Search results for "mass [target]"

showing 10 items of 514 documents

Seesaw Majoron Model of Neutrino Mass and Novel Signals in Higgs Boson Production at LEP

1998

We perform a careful study of the neutral scalar sector of a model which includes a singlet, a doublet, and a triplet scalar field under $SU(2)$. This model is motivated by neutrino physics, since it is simply the most general version of the seesaw model of neutrino mass generation through spontaneous violation of lepton number. The neutral Higgs sector contains three CP-even and one massive CP-odd Higgs boson $A$, in addition to the massless CP-odd majoron $J$. The weakly interacting majoron remains massless if the breaking of lepton number symmetry is purely spontaneous. We show that the massive CP-odd Higgs boson may invisibly decay to three majorons, as well as to a CP-even Higgs $H$ bo…

Modelo de MasonPhysicsNuclear and High Energy PhysicsParticle physicsMass generationHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesLepton numberHigh Energy Physics - ExperimentHiggs sectorHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Equilibrio de masaHiggs bosonHigh Energy Physics::ExperimentSeñales de bosones de Higgs en LEPNeutrinosNeutrinoScalar fieldBosonMajoron
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Drying of shrinking cylinder-shaped bodies

1998

Abstract A mathematical model has been developed for the prediction of sample temperature, average moisture and moisture distribution in a cylinder-shaped solid during the drying process. The effect of shrinkage was taken into account. The macroscopic heat balance and the microscopic mass balance combined with Fick's law were simultaneously solved using the Runge-Kutta-Merson method and a numerical finite difference method. The effective diffusion coefficient was expressed as a function of sample temperature and local moisture content. Using an experimental drying curve determined at 90 °C, the diffusional equation was identified for broccoli stems, and was used to predict the average and l…

MoistureChemistryFinite difference methodMineralogyMechanicsCylinder (engine)law.inventionlawMass transferEffective diffusion coefficientSolid bodyWater contentPhysics::Atmospheric and Oceanic PhysicsFood ScienceShrinkageJournal of Food Engineering
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NMR Studies of Single-File Diffusion in Unidimensional Channel Zeolites

1996

Single-file diffusion is the restricted propagation of particles that cannot pass each other. The occurrence of this phenomenon should be reflected by a change in the time dependence of the mean particle displacement in comparison with ordinary diffusion. Although this process is considered to be the rate-controlling mechanism in a large variety of processes, so far no direct evidence of this phenomenon has been provided. Diffusion measurements made with pulsed field gradient nuclear magnetic resonance (NMR) in unidimensional pore systems (zeolites AlPO4-5 and Theta-1) reflect the expected time dependence of single-file diffusion.

MultidisciplinaryChemical physicsChemistryScientific methodMass transferAnalytical chemistryParticle displacementCrystalliteDiffusion (business)PorosityPulsed field gradientMagnetosphere particle motionScience
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Precision Measurement of the Mass and Lifetime of the Ξ[0 over b] Baryon

2014

Using a proton-proton collision data sample corresponding to an integrated luminosity of 3 fb$^{-1}$ collected by LHCb at center-of-mass energies of 7 and 8 TeV, about 3800 $\Xi_b^0\to\Xi_c^+\pi^-$, $\Xi_c^+\to pK^-\pi^+$ signal decays are reconstructed. From this sample, the first measurement of the $\Xi_b^0$ baryon lifetime is made, relative to that of the $\Lambda_b^0$ baryon. The mass differences $M(\Xi_b^0)-M(\Lambda_b^0)$ and $M(\Xi_c^+)-M(\Lambda_c^+)$ are also measured with precision more than four times better than the current world averages. The resulting values are $\frac{\tau_{\Xi_b^0}}{\tau_{\Lambda_b^0}} = 1.006\pm0.018\pm0.010$, $M(\Xi_b^0) - M(\Lambda_b^0) = 172.44\pm0.39\pm…

Nuclear TheoryAnalytical chemistryGeneral Physics and Astronomyinclusive weak decays; discarding 1/N(C); beaty; charm; ruleLambdaHigh Energy Physics - Experimenthigh energy physicsSettore FIS/04 - Fisica Nucleare e Subnucleare[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]INCLUSIVE WEAK DECAYS; DISCARDING 1/N(C); BEAUTY; CHARM; RULENuclear ExperimentQCPhysicsprecision measurementPhysicsintegrated luminosityParticle physicsBEAUTYtransverse momentaPseudorapidityPhysical SciencesTransverse momentumINCLUSIVE WEAK DECAYSFísica nuclearLHC13.30.Egtellurium compoundsParticle Physics - Experiment530 PhysicsAstrophysics::High Energy Astrophysical PhenomenaPhysics MultidisciplinarypseudorapiditiesPhysics InstituteLHCb - Abteilung HofmannAstrophysics::Cosmology and Extragalactic AstrophysicsCHARMNuclear physicsPhysics and Astronomy (all)Pi14.20.MrScience & Technologycenter-of-mass energiesmass differencetransverse momenta; precision measurement; center-of-mass energies; tellurium compounds; production rates; pseudorapidities; high energy physics; integrated luminosity; hadrons; mass difference; proton proton collisionsDISCARDING 1/N(C)BaryonLHCbproton proton collisionshadronsHadronic decays of baryonBottom baryons (|B|>0)Physics::Accelerator Physicsproduction ratesFísica de partículesExperimentsRULE
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A compact apparatus for mass selective resonance ionization spectroscopy in a buffer gas cell

