Search results for "NATURAL SCIENCES. Physics."

showing 10 items of 50 documents

Quasi-elastic polarization-transfer measurements on the deuteron in anti-parallel kinematics

2019

We present measurements of the polarization-transfer components in the H2(e→,e′p→) reaction, covering a previously unexplored kinematic region with large positive (anti-parallel) missing momentum, pmiss, up to 220MeV/c, and Q2=0.65 (GeV/c)2. These measurements, performed at the Mainz Microtron (MAMI), were motivated by theoretical calculations which predict small final-state interaction (FSI) effects in these kinematics, making them favorable for searching for medium modifications of bound nucleons in nuclei. We find in this kinematic region that the measured polarization-transfer components Px and Pz and their ratio agree with the theoretical calculations, which use free-proton form factor…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciencesKinematicsPolarization (waves)01 natural scienceslcsh:QC1-999NATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Parallel kinematicsNuclear physicsDeuterium0103 physical sciencesddc:530Nuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Nuclear ExperimentMicrotronlcsh:Physicspolarization-transfer ; deuteron ; anti-parallel kinematics
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Nuclear symmetry energy and neutron skins derived from pygmy dipole resonances

2007

By exploiting Coulomb dissociation of high-energy radioactive beams of the neutron-rich nuclei $^{129\ensuremath{-}132}\mathrm{Sn}$ and $^{133,134}\mathrm{Sb}$, their dipole-strength distributions have been measured. A sizable fraction of ``pygmy'' dipole strength, energetically located below the giant dipole resonance, is observed in all of these nuclei. A comparison with available pygmy resonance data in stable nuclei ($^{208}\mathrm{Pb}$ and $N=82$ isotones) indicates a trend of strength increasing with the proton-to-neutron asymmetry. On theoretical grounds, employing the RQRPA approach, a one-to-one correlation is found between the pygmy strength and parameters describing the density d…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryHadronNuclear structureElementary particlereactions induced by unstable nucleiCoulomb excitation01 natural sciencesNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Dipole0103 physical sciencesIsotopes of tinNeutronAtomic physicsCoulomb excitation by heavy ionsNuclear Experiment010306 general physicsNucleonnuclear giant resonancesPhysical Review C
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Polarization-transfer measurement to a large-virtuality bound proton in the deuteron

2017

Possible differences between free and bound protons may be observed in the ratio of polarization-transfer components, $P'_x/P'_z$. We report the measurement of $P'_x/P'_z$, in the $^2\textrm{H}(\vec{e},e^{\prime}\vec{p})n$ reaction at low and high missing momenta. Observed increasing deviation of $P'_x/P'_z$ from that of a free proton as a function of the virtuality, similar to that observed in \hefour, indicates that the effect in nuclei is due to the virtuality of the knock-out proton and not due to the average nuclear density. The measured differences from calculations assuming free-proton form factors ($\sim10\%$), may indicate in-medium modifications.

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciencesPolarization (waves)01 natural sciencesNATURAL SCIENCES. Physics.lcsh:QC1-999Nuclear physicsPRIRODNE ZNANOSTI. Fizika.Deuterium0103 physical sciencesd(e e’p) ; Electron-scatteringPhysics::Accelerator PhysicsNuclear Experiment (nucl-ex)Electron-scattering010306 general physicsNuclear Experimentd(ee'p)Electron scatteringNuclear ExperimentNuclear densitylcsh:PhysicsPhysics Letters B
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New Insight in the $Q^2$-Dependence of Proton Generalized Polarizabilities

2019

Virtual Compton scattering on the proton has been investigated at three yet unexplored values of the four-momentum transfer $Q^2$: 0.10, 0.20 and 0.45 GeV$^2$, at the Mainz Microtron. Fits performed using either the low-energy theorem or dispersion relations allowed the extraction of the structure functions $P_{LL} -P_{TT} / \epsilon$ and $P_{LT}$, as well as the electric and magnetic generalized polarizabilities $\alpha_{E1}(Q^2)$ and $\beta_{M1}(Q^2)$. These new results show a smooth and rapid fall-off of $\alpha_{E1}(Q^2)$, in contrast to previous measurements at $Q^2$ = 0.33 GeV$^2$, and provide for the first time a precise mapping of $\beta_{M1}(Q^2)$ in the low-$Q^2$ region.

