Search results for "Nuclear and High Energy Physics"

showing 10 items of 8241 documents

Recent Progress in the WCLL Breeding Blanket Design for the DEMO Fusion Reactor

2018

The water-cooled lithium-lead (PbLi) breeding blanket is one of the candidate systems considered for the implementation in the European Demonstration Power Plant (DEMO) nuclear fusion reactor. This concept employs PbLi liquid metal as tritium breeder and neutron multiplier, water pressurized at 15.5 MPa as the coolant, and EUROFER as the structural material. The current design is based on the single module segment approach and follows the requirements of the DEMO-2015 baseline design. The module is constituted by a basic toroidal-radial cell that is recursively repeated along the poloidal direction where the liquid metal flows along a radial-poloidal path. The heat generated by the fusion r…

liquid metal technologyNuclear and High Energy PhysicsLiquid metalPower stationLayoutComputer scienceNuclear engineeringNeutronBlanket01 natural sciences7. Clean energy010305 fluids & plasmasBreeding blanket (BB); Demonstration Power Plant (DEMO); fusion reactor design; liquid metal technology; Nuclear and High Energy Physics; Condensed Matter PhysicsBreeding blanket (BB)Conceptual design0103 physical sciencesliquid metal technology.Nuclear fusion010306 general physicsSettore ING-IND/19 - Impianti NucleariNuclear and High Energy PhysicMetalDemonstration Power Plant (DEMO)Fusion powerCondensed Matter PhysicsManifoldbreeding blanket; DEMO; fusion reactor design; liquid metal technologyCoolantElectricity generationCoolantPower generationfusion reactor designIEEE Transactions on Plasma Science
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Removal of molecular contamination in low-energy RIBs by the isolation-dissociation-isolation method

2020

Nuclear instruments & methods in physics research / B 463, 324 - 326 (2020). doi:10.1016/j.nimb.2019.04.072

low-energy RIBNuclear and High Energy PhysicsMaterials scienceCollision-induced dissociationbeam purificationtutkimuslaitteet53001 natural sciencesDissociation (chemistry)RF-quadrupolelaw.inventionIonlawDipole magnet0103 physical sciencesddc:530Instrumentation010308 nuclear & particles physics010401 analytical chemistryContaminationSynchrotronIon source0104 chemical sciencesmolecular contaminationBeamlinecollision-induced dissociationPhysics::Accelerator PhysicsAtomic physicsydinfysiikkaNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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STATUS OF STRANGENESS ELECTRO-PRODUCTION AT MAMI

2009

At the Institut für Kernphysik in Mainz, Germany, the microtron MAMI has been upgraded to 1.5 GeV electron beam energy and can now be used to study strange hadronic systems. The magnetic spectrometer KAOS from GSI was dismantled and re-installed in the spectrometer facility operated by the A1 collaboration. The spectrometer's primary purpose is to study strangeness electro-production. Its compact design and its capability to detect negative and positive charged particles simultaneously under forward scattering angles complements the existing spectrometers. In 2008, an important milestone has been reached by the successful measurement of kaon production off a liquid hydrogen target. The ide…

magnetic spectrometer; particle detector design; kaon electro-production; hypernuclei electro-productionPhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerPhysics::Instrumentation and DetectorsScatteringNuclear TheoryHadronDetectorGeneral Physics and AstronomyStrangenessCharged particleNuclear physicsPhysics::Accelerator PhysicsVacuum chamberNuclear ExperimentMicrotronStrangeness in Nuclear and Hadronic Systems
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High-precision mass measurements for the isobaric multiplet mass equation atA= 52

2017

Masses of $^{52}$Co, $^{52}$Co$^m$, $^{52}$Fe, $^{52}$Fe$^m$, and $^{52}$Mn have been measured with the JYFLTRAP double Penning trap mass spectrometer. Of these, $^{52}$Co and $^{52}$Co$^m$ have been experimentally determined for the first time and found to be more bound than predicted by extrapolations. The isobaric multiplet mass equation for the $T=2$ quintet at $A=52$ has been studied employing the new mass values. No significant breakdown (beyond the $3\sigma$ level) of the quadratic form of the IMME was observed ($\chi^2/n=2.4$). The cubic coefficient was 6.0(32) keV ($\chi^2/n=1.1$). The excitation energies for the isomer and the $T=2$ isobaric analogue state in $^{52}$Co have been d…

