Search results for "Intermediate energy"

showing 10 items of 13 documents

Population of lead isotopes in binary reactions using a Rb 94 radioactive beam

2020

8 pags., 9 figs.

3106PopulationNuclear TheoryBinary number[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyParticle detectorNuclear physicsnuclear reaction ; transfer reaction ; radioactive beam0103 physical sciencesNuclear ReactionsNeutronNuclear Physics - Experiment010306 general physicseducationNuclear Experimentnuclear reactionsPhysicseducation.field_of_studyisotoopitScience & TechnologyIsotope010308 nuclear & particles physicsPhysicsPhysics NuclearPhysical Sciencestransfer reactionsPhysics::Accelerator Physicslow and intermediate energy heavy-ion reactionslyijymodels nad methods for nuclear reactionsNucleonydinfysiikkaBeam (structure)Radioactive beamPhysical Review C
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Probing the Merits of Different Event Parameters for the Identification of Light Charged Particles in CHIMERA CsI(Tl Detectors With Digital Pulse Sha…

2013

We investigated the merits of different event parameters in the identification of Light Charged Particles (LCPs) with CsI(Tl) scintillators read out by photodiodes at high incident energy (400 MeV/u). This investigation is made possible by digital signal processing the output signals. As in the conventional analogue case, the digitized signals allow the discrimination of light charged particles by computing the fast and slow components. In addition other identification parameters as the rise time of the output pulses of the CsI(Tl) come out nearly for free. Aim of this paper is the investigation of novel identification plots and the probe of their merits, in particular at relativistic energ…

Nuclear and High Energy PhysicsPhysics::Instrumentation and Detectorsintermediate energy nuclear physicpulse shape analysiScintillatorParticle identificationlaw.inventionOpticslawElectrical and Electronic EngineeringDigital signal processingPhysicsonline digital signal processingSignal processingsezeleCsI(Tl) scintillatorsbusiness.industrypulse shape analysisDetectorCsI(Tl) scintillatorCsI(Tl) scintillators; intermediate energy nuclear physics; online digital signal processing; particle identification; pulse shape analysisCsI(Tl) scintillators; intermediate energy nuclear physics; online digital signal processing; particle identification; pulse shape analysis; Electrical and Electronic Engineering; Nuclear Energy and Engineering; Nuclear and High Energy PhysicsCharged particlePhotodiodeintermediate energy nuclear physicsNuclear Energy and EngineeringRise timeparticle identificationbusinessnuclear physics; heavy-ions; digital signal processing; scintillation detectors
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Neutron yield from a thick target irradiated by 90MeV protons

2005

In the context or the design of an intense source of low and intermediate energy, neutrons, the angular and energy distributions of neutrons produced in the interaction of 90 MeV protons in a C-12 target, in which the protons are stopped, have been measured by time-of-flight and activation techniques, As compared to C-12 the yield is less than a factor two higher, while it is somewhat less than for a Be-9 target. (c) 2005 Elsevier B.V. All rights reserved.

PhysicsNuclear and High Energy PhysicsFissionNuclear TheoryContext (language use)Nuclear physicsDeuteriumIntermediate energyNeutron yieldYield (chemistry)NeutronIrradiationAtomic physicsNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Charged current weak electroproduction of the Delta resonance

1998

We study the weak production of $\ensuremath{\Delta}$ (i.e., ${e}^{\ensuremath{-}}+\stackrel{\ensuremath{\rightarrow}}{p}{\ensuremath{\Delta}}^{0}+{\ensuremath{\nu}}_{e}$ and ${e}^{+}+\stackrel{\ensuremath{\rightarrow}}{p}{\ensuremath{\Delta}}^{++}+{\overline{\ensuremath{\nu}}}_{e})$ in the intermediate energy range corresponding to the Mainz and TJNAF electron accelerators. The differential cross sections $\ensuremath{\sigma}(\ensuremath{\theta})$ are found to be of the order of ${10}^{\ensuremath{-}39}$ cm${}^{2}$/sr, over a range of angles which increases with energy. The possibility of observing these reactions with the high luminosities available at these accelerators, and studying the…

PhysicsNuclear and High Energy PhysicsParticle physicsAngular distributionIntermediate energyOrder (ring theory)FísicaProduction (computer science)ElectronResonance (particle physics)Energy (signal processing)Charged current
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Double polarization experiments at intermediate energy

1999

At modern electron accelerators with highly polarized, intense, high duty factor beams double polarization coincidence experiments became feasible with good statistical accuracy. The strong potential towards the precise determination of small nucleon structure quantities is illustrated by two recent examples from MAMI. The measurement of $G_E^n$ in the quasifree reaction $D(\vec e, e'\vec n)p$ lead to a new parametrization of $G_E^n$ which is significantly above the previously preferred one from elastic $e-D$ scattering. A $p(\vec e, e'\vec p)\pi^0$ experiment at the energy of the $\Delta$ resonance yields preliminary results for the longitudinal quadrupole mixing. Both experimental errors …

