Search results for "POLARIZATION"

showing 10 items of 1884 documents

Deuteron photodisintegration by polarized photons in the region of the $d^*(2380)$

2019

We report the first large-acceptance measurement of the beam–spin asymmetry for deuteron photodisintegration (γ→d→pn) in the photon energy range 420<Eγ<620MeV. The measurement provides important new constraints on the mechanisms of photodisintegration above the Δ resonance and on the photocoupling of the recently discovered d⁎(2380) hexaquark.

Nuclear and High Energy PhysicsPhotonmedia_common.quotation_subjectNuclear TheoryHexaquarkFOS: Physical sciencesPhoton energy01 natural sciencesAsymmetryResonance (particle physics)Nuclear physics0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear Experimentmedia_commonPhysicsRange (particle radiation)010308 nuclear & particles physicsPhysicslcsh:QC1-999DeuteriumPhotodisintegrationlcsh:Physicsproton polarization ; cross-section ; disintegration ; asymmetry ; energies
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Gravitational depolarization of ultracold neutrons : comparison with data

2015

We compare the expected effects of so-called gravitationally enhanced depolarization of ultracold neutrons to measurements carried out in a spin-precession chamber exposed to a variety of vertical magnetic-field gradients. In particular, we have investigated the dependence upon these field gradients of spin depolarization rates and also of shifts in the measured neutron Larmor precession frequency. We find excellent qualitative agreement, with gravitationally enhanced depolarization accounting for several previously unexplained features in the data.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsField (physics)FOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsGravitationHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]NeutronDetectors and Experimental Techniques010306 general physicsQCLarmor precessionPhysics010308 nuclear & particles physics1420DhDepolarizationInstrumentation and Detectors (physics.ins-det)Magnetic field gradient1130Ernumbers: 1340Em0755GeElectric dipole momentPhysics::Space PhysicsUltracold neutronsAtomic physics
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Measurements of $R^{d}-R^{p}$ and $R^{Ca}-R^{C}$ in deep inelastic muon scattering

1992

Results are presented on the difference in R, the ratio of longitudinally to transversely polarised virtual photon absorption cross sections, for the deuteron and the proton. They are obtained by c ...

Nuclear and High Energy PhysicsProtonmuon nucleus: deep inelastic scatteringNuclear Theorypolarization: longitudinaldeep inelastic scattering: muon deuteronVirtual particlecross section: ratiophoton: absorptionElementary particlemuon deuteron: deep inelastic scattering530Nuclear physicsabsorption: photondeep inelastic scattering: muon ppolarization: transverseHIGH STATISTICS MEASUREMENT; R=SIGMA-L/SIGMA-T; HIGH Q2Nuclear ExperimentAbsorption (electromagnetic radiation)deep inelastic scattering: muon nucleus90: 200: 280 GeVPhysicsHIGH STATISTICS MEASUREMENTMuoncalciumScatteringcarbonstructure function: ratioR=SIGMA-L/SIGMA-TCERN SPSlongitudinal: polarizationParticle scatteringDeuteriummuon p: deep inelastic scatteringHIGH Q2Physics::Accelerator Physicstransverse: polarizationAtomic physicsParticle Physics - Experimentexperimental results
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Magnetic resonance imaging of dissolved hyperpolarized 129Xe using a membrane-based continuous flow system.

2009

Abstract A technique for continuous production of solutions containing hyperpolarized 129Xe is explored for MRI applications. The method is based on hollow fiber membranes which inhibit the formation of foams and bubbles. A systematic analysis of various carrier agents for hyperpolarized 129Xe has been carried out, which are applicable as contrast agents for in vivo MRI. The image quality of different hyperpolarized Xe solutions is compared and MRI results obtained in a clinical as well as in a nonclinical MRI setting are provided. Moreover, we demonstrate the application of 129Xe contrast agents produced with our dissolution method for lung MRI by imaging hyperpolarized 129Xe that has been…

Nuclear and High Energy PhysicsPulmonary Circulationmedicine.diagnostic_testContinuous flowChemistryPhantoms ImagingBiophysicsLung perfusionMagnetic resonance imagingBiocompatible MaterialsMembranes ArtificialCondensed Matter PhysicsBiochemistryMagnetic Resonance ImagingImaging phantomSolutionsMembraneNuclear magnetic resonancemedicineImage Processing Computer-AssistedRespiratory MechanicsXenon IsotopesHyperpolarization (physics)LungJournal of magnetic resonance (San Diego, Calif. : 1997)
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Effect of atomic vibrations in XANES: polarization-dependent damping of the fine structure at the Cu K-edge of (creat)2CuCl4

2016

Polarization-dependent damping of the fine structure in the CuK-edge spectrum of creatinium tetrachlorocuprate [(creat)2CuCl4] in the X-ray absorption near-edge structure (XANES) region is shown to be due to atomic vibrations. These vibrations can be separated into two groups, depending on whether the respective atoms belong to the same molecular block; individual molecular blocks can be treated as semi-rigid entities while the mutual positions of these blocks are subject to large mean relative displacements. The effect of vibrations can be efficiently included in XANES calculations by using the same formula as for static systems but with a modified free-electron propagator which accounts f…

Nuclear and High Energy PhysicsRadiationMaterials scienceStructure (category theory)Propagator02 engineering and technology021001 nanoscience & nanotechnologyBlock (periodic table)01 natural sciencesMolecular physicsXANESVibrationK-edge0103 physical sciencesPolarization dependentAbsorption (chemistry)010306 general physics0210 nano-technologyInstrumentationJournal of Synchrotron Radiation
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Spin transition in iron complexes induced by heat, pressure, light and nuclear decay

