Search results for "solution"

showing 10 items of 5638 documents

Time-of-flight photoelectron emission microscopy TOF-PEEM: first results

1998

The time structure of the synchrotron radiation at BESSY (Berlin) is used to operate a photoemission electron microscope in a time-of-flight (TOF) mode. The electrons which are emitted from the sample surface with different energies are dispersed in a drift tube subsequent to the imaging optics. The screen of the microscope was replaced by a fast scintillator (tau = 1.4 ns) and the light is detected by an ultra fast gated intensified CCD camera (800 ps gate 1 MHz repetition rate). The resolving power in the energy domain is demonstrated and possible implications on the spatial resolution (chromatic correction) are discussed. Additionally, an improved contrast at very low emission energies i…

PhysicsNuclear and High Energy PhysicsMicroscopebusiness.industryPhysics::Instrumentation and DetectorsSynchrotron radiationElectronScintillatorlaw.inventionTime of flightOpticslawChromatic scaleElectron microscopebusinessInstrumentationImage resolution
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Three-Body Coulomb Final-State Interaction Effects in the Coulomb Breakup of Light Nuclei

2005

Coulomb breakup of a projectile in the Coulomb field of a fully stripped heavy nucleus is at present one of the most popular experimental methods to obtain information on reactions of interest in nuclear astrophysics. Its theoretical interpretation presents, however, considerable difficulties, due to the three-body nature and the infinite range of the Coulomb forces involved. Among the uncertainties affecting present analyses, the possible modification of the dissociation cross section by three-body Coulomb final-state interactions plays a major role. Various methods which have been proposed to deal with it are briefly reviewed. However, none of them is based on a consistent and mathematica…

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsProjectileGeneral Physics and AstronomyFOS: Physical sciencesAstronomy and AstrophysicsBreakup01 natural sciences3. Good healthNuclear Theory (nucl-th)Wave–particle dualityAmplitudeExact solutions in general relativityClassical mechanics0103 physical sciencesNuclear astrophysicsCoulomb010306 general physicsQuantum
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Improved W boson mass measurement with the DO detector

2002

We have measured the W boson mass using the DO detector and a data sample of 82 pb(-1) from the Fermilab Tevatron collider. This measurement uses W-->enu decays, where the electron is close to a boundary of a central electromagnetic calorimeter module. Such "edge" electrons have not been used in any previous DO analysis, and represent a 14% increase in the W boson sample size. For these electrons, new response and resolution parameters are determined, and revised backgrounds and underlying event energy flow measurements are made. When the current measurement is combined with previous DO W boson mass measurements, we obtain M-W=80.483+/-0.084 GeV. The 8% improvement from the previous DO meas…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDetectorResolution (electron density)TevatronElectron7. Clean energy01 natural scienceslaw.inventionNuclear physicslawEnergy flowExperimental High Energy Physics0103 physical sciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentFermilab010306 general physicsColliderBosonPHYSICAL REVIEW D
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Production of the charmed baryon $\Lambda_{c}^{+}$ in $\pi^{-}$Cu and K$^{-}$Cu interactions at 230 GeV

1990

Abstract We present results from the NA32 experiment at CERN on the production characteristics of the charmed baryon Λ+c in 230 GeV π−Cu and K−Cu interactions. A high resolution vertex detector consisting of change-coupled devices and silicon microstrip detectors allowed the selection of a very clean sample of 154 Λ+c → pK−π+ (and charge conjugate) decays. Results on differential and integrated cross sections are given.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsResolution (electron density)chemistry.chemical_elementCharge (physics)CopperBaryonNuclear physicschemistryHigh Energy Physics::ExperimentProduction (computer science)Vertex detectorNuclear ExperimentSilicon microstrip detectorsParticle Physics - Experiment
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IS ALR SUGGESTING A LEFT–RIGHT SYMMETRIC SOLUTION?

1996

The implications of the recent measurement of the left–right asymmetry ALR by the SLD collaboration for the left–right symmetric theory are examined. We show that it is possible to arrange for a large, negative value of S, without serious side effects for other observables within this model. We also consider a restricted model with specified Higgs structure, where limits on MZ2 can be obtained.

