Abstract
The thermal neutron capture cross section {sigma}{sub 0} and Resonance integral I{sub 0} of {sup 241}Am leading to the production of {sup 242m}Am and {sup 242g}Am were measured by radiochemical method. The cross sections obtained in this study are {sigma}{sub 0}=60.9 {+-} 2.6 barn, I{sub 0}=213 {+-} 13 barn for {sup 241}Am(n,{gamma}){sup 242m}Am and {sigma}{sub 0}=736 {+-} 31 barn, I{sub 0}=1684 {+-} 92 barn for {sup 241}Am(n,{gamma}){sup 242g}Am. (author)
Shinohara, N;
Hatsukawa, Y;
Hata, K;
Kohno, N
[1]
- Japan Atomic Energy Research Inst., Tokai, Ibaraki (Japan). Tokai Research Establishment
Citation Formats
Shinohara, N, Hatsukawa, Y, Hata, K, and Kohno, N.
Radiochemical determination of the neutron capture cross sections of {sup 241}Am irradiated in the JMTR reactor.
Japan: N. p.,
1997.
Web.
Shinohara, N, Hatsukawa, Y, Hata, K, & Kohno, N.
Radiochemical determination of the neutron capture cross sections of {sup 241}Am irradiated in the JMTR reactor.
Japan.
Shinohara, N, Hatsukawa, Y, Hata, K, and Kohno, N.
1997.
"Radiochemical determination of the neutron capture cross sections of {sup 241}Am irradiated in the JMTR reactor."
Japan.
@misc{etde_530410,
title = {Radiochemical determination of the neutron capture cross sections of {sup 241}Am irradiated in the JMTR reactor}
author = {Shinohara, N, Hatsukawa, Y, Hata, K, and Kohno, N}
abstractNote = {The thermal neutron capture cross section {sigma}{sub 0} and Resonance integral I{sub 0} of {sup 241}Am leading to the production of {sup 242m}Am and {sup 242g}Am were measured by radiochemical method. The cross sections obtained in this study are {sigma}{sub 0}=60.9 {+-} 2.6 barn, I{sub 0}=213 {+-} 13 barn for {sup 241}Am(n,{gamma}){sup 242m}Am and {sigma}{sub 0}=736 {+-} 31 barn, I{sub 0}=1684 {+-} 92 barn for {sup 241}Am(n,{gamma}){sup 242g}Am. (author)}
place = {Japan}
year = {1997}
month = {Mar}
}
title = {Radiochemical determination of the neutron capture cross sections of {sup 241}Am irradiated in the JMTR reactor}
author = {Shinohara, N, Hatsukawa, Y, Hata, K, and Kohno, N}
abstractNote = {The thermal neutron capture cross section {sigma}{sub 0} and Resonance integral I{sub 0} of {sup 241}Am leading to the production of {sup 242m}Am and {sup 242g}Am were measured by radiochemical method. The cross sections obtained in this study are {sigma}{sub 0}=60.9 {+-} 2.6 barn, I{sub 0}=213 {+-} 13 barn for {sup 241}Am(n,{gamma}){sup 242m}Am and {sigma}{sub 0}=736 {+-} 31 barn, I{sub 0}=1684 {+-} 92 barn for {sup 241}Am(n,{gamma}){sup 242g}Am. (author)}
place = {Japan}
year = {1997}
month = {Mar}
}