0000000000480669

AUTHOR

S. Boffi

showing 4 related works from this author

Out-of-plane measurements of the fifth response function of the exclusive electronuclear response

1999

The first measurements of f{sub LT}{sup '}, known as the fifth response function, have been made for the {sup 2}H(e(vector sign),e{sup '}p) and {sup 12}C(e(vector sign),e{sup '}p) reactions. This response is directly related to the imaginary part of the interference between the transverse and longitudinal nuclear electromagnetic currents. Its observation requires longitudinally polarized electron beams and out-of-plane detection, the latter made possible by the newly developed out-of-plane spectrometer system. The initial measurements were made by using a 560-MeV polarized electron beam and quasielastic kinematics at Q{sup 2}=3.3 fm{sup -2}. The development of the methodology for out-of-pla…

PhysicsNuclear reactionNuclear and High Energy Physicsmedia_common.quotation_subjectNuclear structureElectronAsymmetryCoincidenceNuclear physicsTransverse planeCross section (physics)Atomic physicsSign (mathematics)media_commonPhysical Review C
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Comparison of Monte Carlo simulation and direct multistep scattering theory in (e,e′p) nuclear reactions

1999

Abstract Two methods to deal with final state interactions in (e,e′p) reactions in nuclei are compared. One of them uses a Monte Carlo semiclassical approach while the other uses a statistical quantum mechanical approach. The comparison serves to give support to both approaches, showing at the same time their limitations.

PhysicsHybrid Monte CarloNuclear and High Energy PhysicsQuantum Monte CarloMonte Carlo methodDynamic Monte Carlo methodMonte Carlo method in statistical physicsStatistical physicsScattering theoryKinetic Monte CarloMonte Carlo molecular modelingNuclear Physics A
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Measurement of the n-TOF beam profile with a micromegas detector

2004

A Micromegas detector was used in the neutron Time-Of-Flight (n_TOF) facility at CERN to evaluate the spatial distribution of the neutron beam as a function of its kinetic energy. This was achieved over a large range of neutron energies by using two complementary processes: at low energy by capture of a neutron via the 6Li(n,[alpha])t reaction, and at high energy by elastic scattering of neutrons on gas nuclei (argon+isobutane or helium+isobutane). Data are compared to Monte Carlo simulations and an analytic function fitting the beam profile has been calculated with a sufficient precision to use in neutron capture experiments at the n_TOF facility. http://www.sciencedirect.com/science/artic…

Elastic scatteringPhysicsNuclear and High Energy PhysicsArgonPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaBeam profileNuclear Theorychemistry.chemical_elementMicroMegas detectorNUCLEAR PHYSICSNeutron radiationNuclear physicsNeutron capturechemistryNEUTRON BEAMSNeutron cross sectionMICROMEGAS DETECTORNeutron detectionNeutron beam profilerNeutronNuclear ExperimentInstrumentationMicromegas
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On the NN-final-state-interaction in the $^{16}{O}(e,e' pp)$ reaction

2002

The influence of the mutual interaction between the two outgoing nucleons (NN-FSI) in the $^{16}{O}(e,e' pp)$ reaction has been investigated. Results for various kinematics are discussed. In general, the effect of NN-FSI depends on kinematics and the chosen final state in the excitation spectrum of $^{14}{C}$.

PhysicsNuclear and High Energy Physicsnucl-thNuclear TheorySpectrum (functional analysis)Nuclear TheoryFOS: Physical sciencesKinematicsState (functional analysis)Nuclear Theory (nucl-th)Atomic physicsNucleonNuclear ExperimentExcitation
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