1997

Abstract An ultra-sensitive laser spectroscopic method for the investigation of transuranium nuclides has been developed based on resonance ionization in an argon buffer gas cell. This method has been combined with ion-guide extraction and mass selective direct detection of the resonantly ionized atoms. Using argon as a buffer gas, recoils of fusion reactions can be thermalized even at low pressure. The differential pumping system consists of only one roots pump and two turbo molecular pumps. The set-up has been tested with 243 Am evaporated from a filament located inside the optical gas cell. Resonance ionization is performed using a two-step excitation with an excimer-dye-laser combinatio…

Nuclear and High Energy PhysicsArgonBuffer gasAnalytical chemistrychemistry.chemical_elementMass spectrometryIon sourceAtmospheric-pressure laser ionizationchemistryIonizationAtomic physicsInstrumentationQuadrupole mass analyzerElectron ionizationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Physics at CERN's Antiproton Decelerator

2013

The Antiproton Decelerator of CERN began operation in 1999 to serve experiments for studies of CPT invariance by precision laser and microwave spectroscopy of antihydrogen ($\bar{\rm H}$) and antiprotonic helium ($\bar{p}{\rm He}^+$). The first 12 years of operation saw cold $\bar{\rm H}$ synthesized by overlapping clouds of positrons ($e^+$) and antiprotons ($\bar{p}$) confined in magnetic Penning traps. Cold $\bar{\rm H}$ was also produced in collisions between Rydberg positronium atoms and $\bar{p}$. Ground-state $\bar{\rm H}$ was later trapped for up to $\sim 1000$ s in a magnetic bottle trap, and microwave transitions excited between its hyperfine levels. In the $\bar{p}{\rm He}^+$ ato…

Nuclear and High Energy PhysicsAtomic Physics (physics.atom-ph)Other Fields of PhysicsFOS: Physical sciences7. Clean energy01 natural sciencesPhysics - Atomic PhysicsHigh Energy Physics - ExperimentPositroniumHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentHyperfine structureAntiprotonic heliumPhysicsMagnetic moment010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMass ratioAntiproton Decelerator13. Climate actionAntiprotonHigh Energy Physics::ExperimentRotational spectroscopyAtomic physics
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Determination of mass attenuation coefficient by numerical absorption calibration with Monte-Carlo simulations at 59.54 keV

2016

Abstract This study presents a numerical method in order to determine the mass attenuation coefficient of a sample with an unknown chemical composition at low energy. It is compared with two experimental methods: a graphic method and a transmission method. The method proposes to realise a numerical absorption calibration curve to process experimental results. Demineralised water with known mass attenuation coefficient ( 0.2066 cm 2 g − 1 at 59.54 keV) is chosen to confirm the method. 0.1964 ± 0.0350 cm 2 g − 1 is the average value determined by the numerical method, that is to say less than 5% relative deviation compared to more than 47% for the experimental methods.

Nuclear and High Energy PhysicsCalibration curveMonte Carlo method[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]010403 inorganic & nuclear chemistry01 natural sciences030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineOpticsTransmission geometryTransmission methodCalibrationMass attenuation coefficientMass attenuation coefficient[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Absorption (electromagnetic radiation)[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]InstrumentationChemical compositionPhysicsbusiness.industryNumerical analysisSelf-absorptionMonte-Carlo method0104 chemical sciencesComputational physicsbusinessGamma spectrometry
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Quadrupole interaction of $^{8}$Li and $^{9}$Li in LiNbO$_{3}$ and the quadrupole moment of $^{9}$Li

1988

The quadrupole interaction of nuclear spin polarized8Li (I=2) and9Li (I=3/2) in LiNbO3 has been studied at room temperature. The polarization was achieved by optical pumping of a fast atomic beam with circularly polarized laser light. The atoms were implanted into a hexagonal LiNbO3 single crystal and the quadrupole splitting ofβ-NMR spectra was measured. A ratio of ¦Q(9Li)/Q(8Li)¦=0.88(4) for the nuclear quadrupole moments was deduced, yielding a new value of ¦Q(9Li)¦=25.3 (9) mb for the quadrupole moment of9Li.

Nuclear and High Energy PhysicsChemistryIsotopes of lithiumNuclear TheoryPhysics::OpticsQuadrupole splittingSpectral lineOptical pumpingQuadrupolePhysics::Accelerator PhysicsNuclear fusionNuclear Physics - ExperimentPhysics::Atomic PhysicsAtomic physicsQuadrupole mass analyzerSingle crystal
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Ramsey technique applied in a Penning trap mass spectrometer

1991

Abstract The Ramsey method has been applied in an experiment aiming for accurate mass determination of unstable isotopes. The ion motion in a Penning trap has been excited with time-separated oscillatory fields and Ramsey fringes were observed in the case of dipole and quadrupole excitation. The experimental resonances are in good agreement with theory. Further applications of the technique are discussed.

Nuclear and High Energy PhysicsChemistryMass spectrometryPenning trapDipoleQuadrupolePhysics::Atomic PhysicsIon trapDetectors and Experimental TechniquesAtomic physicsQuadrupole ion trapInstrumentationQuadrupole mass analyzerHybrid mass spectrometerNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The squeezer ion guide

1992

Abstract The properties of an ordinary ion guide can be improved by inserting a grid between the nozzle and the skimmer. When positive ions are transported, an electric potential lower than +10 V is connected to the grid and one of the order of − 10 V to the skimmer. Efficient focusing is achieved between the nozzle and the grid by a combined action of the viscous helium flow field and the weak electric field. The focusing device is called a “squeezer”. It can be extended by adding more grids, a second skimmer, and differential pumping. Contrary to the first grid, the additional elements act more or less like electrostatic lenses in medium vacuum. With the squeezer ion guide, ions created i…

Nuclear and High Energy PhysicsChemistryNozzleUltra-high vacuumSkimmer (machine)Electric potentialAtomic physicsInstrumentationQuadrupole mass analyzerElectrostatic lensIonElectric discharge in gasesNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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