PhysicsNuclear and High Energy PhysicsScatteringNuclear TheoryFOS: Physical sciencesElectronPolarization (waves)CoincidenceNuclear physicsIntermediate energyDuty cycleQuadrupoleNuclear Experiment (nucl-ex)NucleonNuclear ExperimentNuclear Experiment
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Electroweak effects in intermediate energy physics

2008

PhysicsParticle physicsIntermediate energyNeutral currentPartial wave analysisElectroweak interactionTechnicolorBorn approximation
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Search for elements 119 and 120

2020

A search for production of the superheavy elements with atomic numbers 119 and 120 was performed in the 50Ti+249Bk and 50Ti+249Cf fusion-evaporation reactions, respectively, at the gas-filled recoil separator TASCA at GSI Darmstadt, Germany. Over four months of irradiation, the 249Bk target partially decayed into 249Cf, which allowed for a simultaneous search for both elements. Neither was detected at cross-section sensitivity levels of 65 and 200 fb for the 50Ti+249Bk and 50Ti+249Cf reactions, respectively, at a midtarget beam energy of Elab=281.5 MeV. The nonobservation of elements 119 and 120 is discussed within the concept of fusion-evaporation reactions including various theoretical pr…

Physicselement 119010308 nuclear & particles physicselement 120Superheavy Elements01 natural sciencesIsland of stabilityRecoil separatorNuclear physicssuperheavy elementsProduction cross sectionSubatomic Physics0103 physical sciences540 Chemistry570 Life sciences; biologylow and intermediate energy heavy-ion reactionsAtomic numberIrradiationSensitivity (control systems)ydinfysiikka010306 general physicsBeam energyPhysical Review C
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High-precision mass measurements and production of neutron-deficient isotopes using heavy-ion beams at IGISOL

2019

An upgraded ion-guide system for the production of neutron-deficient isotopes with heavy-ion beams has been commissioned at the IGISOL facility with an $^{36}\mathrm{Ar}$ beam on a $^{\mathrm{nat}}\mathrm{Ni}$ target. It was used together with the JYFLTRAP double Penning trap to measure the masses of $^{82}\mathrm{Zr}, ^{84}\mathrm{Nb}, ^{86}\mathrm{Mo}, ^{88}\mathrm{Tc}$, and $^{89}\mathrm{Ru}$ ground states and the isomeric state $^{88}\mathrm{Tc}^{m}$. Of these, $^{89}\mathrm{Ru}$ and $^{88}\mathrm{Tc}^{m}$ were measured for the first time. The precision of measurements of $^{82}\mathrm{Zr}, ^{84}\mathrm{Nb}$, and $^{88}\mathrm{Tc}$ was significantly improved. The literature value for $^…

RPPHASEONLINE7. Clean energy01 natural sciences114 Physical sciencesbinding energy and massesPENNING TRAPS0103 physical sciencesNeutron010306 general physicsNuclear ExperimentPhysicsisotoopitSpinsIsotope010308 nuclear & particles physicsenergy levels and level densitiesRAMSEY METHODGAMMAPenning trapAtomic massSPECTROMETRYProduction (computer science)Heavy ionlow and intermediate energy heavy-ion reactionsAtomic physicsydinfysiikkaNUCLEAR-MASSESBeam (structure)Physical Review C
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β and γ bands in N = 88, 90, and 92 isotones investigated with a five-dimensional collective Hamiltonian based on covariant density functional theory…

2019

A comprehensive systematic study is made for the collective β and γ bands in even-even isotopes with neutron numbers N=88 to 92 and proton numbers Z=62(Sm) to 70 (Yb). Data, including excitation energies, B(E0) and B(E2) values, and branching ratios from previously published experiments are collated with new data presented for the first time in this study. The experimental data are compared to calculations using a five-dimensional collective Hamiltonian (5DCH) based on the covariant density functional theory (CDFT). A realistic potential in the quadrupole shape parameters V(β,γ) is determined from potential energy surfaces (PES) calculated using the CDFT. The parameters of the 5DCH are fixe…

electromagnetic transitionsnuclear density functional theorynuclear spin and paritynucleon induced nuclear reactionscollective levelscollective modelslow and intermediate energy heavy-ion reactionsydinfysiikka
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Investigation of fusion probabilities in the reactions with 52,54Cr, 64Ni, and 68Zn ions leading to the formation of Z = 120 superheavy composite sys…

2020

Background: The formation of superheavy nuclei in fusion reactions is suppressed by a competing quasifission process. The competition between the formation of the compound nucleus and the quasifission depends strongly on the reaction entrance channel. Purpose: The investigation of fission and quasifission processes in the formation of Z=120 superheavy composite systems in the 52,54Cr+248Cm and 68Zn+232Th reactions, and their comparison with the 64Ni+238U reaction at energies in the vicinity of the Coulomb barrier. Methods: Mass-energy distributions of fissionlike fragments formed in the reactions 52,54Cr+248Cm and 68Zn+232Th at energies near the Coulomb barrier were measured using the doubl…

fissiofuusioreaktiolow and intermediate energy heavy-ion reactionsydinfysiikkanuclear fusion
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