Abstract
Measurements of absolute transition probabilities in the rotational band built on the 1/2{sup +}(631) single particle state in {sup 235}U have been performed using delayed coincidence technique. The following half-lives were obtained: T{sub 1/2} (13.0 keV level) = (0.50 {+-} 0.03) nsec. T{sub 1/2} (51.7 k e V level) = (0.20 {+-} 0.02) nsec. From the deduced B(E2) and B(M1) values magnetic and electric parameters were determined which could be compared with predictions from the Nilsson model.
Citation Formats
Hoejeberg, M, and Malmskog, S G.
Transition Probabilities in the 1/2+(631) Band in {sup 235}U.
Sweden: N. p.,
1969.
Web.
Hoejeberg, M, & Malmskog, S G.
Transition Probabilities in the 1/2+(631) Band in {sup 235}U.
Sweden.
Hoejeberg, M, and Malmskog, S G.
1969.
"Transition Probabilities in the 1/2+(631) Band in {sup 235}U."
Sweden.
@misc{etde_20956182,
title = {Transition Probabilities in the 1/2+(631) Band in {sup 235}U}
author = {Hoejeberg, M, and Malmskog, S G}
abstractNote = {Measurements of absolute transition probabilities in the rotational band built on the 1/2{sup +}(631) single particle state in {sup 235}U have been performed using delayed coincidence technique. The following half-lives were obtained: T{sub 1/2} (13.0 keV level) = (0.50 {+-} 0.03) nsec. T{sub 1/2} (51.7 k e V level) = (0.20 {+-} 0.02) nsec. From the deduced B(E2) and B(M1) values magnetic and electric parameters were determined which could be compared with predictions from the Nilsson model.}
place = {Sweden}
year = {1969}
month = {Sep}
}
title = {Transition Probabilities in the 1/2+(631) Band in {sup 235}U}
author = {Hoejeberg, M, and Malmskog, S G}
abstractNote = {Measurements of absolute transition probabilities in the rotational band built on the 1/2{sup +}(631) single particle state in {sup 235}U have been performed using delayed coincidence technique. The following half-lives were obtained: T{sub 1/2} (13.0 keV level) = (0.50 {+-} 0.03) nsec. T{sub 1/2} (51.7 k e V level) = (0.20 {+-} 0.02) nsec. From the deduced B(E2) and B(M1) values magnetic and electric parameters were determined which could be compared with predictions from the Nilsson model.}
place = {Sweden}
year = {1969}
month = {Sep}
}