Search results for "530"

showing 10 items of 1476 documents

Lower bound on the proton charge radius from electron scattering data

2019

The proton charge-radius determinations from the electromagnetic form-factor measurements in electron-proton scattering require an extrapolation to zero momentum transfer ($Q^2=0$) which is prone to model-dependent assumptions. We show that the data at finite momentum transfer can be used to establish a rigorous lower bound on the proton charge radius. Using the available $ep$ data at low $Q^2$, we obtain $R_E > 0.850(1)$ fm as the lower bound on the proton radius. This reaffirms the discrepancy between the $ep$ and muonic-hydrogen values, while bypassing the model-dependent assumptions that go into the fitting and extrapolation of the $ep$ data.

PhysicsNuclear and High Energy PhysicsProtonNuclear Theory010308 nuclear & particles physicsScattering530 PhysicsMomentum transferExtrapolationFOS: Physical sciencesCharge densityRadius01 natural sciencesUpper and lower boundslcsh:QC1-999Nuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Charge radius0103 physical sciencesNuclear Experiment (nucl-ex)Atomic physics010306 general physicsNuclear Experimentlcsh:Physics
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Technical design report for the $\overline{{\rm{P}}}\mathrm{ANDA}$ Barrel DIRC detector

2019

The $\overline{{\rm{P}}}\mathrm{ANDA}$ (anti-Proton ANnihiliation at DArmstadt) experiment will be one of the four flagship experiments at the new international accelerator complex FAIR (Facility for Antiproton and Ion Research) in Darmstadt, Germany. $\overline{{\rm{P}}}\mathrm{ANDA}$ will address fundamental questions of hadron physics and quantum chromodynamics using high-intensity cooled antiproton beams with momenta between 1.5 and 15 GeV/c and a design luminosity of up to 2 × 1032 cm−2 s−1. Excellent particle identification (PID) is crucial to the success of the $\overline{{\rm{P}}}\mathrm{ANDA}$ physics program. Hadronic PID in the barrel region of the target spectrometer will be per…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Large Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsHadronDetectorBarrel (horology)7. Clean energy01 natural sciencesRing-imaging Cherenkov detectorParticle identificationCharged particleNuclear physics0103 physical sciencesHigh Energy Physics::Experimentddc:530010306 general physicsNuclear Experiment
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Exclusive ϱ0 and φ muoproduction at large Q2

1994

Abstract Exclusive ϱ 0 and φ muoproduction on deuterium, carbon and calcium has been studied in the kinematic range 2 Q 2 2 and 40 Q 2 dependence of the cross sections, the transverse momentum distributions for the vector mesons, the decay angular distributions and, in the case of the ϱ 0 , nuclear effects. The data for 0 production are compatible with a diffractive mechanism. The distinct features of φ production are a smaller cross section and less steep p t 2 distributions than those for the 0 mesons.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsMesonHADRONSMUON SCATTERINGTRANSVERSE-MOMENTUMPROTONQCD530Nuclear physicsCross section (physics)RATIOAngular distributionDeuteriumTransverse momentumDEEP INELASTIC-SCATTERING; MUON SCATTERING; TRANSVERSE-MOMENTUM; PROTON; HADRONS; RATIO; QCDDEEP INELASTIC-SCATTERINGNuclear Physics B
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Recent progress in laser spectroscopy of the actinides

2020

The interest to perform laser spectroscopy in the heaviest elements arises from the strong impact of relativistic effects, electron correlations and quantum electrodynamics on their atomic structure. Once this atomic structure is well understood, laser spectroscopy also provides access to nuclear properties such as spins, mean square charge radii and electromagnetic moments in a nuclear-model independent way. This is of particular interest for the heaviest actinides around $N = 152$, a region of shell stabilized deformed nuclei. The experimental progress of laser spectroscopy in this region benefitted from continuous methodological and technical developments such as the introduction of buff…

PhysicsNuclear and High Energy PhysicsSpins010308 nuclear & particles physicsAtomic Physics (physics.atom-ph)Nuclear Theorychemistry.chemical_elementFOS: Physical sciencesCharge (physics)ActinideElectron01 natural sciencesPhysics - Atomic Physics3. Good healthNuclear physicschemistry0103 physical sciencesddc:530NobeliumNuclide010306 general physicsRelativistic quantum chemistrySpectroscopyNuclear ExperimentProgress in Particle and Nuclear Physics
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Coulomb and nuclear excitations of narrow resonances in 17Ne

2016

Physics letters / B 759, 200 - 205 (2016). doi:10.1016/j.physletb.2016.05.073

PhysicsNuclear and High Energy PhysicsTeoría de los quantaInternal energySpins010308 nuclear & particles physicsProjectile310601 natural sciences530lcsh:QC1-999Mass formulaNuclear physics0103 physical sciencesPhysical SciencesCoulombIsobaric processFysikddc:530Atomic physics010306 general physicsMultipletExcitationlcsh:PhysicsPhysics Letters B
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Modelling of the magnetic field structures and first measurements of heat fluxes for TEXTOR-DED operation

