Gamma-ray spectroscopic studies on high-spin states inAs71andAs73using heavy-ion reactions

1977 ◽  
Vol 15 (5) ◽  
pp. 1742-1757 ◽  
Author(s):  
B. Heits ◽  
H. -G. Friederichs ◽  
A. Rademacher ◽  
K. O. Zell ◽  
P. von Brentano ◽  
...  
1973 ◽  
Vol 31 (17) ◽  
pp. 1067-1070 ◽  
Author(s):  
P. Gorodetzky ◽  
J. J. Kolata ◽  
J. W. Olness ◽  
A. R. Poletti ◽  
E. K. Warburton

The Nucleus ◽  
2000 ◽  
pp. 261-262 ◽  
Author(s):  
T. Kutsarova ◽  
M.-G. Porquet ◽  
I. Deloncle ◽  
A. Minkova ◽  
E. Gueorguieva ◽  
...  

1987 ◽  
Vol 467 (2) ◽  
pp. 330-348 ◽  
Author(s):  
J. Burde ◽  
I. Labaton ◽  
V. Richter

1980 ◽  
Vol 58 (2) ◽  
pp. 174-190 ◽  
Author(s):  
H. A. Mach ◽  
M. W. Johns ◽  
J. V. Thompson

High spin states of 96Tc populated by the (α,n) reaction using alpha beams from 13 to 27 MeV have been studied. Gamma-ray energies and intensities, gamma–gamma coincidence probabilities, gamma-ray angular distributions, and electron conversion coefficients were determined at 18 MeV. In addition, some results taken at 14 MeV are reported.The high spin structure observed in this work includes the following levels: 49.3(6+), 318.8(6+), 574.7(7+), 926.9(9+), 946.5(8+), 1062.1(8+), 1138.8(8+), 1447.2(9+), 1702.8(10+), 1861.6(9+), 1922.3(11+), 2147.5(11+), 2213.5(10(+)), 2317.2(12+), 2396.8(11(+)), 2599.0((13)+), 2642.4((14)+), and 3020.1(12(+)).These experiments also clarify and extend the information obtained by previous workers. In particular, evidence is adduced for low-lying states at 0.0(7+), 34.3(4+), 45.3(5+), 120.3(3−), 177.0(5+), 226.2(2−), 227.0(4+), and 254.3(3+).The work identifies many other states of intermediate energy.Attenuation coefficients for states in 96Tc are calculated using a theoretical model.


1987 ◽  
Vol 188 (1) ◽  
pp. 25-28 ◽  
Author(s):  
C.Y. Wu ◽  
X.T. Liu ◽  
S.P. Sorensen ◽  
R.W. Kincaid ◽  
M.W. Guidry ◽  
...  

1976 ◽  
Vol 13 (3) ◽  
pp. 1180-1193 ◽  
Author(s):  
A. R. Poletti ◽  
E. K. Warburton ◽  
J. W. Olness ◽  
J. J. Kolata ◽  
Ph. Gorodetzky

1985 ◽  
pp. 405-420 ◽  
Author(s):  
Christoph LAUTERBACH ◽  
Peter BUTLER ◽  
Hans Jürgen WOLLERSHEIM

1975 ◽  
Vol 53 (13) ◽  
pp. 1229-1235 ◽  
Author(s):  
J. V. Thompson ◽  
M. W. Johns ◽  
J. C. Waddington

A study of the 148Nd(α, 2n)150Sm reaction has revealed the high spin states of a Kπ = 0− octupole band, the members of which become the yrast levels above spin 12. Gamma ray angular distributions, gamma–gamma coincidence, and conversion electron studies have established the levels of the octupole band at 1764.6(7−), 2232.1(9−), 2744.0(11−), and tentatively at 3293.0(13−) keV.


1979 ◽  
Vol 57 (3) ◽  
pp. 358-367 ◽  
Author(s):  
N. C. Singhal ◽  
M. W. Johns

High spin slates in 148Tb have been excited by means of 144Sm(6Li,2n), 144Sm(7Li,3n), and 142Nd(10B,4n) reactions and studied by γ-ray and electron measurements. Gamma-ray singles, excitation functions, angular distributions, internal conversion coefficients, and γ–γ coincidence measurements have been made. A seven-fold gamma–gamma cascade feeding the 9+ isomeric state in 148Tb and originating in a level 4137 keV above that state is strongly excited. The spin and parity assignments are made on the basis of angular distribution and internal conversion coefficients. On the basis of these measurements, the 1006 keV transition is E3 in character; the half-life of the 1006 keV (12−) level is established to be 25 ± 2 ns.These experiments also confirm the existence of a number of high spin states in 148Gd seen by earlier workers.


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