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Prog. Theor. Phys. Vol. 101 No. 1 (1999) pp. 119-138
Dynamical Effects on the 9Li-n Interaction Induced by Pauli Blocking of the Jπ=0+ Pairing Correlation
Kiyoshi Katō,
Taiichi Yamada* and
Kiyomi Ikeda**
Division of Physics, Graduate School of Science, Hokkaido
University
Sapporo 060-0810, Japan
*Laboratory of Physics, Kanto Gakuin University,
Yokohama 236-8501, Japan
**Department of Physics, Niigata University, Niigata 950-2102,
Japan
and
The Institute of Physical and Chemical Research (RIKEN),
Wako 351-0198, Japan
(Received September 24, 1998)
Abstract:
The 9Li-n interaction is discussed based on the idea of the
Pauli blocking for the Jπ=0+ neutron pairing correlation
in the 9Li core due to the presence of the last valence neutron.
The present studies are developed in a framework of the microscopic
coupled-channel model for {9Li((0p3/2)4ν) + n} +
{9Li((0p3/2)2ν(0p1/2)2ν) +n} +
{9Li((0p3/2)2ν(1s0d)2ν) +n}. The channel
of the present model consists of the last valence neutron coupled
with a 9Li configurational state connected by the Jπ=0+
pairing interaction. Due to the presence of the valence neutron in the
0p1/2 orbital, the (0p3/2)2→(0p1/2)2 jump
in the 9Li core is prevented. Thus, the p1/2-orbital neutron
states experience a strong repulsive effect due to the lack of the
configuration mixing between (0p3/2)4ν and
(0p3/2)2ν(0p1/2)2ν, and its energy rises up
significantly. In contrast to this, the sd-orbital neutron
imparts a very weak effect on the configuration mixing. As a result,
the s1/2-orbital state is obtained in the
vicinity of the threshold as a bound state or virtual
resonance for the 9Li-n interaction which reproduces
1+(Sn=-0.42 MeV) and 2+(Sn=-0.82 MeV) states
consistently with experimental data observed by Bohlen et al.
The effective 9Li-n potential which has the strong parity
dependence deduced from the present coupled-channel calculation
is discussed to be very promising for studying the halo structure
of 11Li within the 9Li + n + n model.
URL :
http://ptp.ipap.jp/link?PTP/101/119/
DOI : 10.1143/PTP.101.119
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