Search results for "decay [Higgs particle]"

showing 10 items of 254 documents

The new element 112

1996

The new element 112 was produced and identified unambiguously in an experiment at SHIP, GSI Darmstadt. Two decay chains of the isotope277112 were observed in irradiations of208Pb targets with70Zn projectiles of 344 MeV kinetic energy. The isotope decays by emission of α particles with a half-life of (240 −90 +430 )µs. Two different α energies of (11,649±20) keV and (11,454±20) keV were measured for the two observed decays. The cross-section measured in three weeks of irradiations is (1.0 −0.4 +1.8 ) pb.

PhysicsNuclear and High Energy PhysicsIsotopeProjectileNuclear fusionDecay chainAtomic physicsKinetic energyα particlesZeitschrift für Physik A Hadrons and Nuclei
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Measurement of the branching fraction for D0 → K-π+

1997

The branching fraction for D-0 --> K(-)pi(+) is measured with the statistics collected by ALEPH from 1991 to 1994. The method is based on the comparison between the rate for the reconstructed D*+ --> (D) pi(+), D-0 --> K(-)pi(+) decay chain and the rate for inclusive soft pion production at low transverse momentum with respect to the nearest jet. The result is B(D-0 --> K(-)pi(+)) = (3.90 +/- 0.09 +/- 0.12)% (C) 1997 Published by Elsevier Science B.V. RI ANTONELLI, ANTONELLA/C-6238-2011; Passalacqua, Luca/F-5127-2011; Murtas, Fabrizio/B-5729-2012; St.Denis, Richard/C-8997-2012; Sanchez, Federico/F-5809-2012; Forti, Francesco/H-3035-2011; Ferrante, Isidoro/F-1017-2012

PhysicsNuclear and High Energy PhysicsJet (fluid)010308 nuclear & particles physicsBranching fractionElectron–positron annihilationPhysics01 natural sciencesNuclear physicsALEPH ExperimentPion0103 physical sciencesTransverse momentumDecay chain010306 general physicsALEPH experiment
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The decay of $^{31}$Ar

1990

10 pages, 1 table, 4 figures.

PhysicsNuclear and High Energy PhysicsMeasured β-delayed Ep pp coinProtonBranching fractionOn-line mass separationNuclear Theory31Ar deduced decay channelsCaO targetNuclear physicsRadioactivity 31Ar(β+) [from Ca(p 3pxn) reaction]Physics::Accelerator PhysicsSurface barrier Si detectorsNuclear Physics - ExperimentLimit (mathematics)Atomic physicsNuclear ExperimentGround state
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Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry

2014

The magnetic dipole moments and changes in mean-square charge radii of the neutron-rich $^{218m,219,229,231}\text{Fr}$ isotopes were measured with the newly-installed Collinear Resonance Ionization Spectroscopy (CRIS) beam line at ISOLDE, CERN, probing the $7s~^{2}S_{1/2}$ to $8p~^{2}P_{3/2}$ atomic transition. The $\delta\langle r^{2}\rangle^{A,221}$ values for $^{218m,219}\text{Fr}$ and $^{229,231}\text{Fr}$ follow the observed increasing slope of the charge radii beyond $N~=~126$. The charge radii odd-even staggering in this neutron-rich region is discussed, showing that $^{220}\text{Fr}$ has a weakly inverted odd-even staggering while $^{228}\text{Fr}$ has normal staggering. This sugges…

PhysicsNuclear and High Energy PhysicsNUCLEAR MOMENTS 218m219229231Fr; measured hyperfine spectra isotope shifts; deduced charge radii nuclear magnetic moments nuclear g factors. Comparison with available data.Isotopemedia_common.quotation_subjectFOS: Physical scienceschemistry.chemical_elementCharge (physics)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exAsymmetryFranciumNuclear physicschemistryNuclear Experiment (nucl-ex)Atomic physicsGround stateSpin (physics)SpectroscopyNuclear ExperimentMagnetic dipoleRADIOACTIVITY 218mFr measured decay products Ea; deduced T1/2.media_common
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NUCLEAR PROPERTIES FOR ASTROPHYSICAL AND RADIOACTIVE-ION-BEAM APPLICATIONS

1997

Abstract We tabulate the ground-state odd-proton and odd-neutron spins and parities, proton and neutron pairing gaps, one- and two-neutron separation energies, quantities related to β -delayed one- and two-neutron emission probabilities, average energy and average number of emitted neutrons, β -decay energy release and half-life with respect to Gamow–Teller decay with a phenomenological treatment of first-forbidden decays, one- and two-proton separation energies, and α -decay energy release and half-life for 9318 nuclei ranging from  16O to  339136 and extending from the proton drip line to the neutron drip line. This paper is a new and improved version of Atomic Data And Nuclear Data Table…

