Search results for "decay [Higgs particle]"

showing 10 items of 254 documents

Criteria for the Discovery of Chemical Elements

1976

The availability of suitable heavy-ion accelerators should make it possible to synthesize and identify additional heavy transuranium elements. Criteria for adequate proof that a new element has been synthesized or found in nature and identified are suggested. The basic criterion must be the proof that the atomic number of the new element is different from the atomic numbers of all previously known elements. Chemical identification constitutes an ideal proof; the procedure must be valid for application to individual atoms in an unequivocal manner. Also satisfactory is the identification of characteristic x rays in connection with the decay of the isotope of the new element. This is likely to…

MultidisciplinaryIsotopeChemistryAlpha particle010402 general chemistry01 natural sciences0104 chemical sciencesNuclear physicsParticle decay0103 physical sciencesDecay chainAlpha decayDecay product010306 general physicsTransuranium elementSpontaneous fissionScience
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Chiral restoration from pionic atoms?

2002

We evaluate widths and shifts of pionic atoms using a theoretical microscopical potential in which the pion decay constant $f_\pi$ is changed by an in--medium density dependent one ($f_\pi(\rho)$), predicted by different partial Chiral restoration calculations. We show that the results obtained for shifts and widths are worse than if this modification were not implemented. On the other hand, we argue that in microscopic many body approaches for the pion selfenergy, based on effective Lagrangians, the mechanisms responsible for the change of $f_\pi$ in the medium should be automatically incorporated. Therefore, the replacement of $f_\pi$ by $f_\pi(\rho)$ in the many body derivation of the mi…

Nuclear Theory (nucl-th)PhysicsNuclear and High Energy PhysicsParticle physicsPionNuclear TheoryDensity dependentNuclear TheoryFísicaFOS: Physical sciencesPion decay constantMany bodyPhysics Letters B
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Position sensitive plastic scintillator for beta particle detection

2022

A new segmented plastic scintillator detector Tuike has been developed for recoil-beta tagging experiments at the Accelerator Laboratory of the University of Jyväskylä. The detector consists of individual plastic scintillator bars arranged in two orthogonal layers, and the scintillation light is detected using silicon photomultipliers. Performance of the new detector was tested using fusion-evaporation reaction 40Ca(36Ar, pn)74Rb, and the results are discussed here. It was found that for beta particles seen in the main silicon detector, Tuike can tag high-energy beta particles with a 48(10)% efficiency. An energy calibration method using Compton edges of gamma ray transitions is described i…

Nuclear and High Energy Physics010308 nuclear & particles physicsPhysics::Instrumentation and Detectorsbeetasäteilyrecoil-beta taggingtutkimuslaitteet01 natural sciencesplastic scintillatorilmaisimet0103 physical sciences010306 general physicsydinfysiikkaInstrumentationdecay tagging
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Change in structure between the $I = 1/2$ states in $^{181}$Tl and $^{177,179}$Au

2018

Abstract The first accurate measurements of the α-decay branching ratio and half-life of the I π = 1 / 2 + ground state in 181Tl have been made, along with the first determination of the magnetic moments and I = 1 / 2 spin assignments of the ground states in 177,179Au. The results are discussed within the complementary systematics of the reduced α-decay widths and nuclear g factors of low-lying, I π = 1 / 2 + states in the neutron-deficient lead region. The findings shed light on the unexpected hindrance of the 1 / 2 + → 1 / 2 + , 181Tl → g 177 Aug α decay, which is explained by a mixing of π 3 s 1 / 2 and π 2 d 3 / 2 configurations in 177Aug, whilst 181Tlg remains a near-pure π 3 s 1 / 2 .…

