P. A. Wilmarth
Lawrence Berkeley National Laboratory
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Featured researches published by P. A. Wilmarth.
Physics Letters B | 1986
K.S. Tothy; Y. A. Ellis-Akovali; J. M. Nitschke; P. A. Wilmarth; P.K. Lemmertz; D.M. Moltz; Frank T. Avignone
Abstract Intense peaks, superposed on a structureless spectrum, were observed in 151Yb β-delayed proton decay. It is shown that the peak and statistical protons follow the decay of the s 1 2 groundand h 11 2 isomeric states in 151Yb, respectively. It is concluded that the peaks, also seen in 147Dy and 149Er decays, are due to a low density of 1 2 and 3 2 levels at ≈ 4.5 MeV in the N = 82 daughters.
European Physical Journal A | 1991
K. S. Toth; K. S. Vierinen; J. M. Nitschke; P. A. Wilmarth; R. M. Chasteler
Using an on-line mass separator, the α-particle decays of155Lu and157Lu were investigated. A new α-emitting level in157Lu was identified [T1/2=5.7(5) s,Eβ=4924(20) keV]. In addition, a half-life of 140(20) ms was measured for the recently discovered second, low-lying, α-decaying level [Eβ=5579 (5)keV] in155Lu.
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1991
K. S. Toth; J. M. Nitschke; K. S. Vierinen; P. A. Wilmarth; R. B. Firestone; M. O. Kortelahti
Abstract The isotope separator facility OASIS, on-line at the Lawrence Berkeley Laboratory Super-HILAC, was used to investigate proton-rich rare earth nuclei. Single-particle states near the 82-neutron shell were delineated, numerous new isotopes, isomers and β-delayed proton emitters were discovered and the α-decay properties of some nuclides with N ⩾ 84 were re-examined. In this contribution the experimental program is summarized briefly, the excitation energies of the s 1 2 and h 11 2 proton states in this mass region are discussed, and results on the β-delayed-proton spectra of 145Dy and 147Er are presented.
Archive | 1990
R. B. Firestone; J. M. Nitschke; P. A. Wilmarth; K. S. Vierinen; R. M. Chasteler; J. Gilat; A. A. Shihab-Eldin
The decays of rare-earth nuclei in the region near N = 82 and Z = 64 and extending toward the proton drip line have been studied with the OASIS mass-separation facility on-line at the Lawrence Berkeley Laboratory SuperHILAC. Spectra of x rays, γ rays, and β-delayed protons and a particles have been measured in both singles and coincidence modes. Decay schemes have been derived, in many instances, with absolute branching intensities for electron capture, positron emission, and β-delayed particle decay. In favorable cases, Q(EC) values have been determined from the measured electron-capture and positron-decay branchings. Nuclear structure near the closed shells has been qualitatively explained by a simple weak-coupling model, and the disappearance of Z = 64 shell effects near N = 78 has been explored. The systematics of Gamow-Teller spin-flip transitions have been investigated and will be compared with shell-model predictions.
Physical Review C | 1989
J. Gilat; J. M. Nitschke; P. A. Wilmarth; R. B. Firestone
The {beta}/{gamma} and delayed proton decays of mass separated {ital A}=141 isotopes with {ital Z}=63--66 were investigated with an on-line mass separator. Branching ratios have been redetermined for the total {beta} decay of the 2.7(3) s, (11/2){sup {minus}} isomer {sup 141}Eu{sup {ital m}} at 96.5 keV (13{sub {minus}2}{sup +4}%), and for the direct {beta} feeding of the 1.58 keV (3/2){sup +} level of {sup 141}Sm in the decay of 40-s {sup 141}Eu{sup {ital g}} (73(5)%). Detailed decay schemes have been constructed for the decays of the (11/2){sup {minus}} isomer {sup 141}Gd{sup {ital m}} (11(2)% isomeric transition) and the (1/2){sup +} ground state, {sup 141}Gd{sup {ital g}}. Half-lives of 24.5(5) s and 14(4) s, respectively, have been determined for these isomers. A delayed proton branch of 0.03(1)% was identified in the decay of {sup 141}Gd{sup {ital g}}. A detailed decay scheme was also constructed for 3.5(2)-s {sup 141}Tb and a {ital J}{sup {pi}}=(5/2{sup {minus}} ) was assigned to its ground state, at variance with the systematics of heavier, odd-mass Tb isotopes. All {gamma}-ray assignments to the various isotopes are based on {ital x}{gamma} and {gamma}{gamma} coincidences and on half-life measurements. A 0.9(2)-s half-life for {sup 141}Dy was determined from its delayedmorexa0» proton decay. All spin assignments proposed in this paper are discussed in terms of Nilsson level diagrams and nuclear shapes.«xa0less
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1989
K. S. Toth; Y.A. Akovali; H.J. Kim; J. M. Nitschke; P. A. Wilmarth; D.M. Moltz
Abstract We have been involved in the investigation of nuclear structure properties of nuclei close to the proton drip line. In these studies we have used on-line isotope separators at Oak Ridge (UNISOR) and Berkeley (OASIS), the ORNL velocity filter, and a fast helium-gas-jet transport system at the LBL 88-in. cyclotron. We describe briefly three areas of our research that have dealt with particle decays: (1) α-decay in medium-weight nuclei, (2) α-decay rates for even-even isotopes, and (3) s-delayed-proton decay of N = 81 precursors.