PhysicsNuclear and High Energy PhysicsNuclear TheoryBinding energyHalf-lifeBeta decayAtomic and Molecular Physics and OpticsNuclear physicsDecay energyNeutronNuclear drip lineAlpha decayAtomic physicsNuclear ExperimentWave functionAtomic Data and Nuclear Data Tables
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High-statistics measurement of the β-delayed α spectrum of 20Na

2013

A measurement of the 20Na β-delayed alpha spectrum with a high-granularity setup has allowed the decay scheme to be revised on several points. Three new transitions of low intensity are found at low α -particle energy. An R-matrix fit of the complete spectrum gives an improved description of the decay and indicates feeding to the broad 2+ α-cluster state close to 9MeV. c Societa Italiana di Fisica / Springer-Verlag 2013

PhysicsNuclear and High Energy PhysicsParticle and Nuclear PhysicsDecay schemeNuclear Fusion010308 nuclear & particles physicsSpectrum (functional analysis)FOS: Physical sciencesAlpha (ethology)01 natural sciencesIntensity (physics)Computational physics20Na0103 physical sciencesNuclear Physics Heavy Ions HadronsBeta (velocity)Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentEnergy (signal processing)
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Neutrino Coannihilation on Dark-Matter Relics?

2006

High-energy neutrinos may resonate with relic background neutralinos to form short-lived sneutrinos. In some circumstances, the decay chain that leads back to the lightest supersymmetric particle would yield few-GeV gamma rays or charged-particle signals. Although resonant coannihilation would occur at an appreciable rate in our galaxy, the signal in any foreseeable detector is unobservably small.

PhysicsNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)Dark matterHigh Energy Physics::PhenomenologyGamma rayFOS: Physical sciencesAstrophysicsAstrophysicsLightest Supersymmetric ParticleGalaxyHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentDecay chainNeutrinoResonance effect
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Probing double beta decay by nuclear muon capture

2005

A reliable theoretical calculations on two-neutrino and neutrinoless double-beta-decay rates requires a solid description about the nuclear structure of the intermediate nuclear states. It has been suggested that the ordinary muon capture could be used to probe the structure of the intermediate states in double beta decays.

PhysicsNuclear and High Energy PhysicsParticle physicsDecay schemeIsotopes of germaniumNuclear structureBeta decayAtomic and Molecular Physics and OpticsBeta-decay stable isobarsMuon captureNuclear physicsInternal conversionDouble beta decayHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics B - Proceedings Supplements
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Q values of the 76Ge and 100Mo double-beta decays

2008

Abstract Penning trap measurements using mixed beams of 76Ge–76Se and 100Mo–100Ru have been utilized to determine the double-beta decay Q-values of 76Ge and 100Mo with uncertainties less than 200 eV. The value for 76Ge, 2039.04(16) keV is in agreement with the published SMILETRAP value, 2039.006(50) keV. The new value for 100Mo, 3034.40(17) keV is 30 times more precise than the previous literature value, sufficient for the ongoing neutrinoless double-beta decay searches in 100Mo. Moreover, the precise Q-value is used to calculate the phase-space integrals and the experimental nuclear matrix element of double-beta decay.

PhysicsNuclear and High Energy PhysicsParticle physicsDecay schemeQ valuePenning trapDouble-beta decayPenning trapQ-valueBeta decayPhase-space integralNuclear physicsNeutrino massPhase spaceDouble beta decayBeta (plasma physics)Value (mathematics)Physics Letters B
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Measurement of the mass and lifetime of the charmed strange baryon $\Xi_{c}^{+}$

1989

Abstract We have observed six unambiguous decays of the charmed strange baryon Ξc+ (or charge conjugate Ξc−) in the 230 GeV/c negative pions or kaons on a copper target at the CERN SPS using silicon microstrip detectors and charge-coupled devices for vertex reconstruction. Three of them have been reconstructed through the decay chain Ξc+ →Ξ−π+π+, Ξ− →Λ0π−, Λ0 →pπ− and the other three through the decay chain Ξc+ →Σ+K−π+ →pπ0. We present our measurements of the mass, lifetime and production cross-section of the Ξc+, as well as of the branching ration for the two decay modes.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsNuclear TheoryBaryonNuclear physicsPionHigh Energy Physics::ExperimentDecay chainNuclear ExperimentSilicon microstrip detectorsParticle Physics - Experiment
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