Nuclear and High Energy PhysicsHadronNuclear physicsThallium nuclei[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences0103 physical sciencesddc:530Nuclear Physics - ExperimentLaser spectroscopy010306 general physicsSpin (physics)PhysicsMagnetic moment010308 nuclear & particles physicsBranching fractionLandé g-factorGold nucleiDecay spectroscopylcsh:QC1-9993. Good healthNuclear deformationPräzisionsexperimente - Abteilung BlaumAtomic physicsGround stateNucleonlcsh:PhysicsDimensionless quantity
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Production of refractory elements close to the Z=N line using the ion-guide technique

1998

Production of neutron-deficient isotopes of refractory elements in the A = 80-88 region was studied using the IGISOL technique and the 165 MeV Si-32 + Ni-nat reaction. Radioactive isotopes of Y through Mo could be produced up to the M-T = + 1 line. New information on the decay of the A = 82 and 85 nuclei, including a more detailed decay scheme and more accurate half-life for Y-82, was obtained. (C) 1998 Elsevier Science B.V. All rights reserved.

Nuclear and High Energy PhysicsIsotopes of germaniumAnalytical chemistryONLINE[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesY-81Isotopes of oxygenNuclear physicsIsotopes of protactinium0103 physical sciencesNEUTRON-DEFICIENT ISOTOPES010306 general physicsInstrumentationIsotopes of europiumPhysicsDecay schemeIsotope010308 nuclear & particles physicsRefractory metalsIGISOL TECHNIQUEheavy-ion fusion-evaporation reactionsBeta decayrefractory elementsbeta decayDECAY
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Lead–gold eutectic: An alternative liquid target material candidate for high power spallation neutron sources

2011

Abstract One of the main technical concerns of Megawatt-class spallation neutron sources is the removal of the heat deposited in the target station. A way to overcome it is to use targets consisting of flowing liquid metals, but the already tested materials – mercury and lead–bismuth eutectic (LBE) – are not unproblematic. We show here that another eutectic alloy containing lead and gold (LGE) could be a suitable alternative. Besides a chemical toxicity lower than mercury, this low melting-point alloy has the advantage of being solid at RT. Moreover, it combines a neutron production similar to mercury and LBE with smaller amounts of alpha-emitting nuclides, relieving safety and environmenta…

Nuclear and High Energy PhysicsMaterials science010308 nuclear & particles physicsMetallurgyAlloyRadiochemistrychemistry.chemical_elementengineering.material7. Clean energy01 natural sciencesMercury (element)Nuclear Energy and Engineeringchemistry0103 physical sciencesengineeringNeutron sourceGeneral Materials ScienceSpallationNeutronNuclideDecay heat010306 general physicsEutectic systemJournal of Nuclear Materials
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β decay studies of n-rich Cs isotopes with the ISOLDE Decay Station

2017

R. Lica et al. -- 14 pags., 7 figs., tab. -- Open Access funded by Creative Commons Atribution Licence 3.0

Nuclear and High Energy PhysicsNEUTRON-RICHnuclear deformationIsotopes of germaniumβ decayMASS[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesISOLDEBA-148Nuclear physicsLA-1480103 physical sciencesNuclear Physics - ExperimentBAND-STRUCTURESNuclear Experiment010306 general physicsPhysicsDecay schemeNUCLEIIsotope010308 nuclear & particles physicsBEAMSBeta decay3. Good healthexotic nucleiPICOSECOND LIFETIME MEASUREMENTSbeta decayAtomic physicsNuclear deformation ISOLDEExotic nucleiJournal of Physics G: Nuclear and Particle Physics
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A Precise Measurement of the Tau Lepton Lifetime

1996

The tau lepton lifetime has been measured using three different methods with the DELPHI detector. Two measurements of one-prong decays are combined, accounting for correlations, giving a result of \tau_\tau = 291.8 \pm 3.3 \mbox{ (stat.)} \pm 2.0 \mbox{(sys.) fs} while the decay length distribution of three-prong decays gives the result \tau_{\tau} = 286.7 \pm 4.9 \mbox{ (stat.)} \pm 3.3 \mbox{ (sys.) fs}. Combining the results presented here with previous DELPHI measurements, we get \tau_{\tau} = 291.4 \pm 3.0 fs and find that the ratio of the coupling constant for tau decay relative to that for muon decay is 0.990 \pm 0.009, compatible with lepton universality.

