Search results for " high energy physics"

showing 10 items of 8412 documents

Pygmy dipole resonance in 124Sn populated by inelastic scattering of 17O

2014

L. Pellegri et al. ; 5 pags. ; 6 figs. ; open access article under the CC BY license. Funded by SCOAP3

Elastic scatteringPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaIsoscalarGamma rayInelastic scattering01 natural sciences7. Clean energyResonance (particle physics)lcsh:QC1-999Isospin characterLow-lying electric dipole excitationsIonNuclear physicsDipoleLow-lying electric dipole excitations 124Sn0103 physical sciencesAGATAAtomic physics010306 general physics124Snlcsh:PhysicsPhysics Letters B
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Estimating the two-particle $K$-matrix for multiple partial waves and decay channels from finite-volume energies

2017

An implementation of estimating the two-to-two $K$-matrix from finite-volume energies based on the L\"uscher formalism and involving a Hermitian matrix known as the "box matrix" is described. The method includes higher partial waves and multiple decay channels. Two fitting procedures for estimating the $K$-matrix parameters, which properly incorporate all statistical covariances, are discussed. Formulas and software for handling total spins up to $S=2$ and orbital angular momenta up to $L=6$ are obtained for total momenta in several directions. First tests involving $\rho$-meson decay to two pions include the $L=3$ and $L=5$ partial waves, and the contributions from these higher waves are f…

Elastic scatteringPhysicsNuclear and High Energy PhysicsAngular momentumFinite volume methodSpins010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Elastic energyhep-latFOS: Physical sciencesCovariance01 natural sciencesHermitian matrixHigh Energy Physics - LatticeClassical mechanicsPionQuantum electrodynamics0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physics
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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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Compton scattering by a pion and off-shell effects

1994

We consider Compton scattering by a pion in the framework of chiral perturbation theory. We investigate off--shell effects in the s-- and u--channel pole diagrams. For that purpose we perform a field transformation which, in comparison with the standard Gasser and Leutwyler Lagrangian, generates additional terms at order $p^4$ proportional to the lowest--order equation of motion. As a result of the equivalence theorem the two Lagrangians predict the same Compton scattering S--matrix even though they generate different off--shell form factors. We conclude that off--shell effects are not only model--dependent but also representation--dependent.

Elastic scatteringPhysicsNuclear and High Energy PhysicsChiral perturbation theoryNuclear Theory010308 nuclear & particles physicsScatteringHigh Energy Physics::LatticeComputer Science::Information RetrievalCompton scatteringFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)Scattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionQuantum electrodynamics0103 physical sciencesPerturbation theory010306 general physicsS-matrixPhysical Review C
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Doubling of α-cluster statesin22Ne

2001

Excitation functions for ${}^{18}\mathrm{O}+\ensuremath{\alpha}$ elastic scattering were measured by a method using inverse kinematics and a thick gas target. An analysis of the data corresponding to the excitation energy regions of 11.8--13.7 MeV and 19.0--22.0 MeV in ${}^{22}\mathrm{Ne}$ was carried out. A surprising splitting of ${1}^{\ensuremath{-}},$ ${3}^{\ensuremath{-}},$ ${7}^{\ensuremath{-}},$ and ${9}^{\ensuremath{-}}$ $\ensuremath{\alpha}$-cluster levels into doublets was found in ${}^{22}\mathrm{Ne}.$

Elastic scatteringPhysicsNuclear and High Energy PhysicsCluster (physics)Astrophysics::Cosmology and Extragalactic AstrophysicsAtomic physicsEnergy (signal processing)ExcitationPhysical Review C
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Study of Cluster Structures in Nuclei through the Ratio Method. A Tribute to Mahir Hussein

2020

For one-neutron halo nuclei, the cross sections for elastic scattering and breakup at intermediate energy exhibit similar angular dependences. The Recoil Excitation and Breakup (REB) model of reactions elegantly explains this feature. It also leads to the idea of a new reaction observable to study the structure of loosely-bound nuclear systems: the Ratio. This observable consists of the ratio of angular distributions for different reaction channels, viz. elastic scattering and breakup, which cancels most of the dependence on the reaction mechanism; in particular it is insensitive to the choice of optical potentials that simulate the projectile-target interaction. This new observable is very…