massaspektrometriaNuclear and High Energy Physicsisobaric multipletProtonCo-52Proton decayastrofysiikkaPenning trapFOS: Physical scienceskupariQuadratic form (statistics)atomipainot114 Physical sciences01 natural sciences7. Clean energyPENNING TRAPS0103 physical sciencesNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentMultipletmass measurementPhysicsisotoopitSPECTROSCOPY010308 nuclear & particles physicsMIRROR NUCLEIRAMSEY METHODPenning trapMN-52Mass formulaANALOG STATESPROTON RADIOACTIVITYCOULOMB DISPLACEMENT ENERGIESIsobaric processBETA-RAYAtomic physicsydinfysiikkaDECAYExcitationJournal of Physics G: Nuclear and Particle Physics
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The NEXT Project: Towards Production and Investigation of Neutron-Rich Heavy Nuclides

2022

The heaviest actinide elements are only accessible in accelerator-based experiments on a one-atom-at-a-time level. Usually, fusion–evaporation reactions are applied to reach these elements. However, access to the neutron-rich isotopes is limited. An alternative reaction mechanism to fusion–evaporation is multinucleon transfer, which features higher cross-sections. The main drawback of this technique is the wide angular distribution of the transfer products, which makes it challenging to catch and prepare them for precision measurements. To overcome this obstacle, we are building the NEXT experiment: a solenoid magnet is used to separate the different transfer products and to focus those of …

massaspektrometriaNuclear and High Energy Physicsneutron-rich nucleisolenoid separatorNEXT; neutron-rich nuclei; mutlinucleon transfer; solenoid separator; mass spectrometertutkimuslaitteetspektrometritmass spectrometermutlinucleon transferNEXTydinfysiikkaCondensed Matter PhysicsAtomic and Molecular Physics and OpticsAtoms; Volume 10; Issue 2; Pages: 59
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Observation of the rare decay K-S -> pi(0)e(+)e(-)

2003

A search for the decay Ks->pi0e+e- has been made by the NA48/1 experiment at the CERN SPS accelerator. Using data collected during 89 days in 2002 with a high-intensity Ks beam, 7 events were found with a background of 0.15 events. The branching fraction BR(Ks->pi0e+e-, m(ee) > 0.165 GeV/c^2) = (3.0^{+1.5}_{-1.2}(stat) +/-0.2 (syst)) x 10^{-9} has been measured. Using a vector matrix element and a form factor equal to one, the measurement gives BR(Ks->pi0e+e-) = (5.8^{+2.9}_{-2.4}) x 10^{-9}.

mesoni K; decadimenti rariPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsBranching fractionK-LForm factor (quantum field theory)Analytical chemistryKAON DECAYS01 natural sciences3. Good healthHigh Energy Physics - Experimentmesoni Kdecadimenti rariCP VIOLATION; KAON DECAYS; K-L; SEARCHSEARCH0103 physical sciencesMatrix elementCP VIOLATIONAtomic physics010306 general physics
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Observation of the decay KS→π+π−e+e−

2000

Abstract We present the first observation of the decay KS→π+π−e+e− based upon the data collected in 1998 by the NA48 experiment at CERN. We have identified a clean sample of 56 events with negligible background contamination. Using KL→π+π−π0D decays as normalization sample, the branching ratio is measured to be BR(KS→π+π−e+e−)=[4.5±0.7(stat)±0.4(syst)]×10−5. This result is in good agreement with the theoretical expectations from the mechanism of inner bremsstrahlung.

mesoni K; decadimenti rarimesoni KPhysicsNuclear physicsNuclear and High Energy Physicsdecadimenti rariBranching fractionBremsstrahlungNA48 experimentPhysics Letters B
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Single Event Transients and Pulse Quenching Effects in Bandgap Reference Topologies for Space Applications

