Search results for "Virtual"

showing 10 items of 1485 documents

Pion-photon transition distribution amplitudes in the Nambu-Jona-Lasinio model

2007

12 pages, 6 figures.-- PACS nrs.: 13.60.-r; 11.10.St; 12.38.Lg; 24.10.Jv.-- ISI Article Identifier: 000251327200049.-- ArXiv pre-print available at: http://arxiv.org/abs/0707.3366

Nuclear and High Energy PhysicsPhotonBethe–Salpeter equationHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences[PACS] Relativistic models of nucleiPartícules (Física nuclear)PionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio modelBound stateVirtual Compton-scatteringCovariant transformation[PACS] Photon and charged-lepton interactions with hadrons[PACS] Bound and unstable statesMathematical physicsQuantum chromodynamicsPhysicsHigh Energy Physics::PhenomenologyGeneralized Parton distributions[PACS] Bound and unstable states; Bethe-Salpeter equations[PACS] Other nonperturbative calculations in QCDHigh Energy Physics - PhenomenologyAmplitudeQuantum electrodynamicsBethe-Salpeter equationsFísica nuclear
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Compton scattering off pions and electromagnetic polarizabilities

2019

The electric ($\alpha_\pi$) and magnetic ($\beta_\pi$) Compton polarizabilities of both the charged and the neutral pion are of fundamental interest in the low-energy sector of quantum chromodynamics (QCD). Pion polarizabilities affect the shape of the $\gamma\pi\to\gamma\pi$ Compton scattering angular distribution at back scattering angles and $\gamma\gamma\to\pi\pi$ absolute cross sections. Theory derivations are given of the $\gamma\pi\to\gamma\pi$ Compton scattering differential cross section, dispersion relations, and sum rules in terms of the polarizabilities. We review experimental charged and neutral polarizability studies and theoretical predictions. The $\pi^0$ polarizabilities we…

Nuclear and High Energy PhysicsPhotonChiral perturbation theoryNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesVirtual particle01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Pion0103 physical sciencesNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsCompton scatteringAstronomy and AstrophysicsAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentSum rule in quantum mechanicsCrystal BallInternational Journal of Modern Physics A
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Measurements of $R^{d}-R^{p}$ and $R^{Ca}-R^{C}$ in deep inelastic muon scattering

1992

Results are presented on the difference in R, the ratio of longitudinally to transversely polarised virtual photon absorption cross sections, for the deuteron and the proton. They are obtained by c ...

Nuclear and High Energy PhysicsProtonmuon nucleus: deep inelastic scatteringNuclear Theorypolarization: longitudinaldeep inelastic scattering: muon deuteronVirtual particlecross section: ratiophoton: absorptionElementary particlemuon deuteron: deep inelastic scattering530Nuclear physicsabsorption: photondeep inelastic scattering: muon ppolarization: transverseHIGH STATISTICS MEASUREMENT; R=SIGMA-L/SIGMA-T; HIGH Q2Nuclear ExperimentAbsorption (electromagnetic radiation)deep inelastic scattering: muon nucleus90: 200: 280 GeVPhysicsHIGH STATISTICS MEASUREMENTMuoncalciumScatteringcarbonstructure function: ratioR=SIGMA-L/SIGMA-TCERN SPSlongitudinal: polarizationParticle scatteringDeuteriummuon p: deep inelastic scatteringHIGH Q2Physics::Accelerator Physicstransverse: polarizationAtomic physicsParticle Physics - Experimentexperimental results
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Medium energy physics with c.w. electron accelerators

2008

Nuclear physicsAccelerator physicsTriple coincidencePhysicsMedium energylawVirtual particleElectronColliderlaw.invention
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Measurement of the proton and deuteron structure functions, F2p and F2d, and of the ratio

1997

The muon-proton and muon-deuteron inclusive deep inelastic scattering cross sections were measured in the kinematic range 0.002 < x < 0.60 and 0.5 < Q(2) < 75 GeV2 at incident muon energies of 90, 120, 200 and 280 GeV. These results are based on the full data set collected by the New Muon Collaboration, including the data taken with a small angle trigger. The extracted values of the structure functions F-2(p) and F-2(d) are in good agreement with those from other experiments. The data cover a sufficient range of y to allow the determination of the ratio of the longitudinally to transversely polarised virtual photon absorption cross sections, R = sigma(L)/sigma(T), for 0.002 < x < 0.12. The …

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsMuonProtonDeuteriumVirtual particlePerturbative QCDSigmaHigh Energy Physics::ExperimentDeep inelastic scatteringElectron scatteringNuclear Physics B
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The pion electroproduction and the virtual-photon theory

1983

The double differential cross-section for pion electroproduction was measured for the processes p(e,π+n and12C(e,π+)12B. The proton-induced cross-section was evaluated by using the virtual-photon concept. The experimental data were used to test different formulae for the virtual-photon spectrum. We found significant deviations to a generally used formula (Dalitz-Yennie) and good agreement with a new formula (Tiator-Wright). In addition, we have measured pion production crosssections with real photons under equal kinematic conditions. Electro-and photoproduction measurements give the same results.

