Search for cluster structure of excited states in 14 C

2004 ◽  
Vol 21 (2) ◽  
pp. 193-215 ◽  
Author(s):  
W. von Oertzen ◽  
H. G. Bohlen ◽  
M. Milin ◽  
Tz Kokalova ◽  
S. Thummerer ◽  
...  
2019 ◽  
Vol 50 (5) ◽  
pp. 605-607
Author(s):  
A. A. Kasparov ◽  
E. S. Konobeevski ◽  
S. V. Zuyev ◽  
M. V. Morodvskoy ◽  
A. A. Afonin ◽  
...  

2006 ◽  
Vol 21 (31n33) ◽  
pp. 2403-2409
Author(s):  
Yoshiko Kanada-En'yo

Structures of excited states in 11 C and 11 B were studied based on variational calculations after spin-parity projection in a framework of antisymmetrized molecular dynamics (AMD). The calculations systematically reproduce experimental data of the transition strengths such as Gamov-Teller(GT) and M1 transitions. A well-developed cluster structure of 2α+3 He (t) was found in the [Formula: see text] state of 11 C (11 B ). We assigned this state to the observed [Formula: see text] state at 8 MeV. The calculations reproduce the small [Formula: see text] which has been measured in the recent experiments. It was found that the [Formula: see text] state has a dilute cluster state, and its features are similar to those of the [Formula: see text] which is considered to be a gas state of three α clusters.


2003 ◽  
Vol 18 (02n06) ◽  
pp. 170-173
Author(s):  
Y. FUNAKI ◽  
H. HORIUCHI ◽  
A. TOHSAKI ◽  
P. SCHUCK ◽  
G. RÖPKE

In order to study non-zero spin excitations of the recently proposed α-cluster condensation in the self-conjugate 4n nuclei, spatial deformation is introduced into the model wave function of the α-cluster condensate. The rotational band states of 8 Be are investigated as a first step of a test case for the study of the deformation of the α-cluster condensate. Calculations reproduce well the binding energy of the 0+ ground state and also the excitation energy of the 2+ state. Our 0+ wave function is found to be exactly equal to the 0+ wave function obtained by the generator coordinate method using Brink's 2α wave function. The study shows that both the 0+ ground and 2+ excited states can be considered as having a gas-like (i.e. weakly bound) 2α-cluster structure.


2008 ◽  
Vol 17 (10) ◽  
pp. 2336-2344 ◽  
Author(s):  
YOSHIKO KANADA-EN'YO ◽  
MASAAKI KIMURA ◽  
YASUTAKA TANIGUCHI ◽  
TADAHIRO SUHARA

We report three-center cluster structures in the excited states of 11 B (11 C ), 8 He and 14 C based on theoretical calculations with the antisymmetrized molecular dynamics (AMD). In particular we discuss the cluster gas-like states 2α + t(2α+3 He ) in 11 B (11 C ) and α + 2n + 2n in 8 He . In 14 C , the 3α linear-chain structure is discussed.


Author(s):  
M. A. Zhusupov ◽  
K. A. Zhaksybekova ◽  
R. S. Kabatayeva ◽  
A. S. Kopenbayeva

2010 ◽  
Vol 25 (21n23) ◽  
pp. 1858-1861 ◽  
Author(s):  
A. SAITO ◽  
S. SHIMOURA ◽  
T. MINEMURA ◽  
Y. U. MATSUYAMA ◽  
H. BABA ◽  
...  

Cluster structures in the neutron-rich nucleus 12 Be were experimentally investigated via α-inelastic scattering. Excited states in the 12 Be nucleus were populated by a 12 Be (αα') reaction at 60 A MeV in the inverse kinematics, and identified by measuring a 6 He +6 He and α+8 He breakup channels in coincidence. The differential cross section and the angular correlations between the decay particles were obtained for each excitation energy at 10–20 MeV for 6 He +6 He and at 9–19 MeV for α+8 He , respectively, reconstructed by the measured momentum vectors of the two helium isotopes. A multipole decomposition analysis based on the distorted-wave Born approximation was applied for the angular distribution of the inelastic scattering together with the angular correlation between the decay particles with respect to the directions of the incident beam and to the momentum transfer simultaneously. From the decomposed excitation energy spectra for J=0-4, several new excited states were identified. The 0+ excited states were candidates of the band-head of a largely deformed rotational band. The 11.3-MeV 0+ state was found to decay only into the 6 He +6 He channel. This result support the recent theoretical result by the generalized two-center cluster model. Several negative-parity excited states were observed in the α+8 He channel. These excited states possibly forming a negative-parity rotational band, which is very closed to the positive-parity band, can be connected to the existence of the extremely developed cluster structure in 12 Be .


2006 ◽  
Vol 15 (07) ◽  
pp. 1541-1548
Author(s):  
YOSHIKO KANADA-EN'YO ◽  
MASAAKI KIMURA

Structures of excited states in 11 C and 11 B were studied based on variational calculations after spin-parity projection in a framework of antisymmetrized molecular dynamics (AMD). The calculations systematically reproduce the experimental data of the transition strengths such as Gamov-Teller and M1 transitions. A well-developed cluster structure of 2α+3 He (t) was found in the [Formula: see text] state of 11 C (11 B ), which can be assigned to the observed [Formula: see text] state at 8 MeV. The calculations reproduce the small [Formula: see text] measured in the recent experiments. It was suggested that the [Formula: see text] state has a dilute cluster state, and its features are similar to those of the [Formula: see text] which is considered to be a gas state of three α clusters. The structures of 13 C were also discussed.


2006 ◽  
Vol 21 (31n33) ◽  
pp. 2383-2392 ◽  
Author(s):  
T. Kawabata ◽  
H. Akimune ◽  
H. Fujita ◽  
M. Fujiwara ◽  
K. Hara ◽  
...  

The cluster structures of the excited states in 11 B are studied by analyzing the isoscalar monopole and quadrupole strengths in the 11 B (d,d′) reaction at Ed = 200 MeV . The excitation strengths are compared with the predictions by the shell-model and antisymmetrized molecular-dynamics (AMD) calculations. It is found that the large monopole strength for the [Formula: see text] state at Ex = 8.56 MeV is well described by the AMD calculation and is an evidence for a developed 2α + t cluster structure.


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