Search results for "Cross Section"

showing 10 items of 3111 documents

The nucleon axial mass and the MiniBooNE quasielastic neutrino-nucleus scattering problem

2011

The charged-current double differential neutrino cross section, measured by the MiniBooNE Collaboration, has been analyzed using a microscopical model that accounts for, among other nuclear effects, long range nuclear (RPA) correlations and multinucleon scattering. We find that MiniBooNE data are fully compatible with the world average of the nucleon axial mass in contrast with several previous analyses which have suggested an anomalously large value. We also discuss the reliability of the algorithm used to estimate the neutrino energy.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsNuclear Theory010308 nuclear & particles physicsScatteringNuclear TheoryFOS: Physical sciencesFísica01 natural sciencesMiniBooNENuclear physicsNuclear Theory (nucl-th)Cross section (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsNucleonRandom phase approximationCharged current
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Search for particles decaying into a Z boson and a photon in pp¯ collisions at s=1.96 TeV

2006

Abstract We present the results of a search for a new particle X produced in p p ¯ collisions at s = 1.96 TeV and subsequently decaying to Zγ. The search uses 0.3 fb−1 of data collected with the DO detector at the Fermilab Tevatron Collider. We set limits on the production cross section times the branching fraction σ ( p p ¯ → X ) × B ( X → Z γ ) that range from 0.4 to 3.5 pb at the 95% C.L. for X with invariant masses between 100 and 1000 GeV / c 2 , over a wide range of X decay widths.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsPhoton010308 nuclear & particles physicsBranching fractionTevatron7. Clean energy01 natural scienceslaw.inventionCross section (physics)law0103 physical sciencesHigh Energy Physics::ExperimentFermilabInvariant (mathematics)010306 general physicsColliderPhysics Letters B
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Initial-state radiation measurement of thee+e−→π+π−π+π−cross section

2012

We study the process e+e- -> pi+pi-pi+pi-gamma, with a photon emitted from the initial-state electron or positron, using 454.3 fb^-1 of data collected with the BABAR detector at SLAC, corresponding to approximately 260,000 signal events. We use these data to extract the non-radiative sigma(e+e- ->pi+pi-pi+pi-) cross section in the energy range from 0.6 to 4.5 Gev. The total uncertainty of the cross section measurement in the peak region is less than 3%, higher in precision than the corresponding results obtained from energy scan data.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Photon010308 nuclear & particles physicsDetectorElectron01 natural sciencesNuclear physicsCross section (physics)Positron0103 physical sciencesPiHigh Energy Physics::ExperimentAtomic physics010306 general physicsEnergy (signal processing)Physical Review D
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Determination of the total photo-absorption cross section of 197Au from () reaction cross sections

1984

Abstract Cross sections for the reactions 197Au ( γ, ℩ n ) (x ⩽ 12) have been measured for bremsstrahlung end-point energies in the range 60–340 MeV. From these dominant cross sections, the total photon absorption cross section is determined using a cascade-evaporation calculation to account for the missing reaction channels. The enhancement factor for the classical E1 sum rule is found to be 0.93 ± 0.10.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)PhotonBremsstrahlungAbsorption cross sectionNuclear cross sectionSum rule in quantum mechanicsAtomic physicsPhysics Letters B
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Coherent γ-production in (p,p′) reactions in nuclei in the Δ resonance region

1998

Abstract We study the process of coherent photon production in nuclei induced by the (p,p′) reaction around the Δ excitation region. The cross sections are about 200 times smaller than the corresponding ones for coherent pion production but within measurable range with present machines. The cross section selects the transverse part of the NN→NΔ transition, while coherent pion production selects the longitudinal one. The reactions are complementary and show different aspects of Δh propagation through the nucleus which are discussed here.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)PhotonNuclear TheoryResonance (particle physics)Cross section (geometry)Transverse planemedicine.anatomical_structurePionmedicineAtomic physicsNuclear ExperimentNucleusExcitationPhysics Letters B
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Total photofission cross section for 238U as a substitute for the photon absorption cross section in the energy range of the first baryon resonances

