Abstract
We study static non-axial octupole deformations in proton-rich Z=N nuclei, {sup 64}Ge, {sup 68}Se, {sup 72}Kr, {sup 76}Sr, {sup 80}Zr and {sup 84}Mo, by using the Skyrme Hartree-Fock plus BCS method with no restrictions on the nuclear shape. The calculation predicts that the oblate ground state in {sup 68}Se is extremely soft for the Y{sub 33} triangular deformation, and that in {sup 80}Zr the low-lying local minimum state coexisting with the prolate ground state has the Y{sub 32} tetrahedral deformation. (author)
Citation Formats
Takami, Satoshi, Yabana, K, and Matsuo, M.
Exotic octupole deformation in proton-rich Z=N nuclei.
Japan: N. p.,
1998.
Web.
Takami, Satoshi, Yabana, K, & Matsuo, M.
Exotic octupole deformation in proton-rich Z=N nuclei.
Japan.
Takami, Satoshi, Yabana, K, and Matsuo, M.
1998.
"Exotic octupole deformation in proton-rich Z=N nuclei."
Japan.
@misc{etde_630018,
title = {Exotic octupole deformation in proton-rich Z=N nuclei}
author = {Takami, Satoshi, Yabana, K, and Matsuo, M}
abstractNote = {We study static non-axial octupole deformations in proton-rich Z=N nuclei, {sup 64}Ge, {sup 68}Se, {sup 72}Kr, {sup 76}Sr, {sup 80}Zr and {sup 84}Mo, by using the Skyrme Hartree-Fock plus BCS method with no restrictions on the nuclear shape. The calculation predicts that the oblate ground state in {sup 68}Se is extremely soft for the Y{sub 33} triangular deformation, and that in {sup 80}Zr the low-lying local minimum state coexisting with the prolate ground state has the Y{sub 32} tetrahedral deformation. (author)}
place = {Japan}
year = {1998}
month = {Mar}
}
title = {Exotic octupole deformation in proton-rich Z=N nuclei}
author = {Takami, Satoshi, Yabana, K, and Matsuo, M}
abstractNote = {We study static non-axial octupole deformations in proton-rich Z=N nuclei, {sup 64}Ge, {sup 68}Se, {sup 72}Kr, {sup 76}Sr, {sup 80}Zr and {sup 84}Mo, by using the Skyrme Hartree-Fock plus BCS method with no restrictions on the nuclear shape. The calculation predicts that the oblate ground state in {sup 68}Se is extremely soft for the Y{sub 33} triangular deformation, and that in {sup 80}Zr the low-lying local minimum state coexisting with the prolate ground state has the Y{sub 32} tetrahedral deformation. (author)}
place = {Japan}
year = {1998}
month = {Mar}
}