Search results for "nuclide"

showing 10 items of 397 documents

A position sensitive β−γ coincidence technique for sample analysis with the upgraded PANDA device

2020

Abstract PANDA (Particles And Non-Destructive Analysis) is measuring system developed for non-destructive analysis of samples for safety, security and safeguards. The capabilities of the PANDA device were expanded by the addition of a thick silicon detector for β particle detection. The upgraded device can now be used for position-sensitive α − γ and β − γ coincidence measurements of various kinds of radioactive samples. The capability of the PANDA device in using the β − γ coincidence technique was tested using a mixed source of 134Cs and 226Ra. In addition, the ability of PANDA to locate nuclides emitting β particles from samples was tested using a combined sample containing a mixed 134Cs…

PhysicsNuclear and High Energy Physicsbusiness.industry010501 environmental sciences01 natural sciencesSample (graphics)Coincidence030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineOpticsPosition (vector)Silicon detectorParticleNuclidebusinessInstrumentation0105 earth and related environmental sciencesNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Spectroscopy at the two-proton drip line: Excited states in 158W

2017

Abstract Excited states have been identified in the heaviest known even-Z N = 84 isotone 158W, which lies in a region of one-proton emitters and the two-proton drip line. The observation of γ-ray transitions feeding the ground state establishes the excitation energy of the yrast 6+ state confirming the spin-gap nature of the α-decaying 8+ isomer. The 8+ isomer is also expected to be unbound to two-proton emission but no evidence for this decay mode was observed. An upper limit for the two-proton decay branch has been deduced as b 2 p ≤ 0.17% at the 90% confidence level. The possibility of observing two-proton emission from multiparticle isomers in nearby nuclides is considered.

PhysicsNuclear and High Energy Physicsproton radioactivityProtonta114010308 nuclear & particles physicsYrastNuclear Theory01 natural scienceslcsh:QC1-999Excited state0103 physical sciencesNuclideAtomic physics010306 general physicsSpectroscopyGround stateNuclear Experimentmultiparticle excited stateslcsh:PhysicsExcitationLine (formation)Physics Letters B
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High-accuracy mass spectrometry with stored ions

2006

Abstract Like few other parameters, the mass of an atom, and its inherent connection with the atomic and nuclear binding energy is a fundamental property, a unique fingerprint of the atomic nucleus. Each nuclide comes with its own mass value different from all others. For short-lived exotic atomic nuclei the importance of its mass ranges from the verification of nuclear models to a test of the Standard Model, in particular with regard to the weak interaction and the unitarity of the Cabibbo–Kobayashi–Maskawa quark mixing matrix. In addition, accurate mass values are important for a variety of applications that extend beyond nuclear physics. Mass measurements on stable atoms now reach a rela…

PhysicsNuclear physicsAtomic nucleusAtomGeneral Physics and AstronomyNuclear binding energyPhysics::Atomic PhysicsNuclideMass spectrometryPenning trapISOLTRAPAtomic massPhysics Reports
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Studying exotic nuclides close to the N = Z line at the HIGISOL facility

2003

The ion guide [1, 2] for heavy-ion fusion-evaporation reactions (HIGISOL) which was developed by Beraud et al. [3] has been implemented at the IGISOL facility in Jyvaskyla [4]. This system was modified over the past 5 years. Figure 1 shows the present set-up. The HIGISOL takes advantage of the different angular distributions of primary beam and reaction products: the primary beam is stopped in front of the stopping chamber and the reaction products enter the stopping chamber through a thin foil passing the beam stop. This so called “shadow” method removes the plasma effect since the primary beam is not ionising the stopping gas. In order to improve ion optical properties, mainly to reduce t…

PhysicsNuclear physicsDc voltageIon beamPlasma effectSkimmer (machine)NuclideBeam (structure)Line (formation)Ion
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Efficiency calibration of a Ge(Li) detector by absolute counting of fallout nuclides by means of the 4πβ-γ coincidence method

1975

Abstract The 4 π β - γ coincidence method proves to be very suitable for absolute counting of fallout nuclides. Using such nuclides, absolute calibration of a Ge(Li) detector was carried out for different geometry positions.

