Search results for "Nucleon"

showing 10 items of 1041 documents

The EPPS16 nuclear PDFs

2017

We report on EPPS16 - the first analysis of NLO nuclear PDFs where LHC p-Pb data (Z, W, dijets) have been directly used as a constraint. In comparison to our previous fit EPS09, also data from neutrino-nucleus deeply-inelastic scattering and pion-nucleus Drell-Yan process are now included. Much of the theory framework has also been updated from EPS09, including a consistent treatment of heavy quarks in deeply-inelastic scattering. However, the most notable change is that we no longer assume flavour-blind nuclear modifications for valence and sea quarks. This significantly reduces the theoretical bias. All the analysed data are well reproduced and the analysis thereby supports the validity o…

Drell-Yan processHeavy-quarkHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyElementary particlesFOS: Physical sciencesSea quarks Inelastic scatteringHigh-energy collisions114 Physical sciencesHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)nuclear PDFsHigh Energy Physics - Phenomenology (hep-ph)Lead Deeply inelastic scatteringsLeadInelastic ScatteringHeavy nucleusHigh Energy Physics::ExperimentNuclear modificationHigh energy physicsNuclear ExperimentPartonsNucleons
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Sivers asymmetry extracted in SIDIS at the hard scales of the Drell-Yan process at COMPASS

2017

Proton transverse-spin azimuthal asymmetries are extracted from the COMPASS 2010 semi-inclusive hadron measurements in deep inelastic muon-nucleon scattering in those four regions of the photon virtuality $Q^2$, which correspond to the four regions of the di-muon mass $\sqrt{Q^2}$ used in the ongoing analysis of the COMPASS Drell-Yan measurements. This allows for a future direct comparison of the nucleon transverse-momentum-dependent parton distribution functions extracted from these two alternative measurements. Various two-dimensional kinematic dependences are presented for the azimuthal asymmetries induced by the Sivers transverse-momentum-dependent parton distribution function. The inte…

Drellâ YanDrell-Yan processPhotonHadronparton: distribution functionDrell-YanPartontransverse momentum dependence01 natural sciencesCOMPASSSIDISHigh Energy Physics - ExperimentSivers functionSubatomär fysikHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)CompassSubatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]dimension: 2Nuclear ExperimentSIDIS; Drell–Yan; Spin; Azimuthal asymmetries; Sivers; TMDsmedia_commonPhysicsQuantum chromodynamicsdeep inelastic scattering: semi-inclusive reactionpolarized target: transversephotonDrell–Yan processhep-phlcsh:QC1-999Drell–YanAzimuthal asymmetrieHigh Energy Physics - PhenomenologykinematicsSiverpolarized beam: longitudinalNucleonAzimuthal asymmetriesspin: asymmetryParticle Physics - ExperimentParticle physicsNuclear and High Energy Physicsangular distribution: asymmetrymedia_common.quotation_subjectFOS: Physical sciencesTMDsAsymmetryNuclear physicsSpin[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]Azimuthal asymmetries; Drell–Yan; SIDIS; Sivers; Spin; TMDs; Nuclear and High Energy Physics0103 physical sciencesmuon nucleon: deep inelastic scatteringquantum chromodynamicsSiversmuon nucleon: scattering010306 general physicsParticle Physics - Phenomenologynucleon: transverse momentum010308 nuclear & particles physics160 GeV/chep-exCERN SPSmuon+ p: deep inelastic scattering[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentlcsh:Physicsexperimental results
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Unveiling the strong interaction among hadrons at the LHC

2020

One of the key challenges for nuclear physics today is to understand from first principles the effective interaction between hadrons with different quark content. First successes have been achieved using techniques that solve the dynamics of quarks and gluons on discrete space-time lattices1,2. Experimentally, the dynamics of the strong interaction have been studied by scattering hadrons off each other. Such scattering experiments are difficult or impossible for unstable hadrons3–6 and so high-quality measurements exist only for hadrons containing up and down quarks7. Here we demonstrate that measuring correlations in the momentum space between hadron pairs8–12 produced in ultrarelativistic…

