Abstract
We perform theoretical analysis on the structure and decay of a double-strangeness five-body system which consists of {sub {Lambda}{Lambda}}{sup 5}H and {sub {Xi}}{sup 5}H states. In this S=-2 five-body system the thresholds of the t{Lambda}{Lambda} channel and the {alpha}{Xi}{sup -} channel come closer with only 8.51 MeV difference. We treat both bound and resonant states of the three-body channels t{Lambda}{Lambda} and tp{Xi}{sup -} by applying a complex rotation method. It is found that there is a bound {sub {Lambda}{Lambda}}{sup 5}H state with 6.3 MeV below the threshold of t+{Lambda}+{Lambda}. In the {Xi}{sup -} channel a resonant {sub {Xi}}{sup 5}H state appears at 1.7 MeV below the threshold of {alpha}+{Xi}{sup -}. Though the existence of this state is ensured by the Coulomb interaction, it is a `halo` nuclear state rather than an atomic state as judged from its size. The conversion width of this state is 0.2 MeV which is extremely narrow. It is also found that {Xi} mixing into the {sub {Lambda}{Lambda}}{sup 5}H ground state is small with 1.0%. For the {sub {Lambda}{Lambda}}{sup 5}H state, the weak decay to the {alpha}+{Sigma}{sup -} final state produces a high mono-energetic {Sigma}{sup -} with branching ratio of 5.5%. Thus the {Sigma}{sup -} with
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Citation Formats
Myint, K S, and Akaishi, Yoshinori.
Double-strangeness five-body system.
Japan: N. p.,
1995.
Web.
Myint, K S, & Akaishi, Yoshinori.
Double-strangeness five-body system.
Japan.
Myint, K S, and Akaishi, Yoshinori.
1995.
"Double-strangeness five-body system."
Japan.
@misc{etde_109087,
title = {Double-strangeness five-body system}
author = {Myint, K S, and Akaishi, Yoshinori}
abstractNote = {We perform theoretical analysis on the structure and decay of a double-strangeness five-body system which consists of {sub {Lambda}{Lambda}}{sup 5}H and {sub {Xi}}{sup 5}H states. In this S=-2 five-body system the thresholds of the t{Lambda}{Lambda} channel and the {alpha}{Xi}{sup -} channel come closer with only 8.51 MeV difference. We treat both bound and resonant states of the three-body channels t{Lambda}{Lambda} and tp{Xi}{sup -} by applying a complex rotation method. It is found that there is a bound {sub {Lambda}{Lambda}}{sup 5}H state with 6.3 MeV below the threshold of t+{Lambda}+{Lambda}. In the {Xi}{sup -} channel a resonant {sub {Xi}}{sup 5}H state appears at 1.7 MeV below the threshold of {alpha}+{Xi}{sup -}. Though the existence of this state is ensured by the Coulomb interaction, it is a `halo` nuclear state rather than an atomic state as judged from its size. The conversion width of this state is 0.2 MeV which is extremely narrow. It is also found that {Xi} mixing into the {sub {Lambda}{Lambda}}{sup 5}H ground state is small with 1.0%. For the {sub {Lambda}{Lambda}}{sup 5}H state, the weak decay to the {alpha}+{Sigma}{sup -} final state produces a high mono-energetic {Sigma}{sup -} with branching ratio of 5.5%. Thus the {Sigma}{sup -} with discrete energy would become a clear signature of the forming of the {Lambda}{Lambda} hypernucleus. (author).}
journal = []
issue = {117}
journal type = {AC}
place = {Japan}
year = {1995}
month = {Mar}
}
title = {Double-strangeness five-body system}
author = {Myint, K S, and Akaishi, Yoshinori}
abstractNote = {We perform theoretical analysis on the structure and decay of a double-strangeness five-body system which consists of {sub {Lambda}{Lambda}}{sup 5}H and {sub {Xi}}{sup 5}H states. In this S=-2 five-body system the thresholds of the t{Lambda}{Lambda} channel and the {alpha}{Xi}{sup -} channel come closer with only 8.51 MeV difference. We treat both bound and resonant states of the three-body channels t{Lambda}{Lambda} and tp{Xi}{sup -} by applying a complex rotation method. It is found that there is a bound {sub {Lambda}{Lambda}}{sup 5}H state with 6.3 MeV below the threshold of t+{Lambda}+{Lambda}. In the {Xi}{sup -} channel a resonant {sub {Xi}}{sup 5}H state appears at 1.7 MeV below the threshold of {alpha}+{Xi}{sup -}. Though the existence of this state is ensured by the Coulomb interaction, it is a `halo` nuclear state rather than an atomic state as judged from its size. The conversion width of this state is 0.2 MeV which is extremely narrow. It is also found that {Xi} mixing into the {sub {Lambda}{Lambda}}{sup 5}H ground state is small with 1.0%. For the {sub {Lambda}{Lambda}}{sup 5}H state, the weak decay to the {alpha}+{Sigma}{sup -} final state produces a high mono-energetic {Sigma}{sup -} with branching ratio of 5.5%. Thus the {Sigma}{sup -} with discrete energy would become a clear signature of the forming of the {Lambda}{Lambda} hypernucleus. (author).}
journal = []
issue = {117}
journal type = {AC}
place = {Japan}
year = {1995}
month = {Mar}
}