PhysicsNuclear physicsIsotopeCalibration (statistics)DetectorBeta particleGeneral MedicineNuclideCoincidenceAbsolute calibrationNuclear Instruments and Methods
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Quenching of the SnSbTe Cycle in therpProcess

2009

The nuclides 104-108Sn, 106-110Sb, 108,109Te, and 111I at the expected endpoint of the astrophysical rp process have been produced in 58Ni+natNi fusion-evaporation reactions at IGISOL and their mass values were precisely measured with the JYFLTRAP Penning trap mass spectrometer. For 106Sb, 108Sb, and 110Sb these are the first direct experimental mass results obtained. The related one-proton separation energies have been derived and the value for 106Sb, Sp=424(8) keV, shows that the branching into the closed SnSbTe cycle in the astrophysical rp process is weaker than expected.

PhysicsNuclear physicsIsotopeSpectrometerBranching fractionGeneral Physics and AstronomyNucliderp-processNucleonMass spectrometryPenning trapPhysical Review Letters
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Mass Measurements and Implications for the Energy of the High-Spin Isomer inAg94

2008

Nuclides in the vicinity of {sup 94}Ag have been studied with the Penning trap mass spectrometer JYFLTRAP at the Ion-Guide Isotope Separator On-Line. The masses of the two-proton-decay daughter {sup 92}Rh and the beta-decay daughter {sup 94}Pd of the high-spin isomer in {sup 94}Ag have been measured, and the masses of {sup 93}Pd and {sup 94}Ag have been deduced. When combined with the data from the one-proton- or two-proton-decay experiments, the results lead to contradictory mass excess values for the high-spin isomer in {sup 94}Ag, -46 370(170) or -44 970(100) keV, corresponding to excitation energies of 6960(400) or 8360(370) keV, respectively.

PhysicsNuclear physicsMass excessIsotopeAnalytical chemistryGeneral Physics and AstronomyNuclideSpin (physics)Penning trapMass spectrometryBeta decayExcitationPhysical Review Letters
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The new nuclide225U

1989

In the bombardment of a 270μg/cm 2 180Hf target with48 Ca projectiles at a primary beam energy of E/A=4.24 MeV/u the new nuclide225U was produced. The experiment was performed at the velocity filter SHIP. 225U was found to decay by α emission with Eα=(7880 ±20) keV (≈90%), (7830±20) keV (≈10%) and has a half-life ofT 1/2=(80 −20 +40 ms).

PhysicsNuclear physicsNuclear and High Energy Physics010308 nuclear & particles physicsProjectileFilter (video)0103 physical sciencesNuclear fusionNuclide010306 general physics7. Clean energy01 natural sciencesBeam energyZeitschrift f�r Physik A Atomic Nuclei
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Nuclear levels in proton-unboundI109: Relative single-particle energies beyond the proton drip line

2007

A level scheme has been constructed for the proton-unbound, T-z=3/2 nuclide I-109(53)56 following a recoil-decay-tagging experiment using the Ni-58(Fe-54, p2n gamma) reaction at a beam energy of 19 ...

PhysicsNuclear physicsNuclear and High Energy PhysicsIsotopeProtonNuclear structureGamma spectroscopyNuclideNuclear ExperimentSpectroscopyRadioactive decayLine (formation)Physical Review C
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Shape-changing particle decays ofBi185and structure of the lightest odd-mass Bi isotopes

2004

Proton and alpha decay of the proton-rich nuclide Bi-185 has been restudied in more detail in the complete fusion reaction Nb-93(Mo-95, 3n)Bi-185 at the velocity filter SHIP. The observed decay pat ...

PhysicsNuclear physicsNuclear and High Energy PhysicsIsotopeProtonProton decayNuclear fusionParticleNuclideAlpha decayAtomic physicsSpectroscopyPhysical Review C
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