EXCHANGE-POTENTIAL APPROACHStrange quarkALICE CollaborationHadronNuclear TheoryStrong interaction; hadron collisionsPosition and momentum spacehiukkasfysiikkanucl-ex7. Clean energy01 natural sciencesVDP::Fysikk: 430High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Hadron-Hadron scattering (experiments)scattering [hadron]p p scattering[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [p p]Nuclear Experiment (nucl-ex)Experimental nuclear physicsNUCLEONNuclear ExperimentNuclear ExperimentVDP::Physics: 430PhysicsMultidisciplinaryLarge Hadron ColliderPhysicsstrong interactionlattice [space-time]Publisher CorrectionPRIRODNE ZNANOSTI. Fizika.EXCHANGE-POTENTIAL APPROACH; BARYON-BARYON SCATTERING; NUCLEONCERN LHC CollLHCddc:500NucleonBARYON-BARYON SCATTERINGParticle Physics - Experimentdiscrete [space-time]QuarkParticle physicshadron collisionsCERN LabGeneral Science & TechnologyStrong interactionFOS: Physical sciencesshort-rangeHadron strong interaction LHC114 Physical sciences:Fysikk: 430 [VDP]Articlehadron scatteringquarkultrarelativistic proton–proton collisions LHC ALICE0103 physical sciencesNuclear Physics - ExperimentGeneral010306 general physics:Physics: 430 [VDP]interaction [hadron hadron]hep-ex010308 nuclear & particles physicsHigh Energy Physics::Phenomenologyeffect [strong interaction]hadron-hadron interactionhadron scattering ; hadron-hadron interaction ; strong interaction: effect ; space-time: discrete ; space-time: lattice ; p p scattering ; quark ; correlation ; CERN LHC CollNATURAL SCIENCES. Physics.BaryoncorrelationHypernuclei; Neutron Stars; StrangenessPhysics::Accelerator PhysicsHigh Energy Physics::ExperimenthadronExperimental particle physicsNature
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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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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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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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Measurements of the Generalized Electric and Magnetic Polarizabilities of the Proton at LowQ2Using the Virtual-Compton-Scattering Reaction

2006

Experimental details of a virtual Compton scattering (VCS) experiment performed on the proton at the MIT-Bates out-of-plane scattering facility are presented. The VCS response functions ${P}_{LL}\ensuremath{-}{P}_{TT}/\phantom{{P}_{TT}\ensuremath{\varepsilon}}\ensuremath{\varepsilon}$ and ${P}_{LT}$ have been measured at ${Q}^{2}=0.057\phantom{\rule{0.28em}{0ex}}{\mathrm{GeV}}^{2}/{c}^{2}$. The generalized electric and magnetic polarizabilities, $\ensuremath{\alpha}({Q}^{2})$ and $\ensuremath{\beta}({Q}^{2})$, and the mean-square electric polarizability radius$\ensuremath{\langle}{r}_{\ensuremath{\alpha}}^{2}\ensuremath{\rangle}$ are obtained from a dispersion analysis of the data. The resu…

Elastic scatteringPhysicsNuclear and High Energy PhysicsProtonHeavy baryon chiral perturbation theoryScatteringHadronNuclear TheoryCompton scatteringFOS: Physical sciencesGeneral Physics and AstronomyElementary particleChirality (electromagnetism)BaryonPolarizabilityQuantum electrodynamicsDispersion (optics)Nuclear Experiment (nucl-ex)Perturbation theoryAtomic physicsNucleonNuclear ExperimentNuclear ExperimentPhysical Review Letters
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Search for Effects Beyond the Born Approximation in Polarization Transfer Observables ine→pElastic Scattering

2011

Intensive theoretical and experimental efforts over the past decade have aimed at explaining the discrepancy between data for the proton electric to magnetic form factor ratio, $$G_{E}/G_{M}$$, obtained separately from cross section and polarization transfer measurements. One possible explanation for this difference is a two-photon-exchange (TPEX) contribution. In an effort to search for effects beyond the one-photon-exchange or Born approximation, we report measurements of polarization transfer observables in the elastic $$H(\vec{e},e'\vec{p})$$ reaction for three different beam energies at a fixed squared momentum transfer $Q^2 = 2.5$ GeV$^2$, spanning a wide range of the virtual photon p…

Elastic scatteringPhysicsParticle physics010308 nuclear & particles physicsHadronMomentum transferGeneral Physics and AstronomyElementary particle01 natural sciencesBaryon0103 physical sciencesMagnetic form factorHigh Energy Physics::ExperimentBorn approximation010306 general physicsNucleonPhysical Review Letters
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Virtual Compton Scattering and polarizabilities

1999

Abstract Virtual Compton Scattering (VCS) off the proton below pion threshold allows access to generalized polarizabilities of the proton. These observables measure the response of the nucleon to low energy electromagnetic field perturbations. This paper presents a comparison with Real Compton Scattering and also results for the first dedicated VCS experiment performed at the Mainz Microtron MAMI with high resolution spectrometers at Q2 = 0.33 GeV2.

Electromagnetic fieldPhysicsNuclear and High Energy PhysicsParticle physicsProton010308 nuclear & particles physicsNuclear TheoryCompton scatteringMeasure (physics)Observable01 natural sciencesNuclear physicsPion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNucleonNuclear ExperimentMicrotron
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Compton Scattering Program Studying Nucleon Polarizabilities

2017

The A2 collaboration at the Mainz Microtron has undertaken a program of Compton scattering experiments with the goal of extracting the proton and, in the future, neutron polarizabilities. These are fundamental parameters that describe the response of the nucleon to an electromagnetic field. An extraction of these parameters will provide a crucial test of QCD theories. This talk presented the concept and status of this program, including some preliminary results.

Electromagnetic fieldQuantum chromodynamicsPhysicsParticle physicsProton010308 nuclear & particles physicsPhysicsQC1-999Nuclear TheoryCompton scattering01 natural sciencesNuclear physics0103 physical sciencesNeutronNuclear Experiment010306 general physicsNucleonMicrotronEPJ Web of Conferences
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