Search results for "PARTICLES"

showing 10 items of 8085 documents

Compton Scattering from the Deuteron below Pion-Production Threshold

2015

Differential cross sections for elastic scattering of photons from the deuteron have recently been measured at the Tagged-Photon Facility at the MAX IV Laboratory in Lund, Sweden. These first new measurements in more than a decade further constrain the isoscalar electromagnetic polarizabilities of the nucleon and provide the first-ever results above 100 MeV, where the sensitivity to the polarizabilities is increased. We add 23 points between 70 and 112 MeV, at angles 60deg, 120deg and 150deg. Analysis of these data using a Chiral Effective Field Theory indicates that the cross sections are both self-consistent and consistent with previous measurements. Extracted values of \alpha_s = [12.1 +…

Elastic scatteringNuclear reactionPhysicsNuclear and High Energy PhysicsPhoton010308 nuclear & particles physicsScatteringIsoscalarCompton scatteringFOS: Physical sciences01 natural sciences3. Good healthNuclear physicsPion0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear Experiment
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New Measurements of the Transverse Beam Asymmetry for Elastic Electron Scattering from Selected Nuclei

2012

We have measured the beam-normal single-spin asymmetry $A_n$ in the elastic scattering of 1-3 GeV transversely polarized electrons from $^1$H and for the first time from $^4$He, $^{12}$C, and $^{208}$Pb. For $^1$H, $^4$He and $^{12}$C, the measurements are in agreement with calculations that relate $A_n$ to the imaginary part of the two-photon exchange amplitude including inelastic intermediate states. Surprisingly, the $^{208}$Pb result is significantly smaller than the corresponding prediction using the same formalism. These results suggest that a systematic set of new $A_n$ measurements might emerge as a new and sensitive probe of the structure of heavy nuclei.

Elastic scatteringPhysics010308 nuclear & particles physicsScatteringmedia_common.quotation_subjectFOS: Physical sciencesGeneral Physics and AstronomyElastic electronchemistry.chemical_elementElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesAsymmetryAmplitudechemistryExcited state0103 physical sciencesNuclear Experiment (nucl-ex)Atomic physics010306 general physicsNuclear ExperimentNuclear ExperimentHeliummedia_common
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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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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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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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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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Backward spin polarizabilityγπof the proton

2002

Using the Mainz $48\mathrm{cm}\ensuremath{\emptyset}\ifmmode\times\else\texttimes\fi{}64\mathrm{cm}$ NaI(Tl) detector and the segmented G\"ottingen recoil detector SENECA in coincidence, Compton scattering by the proton at ${\ensuremath{\theta}}_{\ensuremath{\gamma}}^{\mathrm{lab}}=136\ifmmode^\circ\else\textdegree\fi{}$ has been measured at MAMI (Mainz) in the energy range from 200 to 470 MeV. The new data confirm the previous observation that there is a systematic discrepancy between MAMI and LEGS (Brookhaven) data leading to different spin polarizabilities ${\ensuremath{\gamma}}_{\ensuremath{\pi}}=\ensuremath{-}38.7\ifmmode\pm\else\textpm\fi{}1.8$ and $\ensuremath{-}27.2\ifmmode\pm\else\…

Elastic scatteringPhysicsNuclear and High Energy PhysicsParticle physicsProton010308 nuclear & particles physicsHadronElementary particle01 natural sciencesOrientation (vector space)Nuclear physicsBaryon0103 physical sciences010306 general physicsNucleonEnergy (signal processing)Physical Review C
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Clusterization and strong coupled-channels effects in deuteron interaction with $^9$Be nuclei

2019

Angular distributions of protons, deuterons, tritons and alpha particles emitted in the d + alt;supagt;9alt;/supagt;Be reaction at Ealt;subagt;labalt;/subagt;=19.5 and 35.0 MeV have been measured.a#13; The elastic scattering channel is analysed in the framework of both the Optical Model and the Coupled-Channel approach. a#13; The interaction potential of the alt;iagt;dalt;/iagt; + alt;supagt;9alt;/supagt;Be system is calculated in the framework of the Double-Folding model using the α+α+alt;iagt;nalt;/iagt; three-body wave function of the alt;supagt;9alt;/supagt;Be nucleus.a#13; The (alt;iagt;dalt;/iagt;,alt;iagt;palt;/iagt;) and (alt;iagt;dalt;/iagt;,alt;iagt;talt;/iagt;) one-nucleon-transf…

Elastic scatteringPhysicsNuclear and High Energy Physicselastic and inelastic scattering010308 nuclear & particles physicsNuclear TheoryAnalytical chemistryDWBAAlpha particleDALT[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]spectroscopic amplitudes01 natural sciencescluster structureCRCdouble foldingInteraction potentialDeuterium0103 physical sciencesoptical model010306 general physicsWave functionNuclear Experiment
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