2016

An architectural performance comparison of bandgap voltage reference variants, designed in a $0.18~\mu \text {m}$ CMOS process, is performed with respect to single event transients. These are commonly induced in microelectronics in the space radiation environment. Heavy ion tests (Silicon, Krypton, Xenon) are used to explore the analog single-event transients and have revealed pulse quenching mechanisms in analogue circuits. The different topologies are compared, in terms of cross-section, pulse duration and pulse amplitude. The measured results, and the explanations behind the findings, reveal important guidelines for designing analog integrated circuits, which are intended for space appli…

mikroelektroniikkaNuclear and High Energy PhysicsBandgap voltage referencecircuit topologysingle-event transient (SET)Integrated circuit01 natural scienceslaw.inventionsingle event transientsCurrent mirrorlawpulse quenchingsingle-event effects (SEE)ionizationradiation hardening by design (RHBD)0103 physical sciencesElectronic engineeringMicroelectronicsAnalog single-event transient (ASET); bandgap voltage reference (BGR); charge sharing; CMOS analog integrated circuits; heavy ion; ionization; parasitic bipolar effect; pulse quenching; radiation effects; radiation hardening by design (RHBD); reference circuits; single-event effects (SEE); single-event transient (SET); space electronics; Voltage reference; Nuclear and High Energy Physics; Nuclear Energy and Engineering; Electrical and Electronic EngineeringAnalog single-event transient (ASET)Electrical and Electronic Engineeringparasitic bipolar effectreference voltage010302 applied physicsPhysicsbandgap voltage reference (BGR)charge sharingta114ta213010308 nuclear & particles physicsbusiness.industryanalog integrated circuitsTransistorspace electronicsPulse durationheavy ionPulse (physics)Voltage referenceNuclear Energy and EngineeringPulse-amplitude modulationreference circuitsmicroelectronicsradiation effectsspace applicationsOptoelectronicsbusinessCMOS analog integrated circuitsIEEE Transactions on Nuclear Science
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Search for a diffuse flux of high-energy ¿µ with the ANTARES neutrino telescope

2011

A search for a diffuse flux of astrophysical muon neutrinos, using data collected by the ANTARES neutrino telescope is presented. A $(0.83\times 2\pi)$ sr sky was monitored for a total of 334 days of equivalent live time. The searched signal corresponds to an excess of events, produced by astrophysical sources, over the expected atmospheric neutrino background. The observed number of events is found compatible with the background expectation. Assuming an $E^{-2}$ flux spectrum, a 90% c.l. upper limit on the diffuse $\nu_\mu$ flux of $E^2\Phi_{90%} = 5.3 \times 10^{-8} \ \mathrm{GeV\ cm^{-2}\ s^{-1}\ sr^{-1}} $ in the energy range 20 TeV - 2.5 PeV is obtained. Other signal models with differ…

neutrino telescope; antares; diffuse muon neutrino fluxNuclear and High Energy PhysicsParticle physics[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE][PHYS.ASTR.IM]Physics [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]media_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaNeutrino telescopeFluxAstrophysicsNeutrino telescope01 natural sciences7. Clean energySpectral lineMUONSLIMITS0103 physical sciencesNeutrins010306 general physicsDETECTORmedia_commonPhysicsRange (particle radiation)MuonsMuonANTARES:Física [Àrees temàtiques de la UPC]010308 nuclear & particles physicsMuon Collaboration[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE]Astrophysics::Instrumentation and Methods for AstrophysicsNeutrino astrophysics[SDU.ASTR.IM]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Instrumentation and Methods for Astrophysic [astro-ph.IM]MODELDiffuse muon neutrino fluxSky:Física::Astronomia i astrofísica [Àrees temàtiques de la UPC]High Energy Physics::ExperimentFísica nuclearNeutrinoAstrophysics - High Energy Astrophysical PhenomenaEnergy (signal processing)
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Recent experiments at the JYFLTRAP Penning trap

2020

AbstractThe JYFLTRAP double Penning trap mass spectrometer at the Ion Guide Isotope Separator On-Line (IGISOL) facility offers excellent possibilities for high-precision mass measurements of radioactive ions. Around 400 atomic masses, including around 50 isomeric states, have been measured since JYFLTRAP became operational. JYFLTRAP has also been used as a high-resolution mass separator for decay spectroscopy experiments as well as an ion counter for fission yield studies. In this contribution, an overview of recent activities at the JYFLTRAP Penning trap is given, with a focus on nuclei discussed in the PLATAN2019 meeting.

nuclear binding energymassaspektrometriaNuclear and High Energy PhysicstutkimuslaitteetFission product yieldMass spectrometry7. Clean energy01 natural sciencesIonNuclear physicsPhysics in General0103 physical sciencesPhysical and Theoretical Chemistry010306 general physicsSpectroscopyPhysicsIsotope010308 nuclear & particles physicsatomic masspenning trapCondensed Matter PhysicsPenning trapAtomic and Molecular Physics and OpticsAtomic massNuclear binding energyisomersydinfysiikkaHyperfine Interactions
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