Nuclear and High Energy PhysicsParticle physicsAlephElectron–positron annihilation01 natural sciencesMeasure (mathematics)Partícules (Física nuclear)tau lepton lifetimeNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsZ-DECAYSDELPHICoupling constantPhysicsMuon010308 nuclear & particles physicsDELPHI; tau lepton lifetime; one-prong; three-prongLARGE ELECTRON POSITRON COLLIDERthree-prongYield (chemistry)PARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIone-prongDecay lengthPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica nuclearVertex detectorParticle Physics - ExperimentLepton
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Measurement ofCP-violating asymmetries inB0→(ρπ)0decays using a time-dependent Dalitz plot analysis

2012

We report on a measurement of CP-violating asymmetries (A{sub CP}) in the Cabibbo-suppressed D{sup 0} {yields} {pi}{sup +}{pi}{sup -} and D{sup 0} {yields} K{sup +}K{sup -} decays reconstructed in a data sample corresponding to 5.9 fb{sup -1} of integrated luminosity collected by the upgraded Collider Detector at Fermilab. We use the strong decay D*{sup +} {yields} D{sup 0}{pi}{sup +} to identify the flavor of the charmed meson at production and exploit CP-conserving strong c{bar c} pair-production in p{bar p} collisions. High-statistics samples of Cabibbo-favored D{sup 0} {yields} K{sup -}{pi}{sup +} decays with and without a D*{sup {+-}} tag are used to correct for instrumental effects an…

Nuclear and High Energy PhysicsParticle physicsMesonCollider physicsmedia_common.quotation_subjectElectron–positron annihilationGeneral Physics and AstronomyDalitz plotMeasure (mathematics)01 natural sciencesResonance (particle physics)Asymmetrylaw.inventionNuclear physicsParticle decaylawTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesB meson010306 general physicsCollidermedia_commonPhysicsUnitarity010308 nuclear & particles physicsDetectorB-factoryCrystallographyDecay timePair productionCP violationHigh Energy Physics::ExperimentProduction (computer science)Collider Detector at FermilabBar (unit)Physical Review D
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Three beta-decaying states in 128In and 130In resolved for the first time using Penning-trap techniques

2020

Isomeric states in 128In and 130In have been studied with the JYFLTRAP Penning trap at the IGISOL facility. By employing state-of-the-art ion manipulation techniques, three different beta-decaying states in 128In and 130In have been separated and their masses measured. JYFLTRAP was also used to select the ions of interest for identification at a post-trap decay spectroscopy station. A new beta-decaying high-spin isomer feeding the isomer in 128Sn has been discovered in 128In at 1797.6(20) keV. Shell-model calculations employing a CD-Bonn potential re-normalized with the perturbative G-matrix approach suggest this new isomer to be a 16⁺ spin-trap isomer. In 130In, the lowest-lying (10⁻) isom…

Nuclear and High Energy PhysicsPenning trapAstronomy & Astrophysics01 natural sciencesIonPhysics Particles & Fieldsbeta-decay spectroscopyIsomersShell model0103 physical sciencesPhysics::Atomic and Molecular ClustersNuclear Experiment010306 general physicsSpectroscopyCouplingPhysicsScience & TechnologyNUCLEI010308 nuclear & particles physicsPhysicsPRECISION MASS-SPECTROMETRYNuclear shell modelR-PROCESSshell modelpenning trapRAMSEY METHODPenning traplcsh:QC1-999Physics NuclearExcited stateBeta (plasma physics)Physical SciencesSHELL-MODELTRANSITION-PROBABILITIESisomersAtomic physicsBeta-decay spectroscopylcsh:PhysicsIon cyclotron resonancePhysics Letters B
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