R.A. Braga
Georgia Institute of Technology
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Featured researches published by R.A. Braga.
Nuclear Physics | 1980
R.A. Braga; W.R. Western; J. Wood; R.W. Fink; R. Stone; C. R. Bingham; L. L. Riedinger
Abstract The isomeric decays of the 1 2 + shell-model intruder states in 199,201Bi have been investigated. In the case of 201Bi we show that the s 1 2 → h 9 2 isomeric transition is pure M4 within experimental error and is 2200 times slower than any other M4 transition observed in odd-mass nuclei. Its l-forbiddenness and the possibility of an E5 admixture and penetration effects are discussed.
Nuclear Instruments and Methods | 1976
H.K. Carter; E.H. Spejewski; R.L. Mlekodaj; A.G. Schmidt; F.T. Avignone; C.R. Bingham; R.A. Braga; J.D. Cole; A.V. Ramayya; J.H. Hamilton; E.L. Robinson; K.S.R. Sastry; E.F. Zganjar
Abstract The data collection system of the on-line separator at Oak Ridge (UNISOR) is described including an overview of the operation and a discussion of some new techniques. Tape transport and computer based data acquisition systems have been developed which allow several experiments to be performed simultaneously on a given mass chain and also enable experiments to be changed quickly. To make efficient use of the cyclotron beam time, methods have been developed for quickly extracting short-lived side masses from the separator. Also described are an on-line scanning Gerholm lens spectrometer, a multiple time analysis system and an angular correlation station for the tape transport.
Nuclear Physics | 1995
J.B. Breitenbach; J. Wood; M. Jarrio; R.A. Braga; J. Kormicki; P.B. Semmes
Abstract The decay of 133 Pm to 133 Nd has been studied with mass-separated sources from the UNISOR facility. Multiscaled spectra of γ-rays, X-rays, and conversion electrons, as well as γγt-, Xγt-, eγt-, and eXt-coincidences were obtained. The half life of 133 Pm was measured to be 15±3 s. A decay scheme has been constructed consisting of 51 excited states and 106 transitions in 133 Nd. Isomers decaying by M3 and E1 transitions are established in 133 Nd. The low-lying levels are discussed in terms of the particle-plus-triaxial-rotor model and the onset of deformation in the region bounded by Z ⩾ 58, N ⩽ 76.
Nuclear Physics | 1991
J.C. Griffin; R.A. Braga; R.W. Fink; J. Wood; H.K. Carter; R.L. Mlekodaj; C. R. Bingham; E. Coenen; M. Huyse; P. Van Duppen
Abstract The radioactive decay of mass-separated 3.0 m 195g Bi to 195 Pb has been studied with the UNISOR and LISOL facilities. Time-sequenced spectra of γ-rays, X-rays, and conversion electrons have been obtained, together with γγt, γXt, eγt, and eXt coincidence data. From this information, a decay scheme has been constructed consisting of 23 excited states and 34 transitions in 195 Pb. Transitions with E0 multipole admixtures, indicative of shape coexistence, have been found to de-excite positive-parity levels at 1093, 1329, and 1380 keV. The beta-decay energy of the 195 Bi ground state is deduced to be Q EC = 4800 −550 +600 keV based on the measurement of γ-ray-gated K / β + ratios. The excitation energy of the i 13 2 isomer in 195 Pb has been determined to be 203±4 keV from the α-decays of 199m,g Po.
Nuclear Physics | 1983
R.A. Braga; B.E. Gnade; R.W. Fink; H.K. Carter
The half-life of the 92− shell-model intruder-state isomer in 187Au has been measured by employing a technique in which each incoming event is tagged with a digital representation of time by means of a real-time clock. With this method we obtain a 2.3 ± 0.1 sec half-life for the h92 → d32 E3 isomeric transition resulting in a retardation of 50 relative to the Weisskopf single-particle estimate.
Nuclear Physics | 1995
J.B. Breitenbach; J. Wood; M. Jarrio; R.A. Braga; H.K. Carter; J. Kormicki; P.B. Semmes
Abstract The decay of 133m Nd (J π = 1 2 + ) and 133g Nd (J π = 7 2 + ) to 133Pr have been studied with mass-separated sources from the UNISOR facility. Multiscaled spectra of γ-rays, X-rays, and conversion electrons, as well as γγt, γXt, eγt, and eXt coincidences were obtained. A decay scheme for 133gNd has been constructed consisting of 49 excited states and 153 transitions in 133Pr. The β decay of the isomer, 133m Nd (J π = 1 2 + ) , is reported for the first time. A decay scheme has been constructed with 13 excited states and 26 transitions in 133Pr. This isomer decays predominantly by an allowed β decay to an excited state at 402.8 keV in 133Pr. The low-energy structure of 133Pr is discussed in terms of the particle-plus-triaxial-rotor model and the onset of deformation in the region bounded by Z ⩾ 58, N ⩽ 76. The π[411] 3 2 configuration is suggested as the ground state of 133Pr, and a low-lying π[413] 5 2 bandhead is also proposed.
Nuclear Physics | 1986
R.A. Braga; P.B. Semmes; W.R. Western; R.W. Fink
Abstract The decays of 201Po (9.0 min) and 201gPo (15.3 min) have been studied with mass-separated sources from the UNISOR facility. Time-sequenced spectra of γ-rays, X-rays, and conversion electrons, as well as γγt and Xγt (coincidences were obtained. A decay scheme has been constructed incorporating 93% of the decay intensity assigned to 201Bi. Levels resulting from h 9 2 , f 7 2 and i 13 2 particle states have been observed.
Nuclear Physics | 1982
Mustafa Tan; R.A. Braga; R.W. Fink; P Venugopala Rao
Abstract The L 1 subshell orbital electron capture probability P L1 in the decay of 33.4 y 207 Bi to the 2339.89 keV level in 207 Pb is measured to be 0.518 ± 0.081 (95% confidence) by a new method in which L 1 subshell characteristic X-rays in the L γ X-ray peak are observed in an X γt coincidence mode with 1770.23 keV γ-rays. The value of P L2 is 0.047 ± 0.015 (95% confidence). From these results a value of Q EC = 39 -8 +21 keV is obtained for capture transitions to the 2339.89 keV level. The absence of K-capture to this level also is established by absence of K X-rays in coincidence with 1770.23 keV γ-rays.
Nuclear Physics | 1987
P.B. Semmes; R.A. Braga; R.W. Fink; J. Wood; J.D. Cole
Abstract The radioactive decay of 7.4 min 203 At to 203 Po has been studied with mass separated sources from the UNISOR facility. Time-sequenced spectra of γ-rays. X-rays, and conversion electrons were obtained, together with γγt, γXt, e − γt, and e − Xt coincidence data. A decay scheme has been constructed that incorporates approximately 90% of the decay intensity assigned to 203 At. All excited states below 1 MeV have been assigned unique spin-parity values, and the observed level scheme can be qualitatively understood in terms of a particle-core weak coupling description. The ground-state decay energy has been deduced to be Q EC = 5.06 ± 0.20 MeV from γ-ray-gated EC/β + ratios.
Nuclear Instruments and Methods | 1979
B.E. Gnade; R.A. Braga; W.R. Western; John Wood; R.W. Fink
Abstract A new method for the evaluation of the net intensity of each component of a partially resolved multiplet in a low energy photon ( α 1 and K α 2 X-rays in coincidence with L X-rays from the decays of 10.4 h 165 Er and 4.68 y 155 Eu.