European Physical Journal A | 1989
J. M. Nitschke; K. S. Toth; K. S. Vierinen; P. A. Wilmarth; R. M. Chasteler
Using an on-line mass separator the decay of153Lu was studied in64Zn bombardments of92Mo. The T1/2=0.9 ±0.2 s activity was assigned to the β decay of the (11/2−) isomer.
European Physical Journal A | 1989
R. M. Chasteler; J. M. Nitschke; R. B. Firestone; K. S. Vierinen; P. A. Wilmarth; A. A. Shihab-Eldin
The heaviest known erbium isotope, 3.3(2) min.174Er, has been identified using on- line isotope separation and by ß and γ- ray spectroscopy. Twelve γ rays were placed in a preliminary decay scheme. The mass of the new isotope was established by the separator and the Z was deduced from Tm K x ray coincident ß and γ rays. In addition, the heaviest known isotope of holmium171Ho was observed with a half-life of 49(5) s.
Physical Review C | 1988
K. S. Vierinen; A. A. Shihab-Eldin; J. M. Nitschke; P. A. Wilmarth; R. M. Chasteler; R. B. Firestone; K. S. Toth
Using mass-separated sources, the ..beta..-decay properties of /sup 154/Lu and /sup 154/Yb were investigated. Limits of /sup 154/Lu decay to the first 8/sup +/ and 6/sup +/ levels in /sup 154/Yb suggest a 7/sup +/ spin for the odd-odd parent; also delayed proton emission and an indication of delayed ..cap alpha..-particle emission were observed to follow /sup 154/Lu ..beta.. decay. The ..beta..-decay branch of the ..cap alpha..-emitting nucleus /sup 154/Yb was identified for the first time by the observation of one intense 133.2-keV ..gamma.. ray. This transition deexcites a 1/sup +/ 133.2-keV level in /sup 154/Tm which is fed by an allowed 0/sup +/..-->..1/sup +/..beta.. transition with a logft value of 3.6 +- 0.3.
Physical Review C | 1988
K. S. Vierinen; A. A. Shihab-Eldin; J. M. Nitschke; P. A. Wilmarth; R. M. Chasteler; R. B. Firestone; K. S. Toth
Using mass-separated sources, the ..beta..-decay properties of /sup 154/Lu and /sup 154/Yb were investigated. Limits of /sup 154/Lu decay to the first 8/sup +/ and 6/sup +/ levels in /sup 154/Yb suggest a 7/sup +/ spin for the odd-odd parent; also delayed proton emission and an indication of delayed ..cap alpha..-particle emission were observed to follow /sup 154/Lu ..beta.. decay. The ..beta..-decay branch of the ..cap alpha..-emitting nucleus /sup 154/Yb was identified for the first time by the observation of one intense 133.2-keV ..gamma.. ray. This transition deexcites a 1/sup +/ 133.2-keV level in /sup 154/Tm which is fed by an allowed 0/sup +/..-->..1/sup +/..beta.. transition with a logft value of 3.6 +- 0.3.