Abstract
The hyperradial adiabatic one-state calculation of resonant states of (dd{mu}){sup +} and (dt{mu}){sup +} below the n=2 level of muonic atoms have been performed. The results are used to produce a new classification scheme for these states. Comparing these calculation with the recent full variational calculation by S.Hara and T.Ishihara it is concluded that the classical Born-Oppenheimer classification scheme can be misleading. 11 refs.; 4 figs.; 6 tabs.
Citation Formats
Matveenko, A V.
On the classification scheme for resonant states of muonic molecules.
JINR: N. p.,
1991.
Web.
Matveenko, A V.
On the classification scheme for resonant states of muonic molecules.
JINR.
Matveenko, A V.
1991.
"On the classification scheme for resonant states of muonic molecules."
JINR.
@misc{etde_10119825,
title = {On the classification scheme for resonant states of muonic molecules}
author = {Matveenko, A V}
abstractNote = {The hyperradial adiabatic one-state calculation of resonant states of (dd{mu}){sup +} and (dt{mu}){sup +} below the n=2 level of muonic atoms have been performed. The results are used to produce a new classification scheme for these states. Comparing these calculation with the recent full variational calculation by S.Hara and T.Ishihara it is concluded that the classical Born-Oppenheimer classification scheme can be misleading. 11 refs.; 4 figs.; 6 tabs.}
place = {JINR}
year = {1991}
month = {Dec}
}
title = {On the classification scheme for resonant states of muonic molecules}
author = {Matveenko, A V}
abstractNote = {The hyperradial adiabatic one-state calculation of resonant states of (dd{mu}){sup +} and (dt{mu}){sup +} below the n=2 level of muonic atoms have been performed. The results are used to produce a new classification scheme for these states. Comparing these calculation with the recent full variational calculation by S.Hara and T.Ishihara it is concluded that the classical Born-Oppenheimer classification scheme can be misleading. 11 refs.; 4 figs.; 6 tabs.}
place = {JINR}
year = {1991}
month = {Dec}
}