1988

The phenomenon of temperature-dependent spin transition will be introduced and the numerous chemical and physical influences affecting the spin transition characteristics will be discussed. We shall mainly concentrate on the spin crossover system [Fe(2-pic)3]X2·Sol (2-pic=2-aminomethylpyridine; X=Cl, Br; Sol=C2H5OH, CH3OH) and demonstrate how the behaviour of the spin transition5T2g(Oh)⇌1A1g(Oh) is influenced by substituting the metalion, the non-coordinating anions X, the crystal solvent molecules Sol and by isotopic exchange with H/D and14N/15N. It will also be shown that the spin transition is very susceptible to pressure. A quantitative spin state conversion from low spin to high spin c…

Nuclear and High Energy PhysicsSpin statesCondensed matter physicsSpin polarizationChemistrySpin transitionZero field splittingCondensed Matter PhysicsAtomic and Molecular Physics and OpticsLIESSTSpin crossoverSpin waveCondensed Matter::Strongly Correlated ElectronsPhysical and Theoretical ChemistryAtomic physicsQuantum spin liquidHyperfine Interactions
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Search for right-handed W bosons in top quark decay

2005

We present a measurement of the fraction f+ of right-handed W bosons produced in top quark decays, based on a candidate sample of $t\bar{t}$ events in the lepton+jets decay mode. These data correspond to an integrated luminosity of 230pb^-1, collected by the DO detector at the Fermilab Tevatron $p\bar{p}$ Collider at sqrt(s)=1.96 TeV. We use a constrained fit to reconstruct the kinematics of the $t\bar{t}$ and decay products, which allows for the measurement of the leptonic decay angle $\theta^*$ for each event. By comparing the $\cos\theta^*$ distribution from the data with those for the expected background and signal for various values of f+, we find f+=0.00+-0.13(stat)+-0.07(syst). This …

Nuclear and High Energy PhysicsTop quarkParticle physicsstandard modelTevatronFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)quark decay0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilabelementary particle jets010306 general physicsBosonPhysicsproton-proton inclusive interactionsRight handed010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPolarization (waves)meson leptonic decayHelicity14.65.Ha 14.70.Fm 12.15.Ji 12.38.Qkhigh-energy elementary particle interactionsHigh Energy Physics::Experimentintermediate boson productionLepton
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The BLAST experiment

2009

The Bates large acceptance spectrometer toroid (BLAST) experiment was operated at the MIT-Bates Linear Accelerator Center from 2003 until 2005. The detector and experimental program were designed to study, in a systematic manner, the spin-dependent electromagnetic interaction in few-nucleon systems. As such the data will provide improved measurements for neutron, proton, and deuteron form factors. The data will also allow details of the reaction mechanism, such as the role of final state interactions, pion production, and resonances to be studied. The experiment used: a longitudinally polarized electron beam stored in the South Hall Storage Ring; a highly polarized, isotopically pure, inter…

Nuclear and High Energy PhysicsTracking detectorScintillator detectorCherenkov detectorNuclear TheoryLinear particle acceleratorlaw.inventionNuclear physicslawNeutron detectionSCATTERINGNeutronSPECTROMETERSTORAGE-RINGBLASTPHOTOEMISSIONNuclear ExperimentInstrumentationCherenkov radiationELECTRON-SPIN POLARIZATIONPhysicsPolarized beamSpectrometerPolarized targetDetectorGAASGAS-TARGETPERFORMANCEPOLARIMETERStorage ringStorage ringSYSTEMCherenkov detectorNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors, and Associated Equipment
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Measurement of proton and nitrogen polarization in ammonia and a test of equal spin temperature

1998

The 1996 data taking of the SMC experiment used polarized protons to measure the spin-dependent structure function g(1) of the proton. Three liters of solid granular ammonia were irradiated at the Bonn electron linac in order to create the paramagnetic radicals which are needed for polarizing the protons. Proton polarizations of +/- (90 +/- 2.5)% were routinely reached. An analysis based on a theoretical line shape for spin-1. systems with large quadrupolar broadening was developed which allowed the nitrogen polarization in the ammonia to be determined with a 10% relative error. The measured quadrupolar coupling constant of N-14 agrees well with earlier extrapolated values. The polarization…

Nuclear and High Energy Physicsspin resonanceProtonp polarized targetNuclear Theorychemistry.chemical_elementAmmoniachemistry.chemical_compoundParamagnetismIrradiationDetectors and Experimental TechniquesNuclear ExperimentInstrumentationPhysicsCoupling constantpolarizationquadrupolar interactionsPolarization (waves)Nitrogennitrogen polarized targetdynamic nuclearnuclear magnetic resonancechemistryDeuteriump polarized target; nitrogen polarized target; spin resonanceAtomic physics
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Spin Polarization of Electrons by Resonance Scattering from Mercury

1980

Hg- compound ion states formed by electron impact with neutral mercury atoms at collision energies of 4.55, 4.71, 4.94, and 5.51 eV show up in the 2S1/2, 2D3/2, 2D5/2, and 2D5/2 scattering states in order of increasing energy. This identification is supported by the observed energy dependence of (i) elastic (e-, Hg) differential cross section, of (ii) 63P0 excitation of mercury by electron impact, and of (iii) spin polarization of electrons scattered elastically from mercury.

Nuclear magnetic resonanceX-ray Raman scatteringMaterials scienceSpin polarizationchemistryScatteringchemistry.chemical_elementElectronMott scatteringAtomic physicsElectron ionizationMercury (element)Ion
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