Elastic scatteringPhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsHadronNuclear TheoryFOS: Physical sciencesObservableBreakup7. Clean energy01 natural sciencesMolecular physicsPhysique atomique et nucléaireNuclear Theory (nucl-th)Recoil0103 physical sciencesNuclear fusionNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentExcitationBeam (structure)
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Virtual Compton Scattering and Neutral Pion Electroproduction in the Resonance Region up to the Deep Inelastic Region at Backward Angles

2009

We have made the first measurements of the virtual Compton scattering (VCS) process via the H$(e,e'p)\gamma$ exclusive reaction in the nucleon resonance region, at backward angles. Results are presented for the $W$-dependence at fixed $Q^2=1$ GeV$^2$, and for the $Q^2$-dependence at fixed $W$ near 1.5 GeV. The VCS data show resonant structures in the first and second resonance regions. The observed $Q^2$-dependence is smooth. The measured ratio of H$(e,e'p)\gamma$ to H$(e,e'p)\pi^0$ cross sections emphasizes the different sensitivity of these two reactions to the various nucleon resonances. Finally, when compared to Real Compton Scattering (RCS) at high energy and large angles, our VCS data…

Elastic scatteringPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsScatteringCompton scatteringResonanceFOS: Physical sciencesInelastic scattering[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Deep inelastic scattering01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear Experiment
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Combined description of N-barN scattering and annihilation with a hadronic model.

1995

A model for the nucleon-antinucleon interaction is presented which is based on meson-baryon dynamics. The elastic part is the {ital G}-parity transform of the Bonn {ital NN} potential. Annihilation into two mesons is described in terms of microscopic baryon-exchange processes including all possible combinations of {pi},{eta},{rho},{omega},{ital a}{sub 0},{ital f}{sub 0},{ital a}{sub 1},{ital f}{sub 1},{ital a}{sub 2},{ital f}{sub 2},{ital K},{ital K}{sup *}. The remaining annihilation part is taken into account by a phenomenological energy- and state-independent optical potential of Gaussian form. The model enables a simultaneous description of nucleon-antinucleon scattering and annihilatio…

Elastic scatteringPhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationMesonScatteringComputer Science::Information RetrievalNuclear TheoryHadronG-parityBaryonNuclear ExperimentEnergy (signal processing)Physical review. C, Nuclear physics
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πNscattering in relativistic baryon chiral perturbation theory reexamined

2011

We have analyzed pion-nucleon scattering using the manifestly relativistic covariant framework of infrared regularization up to $\mathcal{O}({q}^{3})$ in the chiral expansion, where $q$ is a generic small momentum. We describe the low-energy phase shifts with a similar quality as previously achieved with heavy baryon chiral perturbation theory, $\sqrt{s}\ensuremath{\lesssim}1.14$ GeV. New values are provided for the $\mathcal{O}({q}^{2})$ and $\mathcal{O}({q}^{3})$ low-energy constants, which are compared with previous determinations. This is also the case for the scattering lengths and volumes. Finally, we have unitarized the previous amplitudes and as a result the energy range where data …

Elastic scatteringPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryUnitarityHeavy baryon chiral perturbation theory010308 nuclear & particles physicsScatteringHadronScattering length01 natural sciencesBaryon0103 physical sciencesNuclear Experiment010306 general physicsPhysical Review C
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Neutral-current atmospheric neutrino flux measurement using neutrino-proton elastic scattering in Super-Kamiokande

2003

Recent results show that atmospheric $\nu_\mu$ oscillate with $\delta m^2 \simeq 3 \times 10^{-3}$ eV$^2$ and $\sin^2{2\theta_{atm}} \simeq 1$, and that conversion into $\nu_e$ is strongly disfavored. The Super-Kamiokande (SK) collaboration, using a combination of three techniques, reports that their data favor $\nu_\mu \to \nu_\tau$ over $\nu_\mu \to \nu_{sterile}$. This distinction is extremely important for both four-neutrino models and cosmology. We propose that neutrino-proton elastic scattering ($\nu + p \to \nu + p$) in water \v{C}erenkov detectors can also distinguish between active and sterile oscillations. This was not previously recognized as a useful channel since only about 2% …

Elastic scatteringPhysicsNuclear and High Energy PhysicsParticle physicsNeutral currentProtonPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFOS: Physical sciencesParticle identificationHigh Energy Physics - ExperimentNuclear physicsMiniBooNEHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoNeutrino oscillationSuper-KamiokandePhysical Review D
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