PhysicsProtonCompton scatteringFOS: Physical sciencesGeneral Physics and Astronomy25.30.Dh[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Nuclear physics13.60.FzVirtual Compton Scattering VCS Proton Polarizability MAMI0103 physical sciences14.20.DhNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear Physics
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Level structure of 99Nb

1998

The β decay of 97Sr to 97Y has been investigated using ion-guide on-line mass separation and a 10 Ge-detector array to record γ−γ coincidences to a detection limit well below that of former studies. Similarities are found in the β-decay patterns of 99Zr and of its isotone 97Sr and also in the γ-ray decay rates and branchings of the corresponding levels in their respective daughters 99Nb and 97Y. This indicates a persisting influence of the d5/2 neutron shell closure for 99Nb. The level structure of 99Nb and the β-feeding pattern are discussed in the frame of the interacting boson-fermion plus broken pair model and the microscopic quasiparticle phonon model.

Physicsbeta decay nuclear stucture 99Nb interacting boson-fermion plus broken pair modelNuclear and High Energy PhysicsCondensed matter physicsPhononIsotoneShell (structure)Beta decayMolecular physicsNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.QuasiparticleLevel structureNeutronInteracting boson modelbeta decay; nuclear stucture; 99Nb; interacting boson-fermion plus broken pair model
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Level structure of ^100Nb

2000

Levels in the odd-odd nucleus ${}^{100}\mathrm{Nb}$ situated at the edge of a region of especially fast shape transitions have been calculated in the framework of the interacting boson fermion fermion model. Levels observed in decay studies can be interpreted in a spherical basis. Low-lying ${I}^{\ensuremath{\pi}}{=8}^{+}$ and ${10}^{\ensuremath{-}}$ states are predicted. Their relationship with the unplaced levels populated with a $12 \ensuremath{\mu}\mathrm{s}$ delay after fission is discussed.

Physicsnuclear structure; atomic nucleus 100Nb; shape transitions; boson fermion fermion model; nuclear levelsNuclear and High Energy PhysicsFissionNuclear structurenuclear levelsFermionSpherical basisatomic nucleus 100NbNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.shape transitionsnuclear structureboson fermion fermion modelLevel structureAtomic physicsBoson
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Measurement of visible cross sections in proton-lead collisions at √sNN= 5.02 TeV in van der Meer scans with the ALICE detector

2014

In 2013, the Large Hadron Collider provided proton-lead and lead-proton collisions at the center-of-mass energy per nucleon pair $\sqrt{s_{\rm{NN}}}=5.02$ TeV. Van der Meer scans were performed for both configurations of colliding beams, and the cross section was measured for two reference processes, based on particle detection by the T0 and V0 detectors, with pseudo-rapidity coverage $4.6<\eta< 4.9$, $-3.3<\eta<-3.0$ and $2.8<\eta< 5.1$, $-3.7<\eta<-1.7$, respectively. Given the asymmetric detector acceptance, the cross section was measured separately for the two configurations. The measured visible cross sections are used to calculate the integrated luminosity of the proton-lead and lead-…

ProtonNuclear Theorylarge detector systems for particle and astroparticle physicsLarge detector systems for particle and astroparticle physics; Particle tracking detec- tors; Heavy-ion detectors01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Particle tracking detectorsparticle tracking detectors[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Neutron detectionNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentInstrumentationMathematical PhysicsPhysicsLarge Hadron ColliderLuminosity (scattering theory)PhysicsDetectorLuminosity measurement3. Good healthPRIRODNE ZNANOSTI. Fizika.Large detector systems for particle and astroparticle physics Particle tracking detec- torNucleonParticle Physics - ExperimentLarge detector systems for particle and astroparticle physics ; Particle tracking detectors ; Heavy-ion detectorsParticle physicsParticle tracking detec- torsInstrumentationHeavy-ion detectorsFOS: Physical sciencesLarge detector systems for particle and astroparticle physics; Particle tracking detectors; Heavy-ion detectors[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear physicsCross section (physics)p-Pb collisions at the LHC0103 physical sciencesNuclear Physics - Experiment010306 general physics010308 nuclear & particles physicsLarge detector systems for particle and astroparticle physicsALICE experimentLarge detector systems for particle and astroparticle physics Particle tracking detec- tors; Heavy-ion detectorsNATURAL SCIENCES. Physics.heavy-ion detectorsInstrumentation; Mathematical PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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Technical design report for the upgrade of the ALICE inner tracking system

2014

ALICE (A Large Ion Collider Experiment) is studying the physics of strongly interacting matter, and in particular the properties of the Quark–Gluon Plasma (QGP), using proton–proton, proton–nucleus and nucleus–nucleus collisions at the CERN LHC (Large Hadron Collider). The ALICE Collaboration is preparing a major upgrade of the experimental apparatus, planned for installation in the second long LHC shutdown in the years 2018–2019. A key element of the ALICE upgrade is the construction of a new, ultra-light, high- resolution Inner Tracking System (ITS) based on monolithic CMOS pixel detectors. The primary focus of the ITS upgrade is on improving the performance for detection of heavy-flavour…

