^{233}$U sources have been characterized via alpha and gamma spectroscopy of the decay radiation obtained directly from the sources and from alpha-recoils embedded in implantation foils. These measurements revealed rather low $^{229}$Th recoil efficiencies of only a few percent. Although the low efficiency of one of the two sources can be attributed to its inherent thickness, the low recoil efficiency of th…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsMaterials sciencePhysics::Instrumentation and Detectors010308 nuclear & particles physicsRadioactive sourceFOS: Physical sciencesThoriumchemistry.chemical_elementInstrumentation and Detectors (physics.ins-det)RadiationRutherford backscattering spectrometry01 natural sciencesIon sourceRecoilchemistry0103 physical sciencesGamma spectroscopyNuclear Experiment (nucl-ex)Atomic physicsNuclear Experiment010306 general physicsSpectroscopyNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Energy calibration of the NEXT-White detector with 1% resolution near Q ββ of 136Xe

2019

Excellent energy resolution is one of the primary advantages of electroluminescent high pressure xenon TPCs, and searches for rare physics events such as neutrinoless double-beta decay ($\beta\beta0\nu$) require precise energy measurements. Using the NEXT-White detector, developed by the NEXT (Neutrino Experiment with a Xenon TPC) collaboration, we show for the first time that an energy resolution of 1% FWHM can be achieved at 2.6 MeV, establishing the present technology as the one with the best energy resolution of all xenon detectors for $\beta\beta0\nu$ searches.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysical measurementsPhysics::Instrumentation and DetectorsDark Matter and Double Beta DecayFísica -- Mesuramentschemistry.chemical_elementBioengineeringAtomic01 natural sciencesMathematical SciencesNuclear physicsParticle and Plasma PhysicsXenonAffordable and Clean Energy0103 physical sciencesDark Matter and Double Beta Decay (experiments)CalibrationNuclearlcsh:Nuclear and particle physics. Atomic energy. RadioactivityCalibratge010306 general physicsMathematical PhysicsPhysicsQuantum Physics010308 nuclear & particles physicsDetectorResolution (electron density)MolecularDetectorsNuclear & Particles PhysicsFull width at half maximumchemistryBeta (plasma physics)Physical SciencesCalibrationlcsh:QC770-798High Energy Physics::ExperimentNeutrinoEnergy (signal processing)
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Time-of-flight telescope for heavy-ion RBS

2007

Abstract This paper describes a time-of-flight (TOF) spectrometer for Heavy-Ion Rutherford Backscattering Spectrometry (HI-RBS) recently installed at IMEC for thin film analysis. The TOF telescope allows the use of ion beams heavier than He, with advantages in terms of depth and mass resolution and sensitivity compared to conventional RBS based on planar Si detectors. The start timing-signal is produced by the secondary electrons emitted from a thin C foil when traversed by a backscattered ion; the electrons are deflected in an electrostatic mirror towards a Micro-channel plate (MCP) assembly which provides a fast timing response. The stop signal is obtained directly from a second MCP assem…

Nuclear and High Energy PhysicsSpectrometerPhysics::Instrumentation and Detectorsbusiness.industryChemistryRutherford backscattering spectrometrySecondary electronslaw.inventionIonElastic recoil detectionTelescopeTime of flightOpticslawTime-of-flight mass spectrometrybusinessInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Estimates of the Nuclear Time Delay in Dissipative U + U and U + Cm Collisions Derived from the Shape of Positron andδ-Ray Spectra

1983

Positron and delta-ray spectra have been measured in coincidence with quasielastic scattered particles and fission fragments from the bombardment of Pd, U, and Cm targets with U beams of energies between 5.9 and 8.4 MeV/u. For collisions leading to a fission reaction, the atomic positron and delta-ray spectra fall off more steeply at high energies than expected from calculations based on pure Rutherford trajectories. A quantitative analysis of this effect is in accord with a nuclear contact time of about 10/sup -21/ s.

Nuclear reactionElastic scatteringPhysicsAntiparticleFissionAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryGeneral Physics and AstronomyNuclear physicssymbols.namesakePositronNuclear fissionAntimattersymbolsPhysics::Accelerator PhysicsRutherford scatteringAtomic physicsNuclear ExperimentPhysical Review Letters
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Available Lysine in Protein, Assay Using o-Phthalaldehyde/ N-Acetyl-L-cysteine Spectrophotometric Method

1992

An assay was based on reaction of free e-amino groups in proteins with the o-phthalaldehyde/N-acetyl-L-cysteine reagent to form isoindoles, which absorb at 335 nm. The procedure was suitable for proteins or mixtures of proteins with available lysine contents of more than 5 moles lysine/mole protein and required absence of free amino acids and peptides. This method was simpler and more convenient than other methods, since it did not require hydrolysis, amino acid analysis, long heating periods or solvent extraction.

O-PhthalaldehydeHydrolysisChromatographyIsoindolesmedicine.diagnostic_testChemistrySpectrophotometryReagentLysineMolemedicineBradford protein assayFood ScienceJournal of Food Science
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