Search results for "scattering [nucleus nucleus]"

showing 10 items of 161 documents

Coulomb breakup of 23O

2005

Abstract The ground-state structure of the near-drip-line nucleus 23O has been investigated in a one-neutron Coulomb breakup reaction. Differential cross sections d σ / d E * for electromagnetic excitation of 23O projectiles (422 MeV/nucleon) incident on a lead target have been obtained from the measurement of the momenta of all breakup products including γ rays. The analysis of the deduced dipole-transition probability into the continuum infers a 2 s 1 / 2 ⊗ O 22 ( 0 + ) ground state configuration with a spectroscopic factor of 0.77(10) and thus a ground-state spin I π ( O 23 ) = 1 / 2 + , resolving earlier conflicting experimental findings. Final-state interaction is of significant influe…

PhysicsNuclear and High Energy PhysicsNuclear TheoryCoulombScattering lengthNeutron scatteringAtomic physicsNuclear ExperimentNucleonGround stateBreakupExcitationSpin-½Physics Letters B
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ΛNNandΣNNsystems at threshold

2007

We calculate the hypertriton binding energy and the $\ensuremath{\Lambda}d$ and $\ensuremath{\Sigma}d$ scattering lengths using baryon-baryon interactions obtained from a chiral constituent quark model. We study consistently the $\ensuremath{\Lambda}\mathit{NN}$ and $\ensuremath{\Sigma}\mathit{NN}$ systems by analyzing the effect of the $\ensuremath{\Sigma}\ensuremath{\leftrightarrow}\ensuremath{\Lambda}$ conversion. Our interactions correctly predict the hypertriton binding energy. The $(I,J)=(0,3/2)$ $\ensuremath{\Lambda}\mathit{NN}$ channel is also attractive and it might have a bound state. From the condition of nonexistence of a (0,3/2) $\ensuremath{\Lambda}\mathit{NN}$ bound state, an…

PhysicsNuclear and High Energy PhysicsParticle physicsBound stateQuark modelHyperonScattering lengthFew-body systemsLambdaHypertritonSpin-½Physical Review C
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Measurement of the integrated luminosities of the data taken by BESIII at √ s = 3.650 and 3.773 GeV

2013

Data sets were collected with the BESIII detector at the BEPC II collider at the center-of-mass energy of root s=3.650 GeV during May 2009 and at root s=3.773 GeV from January 2010 to May 2011. By analyzing the large angle Bhabha scattering events, the integrated luminosities of the two data sets are measured to be (44.49 +/- 0.02 +/- 0.44) pb(-1) and (2916.94 +/- 0.18 +/- 29.17) pb(-1), respectively, where the first error is statistical and the second error is systematic.

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)ScatteringDetectorPOTENTIALSVECTORAstronomy and AstrophysicsBhabha Scattering EventsCross SectionUPPER-BOUNDSlaw.inventionNuclear physicsIntegrated LuminositylawKLEIN-GORDON EQUATIONColliderInstrumentationBhabha scatteringChinese Physics C
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Photoproduction of theωmeson on the proton near threshold

2015

An experimental study of omega photoproduction on the proton was conducted by using the Crystal Ball and TAPS multiphoton spectrometers together with the photon tagging facility at the Mainz Microtron MAMI. The gamma p -> omega p differential cross sections are measured from threshold to the incident-photon energy E-gamma = 1.40 GeV (W = 1.87 GeV for the center-of-mass energy) with 15-MeV binning in E-gamma and full production-angle coverage. The quality of the present data near threshold gives access to a variety of interesting physics aspects. As an example, an estimation of the omega N scattering length alpha(omega p) is provided.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonProtonMesonVector meson dominanceScattering length7. Clean energyOmegaNuclear physicsNuclear ExperimentMicrotronCrystal BallPhysical Review C
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Angular and polarization dependence of Compton scattering from in the Δ-resonance region

1998

Abstract Using linearly polarized tagged photons from coherent bremsstrahlung, differential cross sections and beam asymmetries for Compton scattering by 4 He have been measured at MAMI in the energy interval between 150 MeV and 500 MeV for scattering angles of θ γ lab =37°, 93° and 137°, thus largely increasing the available data base. Improved calculations in terms of the Δ -hole model completely fail to describe the data at large scattering angles. The same proved to be true for a schematic model, even after taking into account properties of nuclear photo-absorption in very detail.