ROOT-S=2.76 TEV; PP COLLISIONS; DETECTORS; RECONSTRUCTION; ELECTRONICS; SILICON; PHYSICS; MODELPhysics::Instrumentation and DetectorsNuclear TheoryNuclear and High Energy Physics;Tracking (particle physics)01 natural sciences7. Clean energydecaylaw.inventionUpgradeALICElawLHC; ALICE; Inner Tracking SystemNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ComputingMilieux_MISCELLANEOUSPhysicsLarge Hadron ColliderDetectorSettore FIS/01 - Fisica SperimentaleTracking systemPRIRODNE ZNANOSTI. Fizika.UpgradeLHCParticle physicsNuclear and High Energy PhysicsALICE Inner Tracking SystemROOT-S=2.76 TEV; pp collisions; DETECTORS; RECONSTRUCTION; ELECTRONICS; SILICON; PHYSICS; MODEL; decay[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Dot pitchPHYSICSELECTRONICS0103 physical sciencesDETECTORSRECONSTRUCTIONCMOS pixel sensors010306 general physicsColliderROOT-S=2.76 TEVSILICONPP COLLISIONSPixel010308 nuclear & particles physicsbusiness.industryALICE experimentInner Tracking SystemTechnical Design ReportNATURAL SCIENCES. Physics.MODELDetector upgradeTechnical Design Report; Upgrade; ALICE Inner Tracking SystemHigh Energy Physics::Experimentbusiness
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First Measurement of the $Q^2$ Dependence of the Beam-Normal Single Spin Asymmetry for Elastic Scattering off Carbon

2018

We report on the first Q^{2}-dependent measurement of the beam-normal single spin asymmetry A_{n} in the elastic scattering of 570 MeV vertically polarized electrons off ^{12}C. We cover the Q^{2} range between 0.02 and 0.05  GeV^{2}/c^{2} and determine A_{n} at four different Q^{2} values. The experimental results are compared to a theoretical calculation that relates A_{n} to the imaginary part of the two-photon exchange amplitude. The result emphasizes that the Q^{2} behavior of A_{n} given by the ratio of the Compton to charge form factors cannot be treated independently of the target nucleus.

carbon: targetelectron: polarized beammedia_common.quotation_subjectGeneral Physics and AstronomyElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]momentum transfer dependence01 natural sciencesAsymmetryMainz Linac0103 physical sciencesgallium: arsenicpolarization: transverseelektronsko raspršenje010306 general physicsNuclear ExperimentSpin-½media_commonPhysicsElastic scatteringform factor: ratioform factor: chargeexchange: two-photon010308 nuclear & particles physicsnucleus: targetizmjena dva fotonaelectron nucleus: elastic scatteringCharge (physics)amplitude analysisNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.spin: asymmetry: measuredElektronsko raspršenje izmjena dva fotonaAmplitudeCover (topology)High Energy Physics::ExperimentAtomic physicsradiation: laserBeam (structure)photoelectronexperimental results
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Precision measurement of the mass difference between light nuclei and anti-nuclei

2015

The measurement of the mass differences for systems bound by the strong force has reached a very high precision with protons and anti-protons. The extension of such measurement from (anti-)baryons to (anti-)nuclei allows one to probe any difference in the interactions between nucleons and anti-nucleons encoded in the (anti-)nuclei masses. This force is a remnant of the underlying strong interaction among quarks and gluons and can be described by effective theories, but cannot yet be directly derived from quantum chromodynamics. Here we report a measurement of the difference between the ratios of the mass and charge of deuterons and anti-deuterons, and $^{3}{\rm He}$ and $^3\overline{\rm He}…

electronQuarkspectroscopyAntiparticleParticle physicsPhysics of Elementary Particles and FieldsCPT symmetryStrong interactionNuclear TheoryantunucleiFOS: Physical sciencesAntiprotonGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ElectronHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Physics and Astronomy (all)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Physics - ExperimentNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentAntihydrogenSpectroscopyNuclear Physicsantihydrogenmass measurementQuantum chromodynamicsPhysicsanti-nucleita114SPECTROSCOPY; ANTIHYDROGEN; ANTIPROTON; ELECTRONmass difference nuclei antunucleiHigh Energy Physics::Phenomenologymass differenceNATURAL SCIENCES. Physics.3. Good healthGluonPRIRODNE ZNANOSTI. Fizika.antiprotonnucleiQuark–gluon plasmamassmass difference ; nuclei ; anti-nuclei ; ALICE ; CERNHigh Energy Physics::ExperimentNucleon
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