GAMMA TRANSITIONS BETWEEN EVEN-PARITY STATES IN 16O

1965 ◽  
Vol 43 (11) ◽  
pp. 2045-2051 ◽  
Author(s):  
S. Fujii ◽  
M. E. Rose

The large transition rates in the rotational band based on the 0+ state at 6.05 MeV in 16O are studied using Eisenberg, Spicer, and Rose's model for the even-parity states. The transition rates from low-lying 4+ states to low-lying 2+ states and from these 2+ states to the first excited 0+ state are calculated. The calculated values are much smaller than the experimental ones.

1976 ◽  
Vol 29 (3) ◽  
pp. 139 ◽  
Author(s):  
D Branford ◽  
LE Carlson ◽  
FCP Huang ◽  
N Gardner ◽  
TR Ophel ◽  
...  

A search is described for an excited Kn = 0+ rotational band based on the 6� 44 MeV level of 24Mg. Mean nuclear lifetimes have been measured by the Doppler shift attenuation method using the 12C('60,a)24Mg reaction and the results are 't'm = 66�29, 28�7 and 13�3 fs for levels at 6'44, 8�65 and 10� 58 MeV respectively. The absolute transition rates found for the y decays from the 6�44 and 8�65 MeV levels are in good agreement with the results of shell model calculations if it is assumed that these levels are the 0+ and 2 + members respectively of the excited Kn = 0+ rotational band. Based on this assumption, a result Qoo = 0�48 �0�08b is obtained for the intraband quadrupole moment. From a study of the 23Na(p, y) reaction, it is established that the J = 4 levels at 12� 63 and 13�05 MeV do not decay by enhanced E2 transitions to the 8� 65 MeV level. This suggests that neither of these levels is the 4 + member of the excited Kn = 0+ rotational band. An assignment of J" = 4+ is made to one member of the doublet at 10�58 MeV.


1960 ◽  
Vol 38 (2) ◽  
pp. 262-271 ◽  
Author(s):  
M. A. Clark

K-conversion coefficients for gamma transitions in Dy160 have been measured and the transition multipolarities determined as follows (Eγ, αK, multipolarity): 86.7 kev, 1.5 (E2); 197 kev, 1.6 × 10−1 (E2); 216 kev, 4.0 × 10−2 (E1); 299 kev, 1.3 × 10−2 (E1); 880 kev, 3.1 × 10−3 (E2); (962 + 966) kev, 2.5 × 10−3 (E2); 1179 kev, 6.6 × 10−4 (E1); 1205 kev, 4.6 × 10−4 (E1); 1273 kev, 6.1 × 10−4 (E1); 1315 kev, 3.9 × 10−4 (E1), Relative transition intensities are compared with the predictions of the Unified Model of Bohr and Mottelson and the asymmetric rotor theory of Davydov and Filippov. Transition intensities from the 966-kev level to members of the ground state rotational band suggest the asymmetric rotor interpretation.


1971 ◽  
Vol 49 (19) ◽  
pp. 2462-2495 ◽  
Author(s):  
J. Barrette ◽  
M. Barrette ◽  
A. Boutard ◽  
G. Lamoureux ◽  
S. Monaro ◽  
...  

The γ rays emitted in the decay of the 152Eum,g isomeric pair have been studied with the use of high-efficiency, high-resolution, solid-state detectors. These measurements together with Ge(Li)–Ge(Li) coincidence experiments revealed the existence of several new gamma transitions never previously reported. In all, 93 and 30 γ rays were observed in the decay of 152Eug and 152Eum, respectively. Calculations of the β- and γ-band mixing into the ground-state rotational band and into each other were carried out. These calculations showed that this mixing is insufficient in explaining the B(E2) ratios from the members of both the β and γ band. In addition, the very likely existence of a Kπ = 2− band in 152Sm, with levels at 1649.90 (2−) and 1757.0 keV (3−), has been unveiled in these measurements. Furthermore, the existence of a new Kπ = 0− octupole rotational band (levels at 1680.58 (1−) and 1730.3 (3−)) built on the β-vibrational band and the presence of a collective Kπ = 2+ vibrational state at 1769.1 keV, which most probably can be described as a coupled (βγ) two phonon state, are also proposed. Moreover, a new level at 1292.75 keV has been established through coincidence experiments in 152Sm. This level may be considered either as the 2+ member of a second β-vibrational band or, more likely, can be described as a truly spherical state in light of recent experiments involving (t,p) and (p,t) transfer reactions to levels of 152Sm. Finally, a qualitative analysis of the level structure of 152Gd, as well as 150Sm, seems to show that these two nuclei display a more rotational nature than a spherical (or vibrational) one as previously suggested.


1971 ◽  
Vol 32 (C6) ◽  
pp. C6-289-C6-290
Author(s):  
P. THIEBERGER ◽  
A. W. SUNYAR ◽  
P. C. ROGERS ◽  
N. LARK ◽  
O. C. KISTNER ◽  
...  
Keyword(s):  

2021 ◽  
Vol 155 (3) ◽  
pp. 034105
Author(s):  
Taha Selim ◽  
Arthur Christianen ◽  
Ad van der Avoird ◽  
Gerrit C. Groenenboom

Aquaculture ◽  
2021 ◽  
Vol 541 ◽  
pp. 736825
Author(s):  
Jonathan S.F. Lee ◽  
Melissa L. Pierce ◽  
Rachel S. Poretsky ◽  
Matthew A. Cook ◽  
Barry A. Berejikian ◽  
...  

2021 ◽  
pp. 096228022199750
Author(s):  
Zvifadzo Matsena Zingoni ◽  
Tobias F Chirwa ◽  
Jim Todd ◽  
Eustasius Musenge

There are numerous fields of science in which multistate models are used, including biomedical research and health economics. In biomedical studies, these stochastic continuous-time models are used to describe the time-to-event life history of an individual through a flexible framework for longitudinal data. The multistate framework can describe more than one possible time-to-event outcome for a single individual. The standard estimation quantities in multistate models are transition probabilities and transition rates which can be mapped through the Kolmogorov-Chapman forward equations from the Bayesian estimation perspective. Most multistate models assume the Markov property and time homogeneity; however, if these assumptions are violated, an extension to non-Markovian and time-varying transition rates is possible. This manuscript extends reviews in various types of multistate models, assumptions, methods of estimation and data features compatible with fitting multistate models. We highlight the contrast between the frequentist (maximum likelihood estimation) and the Bayesian estimation approaches in the multistate modeling framework and point out where the latter is advantageous. A partially observed and aggregated dataset from the Zimbabwe national ART program was used to illustrate the use of Kolmogorov-Chapman forward equations. The transition rates from a three-stage reversible multistate model based on viral load measurements in WinBUGS were reported.


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