PhysicsNuclear and High Energy PhysicsPhoton010308 nuclear & particles physicsScatteringCompton scatteringScattering lengthInelastic scatteringMott scattering01 natural sciencesSmall-angle neutron scatteringNuclear physicsX-ray Raman scattering0103 physical sciencesNuclear Experiment010306 general physicsPhysics Letters B
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Characterization of alpha sources by Rutherford backscattering spectrometry

1996

Radioactive sources for alpha spectrometry are usually prepared by electrodeposition onto stainless steel backings (and sometimes heated). In earlier work, using the conventional method with passivated implanted planar silicon detectors for the measurements, several sources had been characterized in terms of various parameters by fitting the data of each spectrum to a certain mathematical function. In the present work, the Rutherford Backscattering Spectrometry (RBS) technique with a 1.6 MeV He+ beam was used to study the influence of those factors on the surface distribution and depth profiles of the thin radionuclide layers. Simulations of the measurements using the RUMP computer code wer…

PhysicsNuclear and High Energy PhysicsPlanarSiliconchemistryAlpha spectrometryDetectorchemistry.chemical_elementAtomic physicsRutherford backscattering spectrometryInstrumentationBeam (structure)Characterization (materials science)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Study of meson production in nuclei near threshold

2009

We present a study of the η production at low energies in pd collision with 3He and pd nuclear systems in the final state. The η production mechanism is described by a two-step model and the final state interactions are included fully. The η - d and η - 3He final state interactions are incorporated through the solution of the Lippmann Schwinger equation for a half off-shell η - AT-matrix. For η - d this t -matrix is written in a factorized form, with an off-shell form factor multiplying an on-shell part having the scattering length representation. The p - d final state interaction is included by multiplying the production matrix element by the inverse of the Jost function which includes th…

PhysicsNuclear and High Energy PhysicsRank (linear algebra)Quantum mechanicsCoulombForm factor (quantum field theory)General Physics and AstronomyInverseScattering lengthProduction (computer science)State (functional analysis)Atomic physicsLippmann–Schwinger equation
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Study of internal structures of 9,10Be and 10B in scattering of 4He from 9Be

2013

A study of inelastic scattering and single-particle transfer reactions was performed by an alpha beam at 63 MeV on a 9$Be target. Angular distributions of the differential cross sections for the 9Be(4He,4He')9Be*, 9Be(4He,3He)10Be and 9Be(4He,t)10B reactions were measured. Experimental angular distributions of the differential cross sections for the ground state and a few low-lying states were analyzed in the framework of the optical model, coupled channels and distorted-wave Born approximation. An analysis of the obtained spectroscopic factors was performed.

PhysicsNuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryScatteringFOS: Physical sciencesDWBAScattering length[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Inelastic scatteringAlpha (navigation)Nuclear Theory (nucl-th)Angular distributiondifferential cross sectionoptical modelangular distribution25.55.Ci; 24.10.Eq; 27.20.+n; 25.55.hp; 21.10.Pc; 24.10.TtNuclear cross sectioninelatic scatteringNuclear Experiment (nucl-ex)Atomic physicsBorn approximationNuclear ExperimentBeam (structure)
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ΛNNandΣNNsystems at threshold. II. The effect ofDwaves

2007

Using the two-body interactions obtained from a chiral constituent quark model, we study allN N andN N states with I = 0, 1, 2a ndJ = 1/2, 3/2 at threshold, taking into account all three-body configurations with S and D wave components. We constrain further the limits for theN spin-triplet scattering length a1/2,1 .U sing the hypertriton binding energy, we find a narrow interval for the possible values of theN spin-singlet scattering length a1/2,0. We find that theN N system has a quasibound state in the (I,J ) = (1, 1/2) channel very near threshold with a width of about 2.1 MeV.

PhysicsNuclear physicsNuclear and High Energy PhysicsQuark modelConstituent quarkScattering lengthFew-body systemsNucleonLambda baryonLambdaHypertritonPhysical Review C
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EXTRACTION OF ΛΛ SCATTERING LENGTH

2009

We determine ΛΛ scattering parameters from a ΛΛ invariant mass spectrum that was obtained by 12 C (K-, K+ΛΛ) reaction at the KEK Proton Synchrotron. In the framework of Watson's procedure, the obtained scattering length [Formula: see text] and effective range [Formula: see text] are most consistent with the values predicted by using the Nijmegen soft core models (NSC97's). However, the predicted values by using the Nijmegen hard-core ND ( G -matrix) and the extended soft-core (ESC00) models are out of two standard deviations from the determined scattering parameters.

PhysicsNuclear physicsNuclear and High Energy PhysicsRange (particle radiation)Soft coreExtraction (chemistry)Scattering parametersGeneral Physics and AstronomyProton SynchrotronInvariant massScattering lengthLambdaStandard deviationInternational Journal of Modern Physics E
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