2004

The dynamic ergodic divertor (DED) was recently installed at the TEXTOR tokamak. One of the aims of the DED is to control and study heat and particle deposition on a plasma wall via modification of the plasma edge by external perturbation coils. Sixteen perturbation coils are mounted on the high-field side of the torus. The external magnetic perturbation creates a zone of chaotic field lines at the plasma edge by destroying several resonant surfaces. These structures have the properties of an open chaotic system while the field lines intersect the tokamak vessel. In order to study the topology of the field lines in different regimes, a set of tools called Atlas was created. Atlas uses a sym…

PhysicsNuclear and High Energy PhysicsTokamakField lineDivertorChaoticPerturbation (astronomy)TorusPlasmaCondensed Matter PhysicsComputational physicslaw.inventionMagnetic fieldJlawPhysics::Plasma Physicsddc:530Atomic physics
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Zeptosecond contact times for element Z=120 synthesis

2020

The synthesis of new superheavy elements beyond oganesson (Z=118) requires fusion reactions with projectile nuclei with proton numbers larger than that of $^{48}$Ca (Z=20), which has been successfully employed for the synthesis of elements with Z=112-118. In such reactions, fusion is drastically hindered by fast non-equilibrated dynamical processes. Attempts to produce nuclei with Z=120 using the $^{64}$Ni+$^{238}$U, $^{58}$Fe+$^{244}$Pu, $^{54}$Cr+$^{248}$Cm, and $^{50}$Ti+$^{249}$Cf reactions have been made, which all result in larger Coulomb forces than for $^{48}$Ca-induced reactions, but no discovery has been confirmed to date. In this work, mass and angle distributions of fission frag…

PhysicsNuclear and High Energy PhysicsWork (thermodynamics)FusionSuperheavy-element formationProton010308 nuclear & particles physicsFissionProjectile01 natural scienceslcsh:QC1-9993. Good healthYield (chemistry)Quasifission0103 physical sciencesCoulombNuclear fusionddc:530Atomic physics010306 general physicsZ=120lcsh:PhysicsPhysics Letters
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Mass spectrometry and decay spectroscopy of isomers across the Z=82 shell closure

2013

Recent results from a measurement campaign studying the isomerism in neutron-deficient Tl isotopes are presented. The measurements make use of a nuclear spectroscopy setup coupled to the high-resolution Penning-trap mass spectrometer ISOLTRAP at CERN's radioactive ion-beam facility ISOLDE. The mass values of 190,194Tl are improved and a mass-spin-state assignment is carried out. An additional mass measurement of the grandparent nuclide 198At allows the deduction of the spin-state ordering in 190Tl. As a result, the excitation energies of the isomers in both Tl isotopes are determined for the first time to Eex(194Tl)=260(15) keV and E ex(190Tl)=89(12) keV. Furthermore, this allows anchoring …

PhysicsNuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsClosure (topology)Shell (structure)ISOLTRAPMass spectrometry01 natural sciencesIon trappingISOLTRAPPenning ion trapTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesisomersddc:530Atomic physicsNuclear Experiment010306 general physicsSpectroscopyZ=82mass spectrometry
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Proton emission from an oblate nucleus 151Lu

2013

Abstract Excited states in the proton-unbound nucleus 151Lu have been established using γ-ray coincidence techniques. The lifetime of the first excited state above the proton-emitting ground state has been measured using the recoil-distance Doppler-shift method combined with recoil-decay tagging. The experimental level scheme and extracted lifetime have been compared with state-of-the-art theoretical calculations based upon a non-adiabatic deformed Woods–Saxon potential. This comparison suggests that the proton-emitting ground state in 151Lu is mildly oblate with a deformation β = − 0.11 − 0.05 + 0.02 and represents the best evidence to date for proton emission from an oblate nucleus.

PhysicsNuclear and High Energy Physicsta114010308 nuclear & particles physicsNuclear TheoryHadronElementary particle01 natural sciences7. Clean energyBaryonmedicine.anatomical_structureExcited state0103 physical sciencesmedicineddc:530Atomic physicsProton emissionNuclear Experiment010306 general physicsGround stateNucleonNucleusPhysics Letters B
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On the measured lifetime of light hypernuclei 3ΛH and 4ΛH

2014

A statistical combination of the experimental lifetime estimations available in the literatures is performed for 3 Λ H and 4 Λ H, including several recent measurements. The combined average values of the lifetime for 3 Λ H and 4 Λ H are respectively 216−16+19 ps and 192−18+20 ps with a reduced χ2 of 0.89 and 0.48. A new insight into the lifetime estimation of the HypHI Phase 0 experiment by a Bayesian approach is also presented. In this approach, several different prior distributions including the combination of previous lifetime data and a Jeffrey prior are used. The principal mode and the smallest credible interval at 68% of the posterior distribution, given by the prior belief of the pre…

PhysicsNuclear physicsNuclear and High Energy PhysicsLifetime measurementPosterior probabilityHypernucleiBayesian approachCredible intervalddc:530LambdaHypertritonAveraged combinationPhysics Letters B
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