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectStructure (category theory)General Physics and AstronomyAstronomy and AstrophysicsObservableAsymmetryNuclear physicsHiggs bosonSymmetric solutionValue (mathematics)media_commonModern Physics Letters A
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UTSW Small Animal Positron Emission Imager

2006

A Small Animal Imager (SAI) for PET has been designed, built, tested in phantoms, and applied to investigations in mice and rats. The device uses principles based on gamma-ray induced scintillation in crossed fiber optic detectors connected to Position Sensitive Photomultiplier Tubes (PSPMT). Each detector consists of an epoxied stack of 28 layers of 135 round 1 mm BCF-10 scintillating plastic fibers. The overlap region forms a 13.5times13.5times2.8 cm3 detector volume. Scintillating light from the fibers is detected by two (X and Y directions) Hamamatsu R-2486 PSPMTs with 16 anode wires in each of two orthogonal directions. A centroid-finding algorithm gives the position of a light cluster…

PhysicsNuclear and High Energy PhysicsPhotomultiplierScintillationOptical fiberPhotonbusiness.industryDetectorIterative reconstructionPhotocathodelaw.inventionOpticsNuclear Energy and EngineeringlawElectrical and Electronic EngineeringbusinessImage resolutionIEEE Transactions on Nuclear Science
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Plastic Scintillation Detectors for Time-of-Flight Mass Measurements

2020

Fast timing detectors are an essential element in the experimental setup for time-of-flight (ToF) mass measurements of unstable nuclei. We have upgraded the scintillator detectors used in experiments at the National Superconducting Cyclotron Laboratory (NSCL) by increasing the number of photomultiplier tubes that read out their light signals to four per detector, and characterized them in a test experiment with $^{48}$Ca beam at the NSCL. The new detectors achieved a time resolution ($\sigma$) of 7.5 ps. We systematically investigated different factors that affect their timing performance. In addition, we evaluated the ability of positioning the hitting points on the scintillator using the …

PhysicsNuclear and High Energy PhysicsPhotomultiplierScintillationPhysics - Instrumentation and DetectorsResolution (mass spectrometry)010308 nuclear & particles physicsbusiness.industryPhysics::Instrumentation and DetectorsDetectorFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)Scintillator01 natural sciencesTime of flightOpticsSuperconducting cyclotron0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsbusinessInstrumentationNuclear ExperimentBeam (structure)
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A scintillator based time-of-flight hodoscope with a new type of emitter follower divider

2004

A high precision, time-of-flight hodoscope has been constructed to analyse the secondary pion beam at GSI, Darmstadt. The hodoscope comprises three scintillator planes with the individual scintillator rods read out by photomultipliers in both ends. A new active base of the emitter follower type has been developed for stabilization of voltages at the last dynodes of the photomultiplier. The time resolution of this system was found to be sigma less than or equal to 150 ps for counting rates up to 2 MHz.

PhysicsNuclear and High Energy PhysicsPhotomultiplierbusiness.industryPhysics::Instrumentation and Detectors25.80.Ls; 29.70.Eg; 25.75.Dw; 29.27.-tCommon collectorTime resolutionScintillatorRodTime of flightOpticsTime-of-flight measurementsHodoscopePhysics::Accelerator Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]businessNuclear ExperimentInstrumentationVoltage
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K+Λ and K+Σ0 photoproduction with fine center-of-mass energy resolution

2014

Measurements of γp→K+Λγp→K+Λ and γp→K+Σ0γp→K+Σ0 cross-sections have been obtained with the photon tagging facility and the Crystal Ball calorimeter at MAMI-C. The measurement uses a novel K+K+ meson identification technique in which the weak decay products are characterized using the energy and timing characteristics of the energy deposit in the calorimeter, a method that has the potential to be applied at many other facilities. The fine center-of-mass energy (W) resolution and statistical accuracy of the new data results in a significant impact on partial wave analyses aiming to better establish the excitation spectrum of the nucleon. The new analyses disfavor a strong role for quark–diqua…

PhysicsNuclear and High Energy PhysicsPhotonMesonResolution (electron density)7. Clean energyCalorimeterNuclear physicsHigh Energy Physics::ExperimentCenter of massAtomic physicsNucleonExcitationCrystal BallPhysics Letters B
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Response of BGO detectors to photons of 3–50 MeV energy

1993

Abstract The response of an array of 7 hexagonal BGO detectors each 7.5 cm long (6.7 radiation lengths) with 3.6 cm side-to-side distance was measured using monochromatic photons from the tagged-photon facility at the electron accelerator MAMI A at Mainz. The experimental spectra of the deposited energy for a single detector and for the array of seven modules compare very well with the predictions of Monte Carlo shower simulations using the code GEANT3. Significant improvement of the energy resolution is observed for the summed energy spectra compared to the resolution of a single module. This improvement deteriorates at higher photon energies because the length of the detector is not suffi…

PhysicsNuclear and High Energy PhysicsPhotonPhysics::Instrumentation and Detectorsbusiness.industryMonte Carlo methodResolution (electron density)DetectorParticle acceleratorRadiationSpectral linelaw.inventionNuclear physicsOpticslawMonochromatic colorbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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