1992

Abstract The total photofission cross section σγ, F for 238U has been measured as a substitute for the total photon absorption cross section σtot in the energy range of the first baryon resonances (50⩽Eγ⩽800 MeV). The experiments were performed at the tagging facility of the new 855 MeV Mainz Microton MAMI B using monochromatic photons and a sophisticated 4π-arrangement of position sensitive fragment detectors. The measured cross section agrees in the Δ-resonance region with previous results and the so-called universal curve αtot/A. In the energy region of the D13-resonance near 710 MeV resonancelike structure could be observed as is seen for the free proton.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)PhotonProtonNuclear TheoryPhotofissionAbsorption cross sectionNuclear physicsBaryonCross section (physics)Monochromatic colorAtomic physicsNuclear ExperimentPhysics Letters B
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Zu notwendigen Resonanzkriterien im station�ren Einkanal-Fall

1975

First will be exhibited, for the stationary case, a connection between the probability, to find a particle in the region of interaction, and the derivative of the scattering phase shift for the momentum. From the idea, that in stationary scattering a resonance is linked with an appreciable increase of this probability, one obtains new and quantitative criteria for the behavior ofδl(k). For instance, the nonresonant behavior can be characterised by the condition 2kdδl(k)/dk<1. The maximum of probability for the particle to be in the region of interaction, is considered in accordance with the criterium of maximal change of the phase shift, as a function ofk. This characterises the location of…

PhysicsNuclear and High Energy PhysicsScatteringbusiness.industryDerivativeFunction (mathematics)CollisionResonance (particle physics)Connection (mathematics)MomentumCross section (physics)OpticsQuantum mechanicsbusinessZeitschrift f�r Physik A Atoms and Nuclei
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MONSTER: a TOF Spectrometer for beta-delayed Neutron Spectroscopy

2014

β-delayed neutron (DN) data, including emission probabilities, Pn, and energy spectrum, play an important role in our understanding of nuclear structure, nuclear astrophysics and nuclear technologies. A MOdular Neutron time-of-flight SpectromeTER (MONSTER) is being built for the measurement of the neutron energy spectra and branching ratios. The TOF spectrometer will consist of one hundred liquid scintillator cells covering a significant solid angle. The MONSTER design has been optimized by using Monte Carlo (MC) techniques. The response function of the MONSTER cell has been characterized with mono-energetic neutron beams and compared to dedicated MC simulations.

PhysicsNuclear and High Energy PhysicsSpectrometerta114Nuclear TheoryNeutron stimulated emission computed tomographyNeutron scatteringNeutron temperatureNeutron time-of-flight scatteringNeutron spectroscopyNuclear physicsNeutron cross sectionNeutronNuclear ExperimentNuclear Data Sheets
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Thermal neutron capture cross section of the radioactive isotopeFe60

2015

Background: Fifty percent of the heavy element abundances are produced via slow neutron capture reactions in different stellar scenarios. The underlying nucleosynthesis models need the input of neutron capture cross sections.Purpose: One of the fundamental signatures for active nucleosynthesis in our galaxy is the observation of long-lived radioactive isotopes, such as $^{60}\mathrm{Fe}$ with a half-life of $2.60\ifmmode\times\else\texttimes\fi{}{10}^{6}$ yr. To reproduce this $\ensuremath{\gamma}$ activity in the universe, the nucleosynthesis of $^{60}\mathrm{Fe}$ has to be understood reliably.Methods: An $^{60}\mathrm{Fe}$ sample produced at the Paul Scherrer Institut (Villigen, Switzerla…

PhysicsNuclear and High Energy PhysicsThermal neutron captureResonance7. Clean energyGalaxyNuclear physicsNeutron captureCross section (physics)13. Climate actionNucleosynthesisAtomic physicss-processEnergy (signal processing)Physical Review C
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Measurement of the t-channel single top-quark production cross section in pp collisions at s=7 TeV with the ATLAS detector

2012

We report a measurement of the cross section of single top-quark production in the t-channel using 1.04 fb -1 of pp collision data at s=7 TeV recorded with the ATLAS detector at the LHC. Selected e ...

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron ColliderChannel (digital image)Physics::Instrumentation and Detectors010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixAtlas detectorHigh Energy Physics::Phenomenology01 natural sciencesCross section (physics)medicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineHigh Energy Physics::ExperimentProduction (computer science)010306 general physicsPhysics Letters B
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