Nuclear physicsPhysicsParticle physicsPionPhotonNuclear TheorySpectrum (functional analysis)Virtual particleHigh Energy Physics::ExperimentNuclear ExperimentIl Nuovo Cimento A
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Virtual Compton Scattering at MAMI γ*p→ γ1p1

1999

The virtual Compton scattering (VCS) is the electron scattering on a proton which radiates a real photon before being detected. The new observables, called Generalized Polarizabilities (GP), extracted from this VCS at threshold can be understood as the deformation of the charge and current distributions of the proton [1]. These GP are functions of the mass of the virtual photon Q2. In real Compton scattering (Q2 = 0), some polarizabilities of the nucleon are already measured [2]. With the VCS, we will generalize these observables by measuring them at different values of Q2.

Nuclear physicsPhysicsPhotonProtonCompton scatteringVirtual particleCharge (physics)ObservableNucleonElectron scattering
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The Experimental Program of the MAMI-Project

1992

At Mainz university, a 100% duty-factor electron accelerator for beam current and energy up to 100 µA and 855 MeV,respectively, has become operational recently, the Mainz Microtron MAMI. The experimental program is based on three major equipments which are built up and will be run by three facility-oriented collaborations. Collaboration A1 is centered around a magnetic spectrometer setup and will do experiments with virtual photons. For experiments with real photons collaboration A2 runs a high-efficiency tagger. Collaboration A3 sets up a polarized electron source in order to exploit the polarization degrees of freedom.

Nuclear physicsPhysicsPhotonSpectrometerlawDegrees of freedom (statistics)Virtual particleParticle acceleratorElectron sourceMicrotronBeam (structure)law.invention
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A time-of-flight facility for the measurement of electron-induced neutron spectra

1974

Abstract A time-of-flight facility is constructed to investigate photoneutrons in the energy range 5 MeV ≤ En ≤ 200 MeV. Photoneutrons are detected simultaneously at four angles (40.2°, 90°, 113.5°, 142.2°). The overall time resolution varies from 0.282 ns/m to 0.358 ns/m, depending on the different flight paths (18.56 m to 11.40 m). As a first check the facility is used to measure the ratio of the number of virtual photons to real photons via the photodisintegration of 2H. The measured values agree with the calculated photon spectra.

Nuclear physicsPhysicsRange (particle radiation)Time of flightPhotonPhotodisintegrationVirtual particleNeutron spectraGeneral MedicineElectronPhoton spectraNuclear Instruments and Methods
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Comprehensive Anatomic Assessment of Ipsilateral Pterional Versus Contralateral Subfrontal Approaches to the Internal Carotid Ophthalmic Segment: A C…

2019

Objective Medially pointing aneurysms of the ophthalmic segment of the internal carotid artery (oICA) represent a neurosurgical challenge. Conventional ipsilateral approaches require internal carotid artery and optic nerve (ON) mobilization as well as anterior clinoidectomy (AC), all associated with increased surgical risk. Contralateral approaches could provide a better exposure of the superomedial aspect of the oICA, ophthalmic artery, and superior hypophyseal artery, sparing AC and internal carotid artery or ON mobilization. However, the microsurgical anatomy of this approach has not been systematically studied. In the present work, we exhaustibly analyzed the anatomic and morphometric c…

Olfactory NerveSuperior Hypophyseal ArteryDissection (medical)Neurosurgical ProceduresOphthalmic Artery03 medical and health sciencesImaging Three-Dimensional0302 clinical medicinemedicine.arteryCadavermedicineHumansbusiness.industryVirtual RealityIntracranial AneurysmOptic NerveOrgan Sizemedicine.diseaseThree dimensional simulationFrontal lobe030220 oncology & carcinogenesisOphthalmic arteryOptic nerveSurgeryNeurology (clinical)Internal carotid arteryCadaveric spasmNuclear medicinebusinessCarotid Artery Internal030217 neurology & neurosurgeryWorld Neurosurgery
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