EXOTIC CARBON SYSTEMS IN TWO-NEUTRON HALO THREE-BODY MODELS

2011 ◽  
Vol 20 (supp01) ◽  
pp. 254-262
Author(s):  
LAURO TOMIO ◽  
ANTONIO DELFINO ◽  
TOBIAS FREDERICO ◽  
M. R. HADIZADEH ◽  
M. T. YAMASHITA ◽  
...  
Keyword(s):  
Halo Nucleus ◽  
Scaling Function ◽  
Neutron Halo ◽  
Mass Ratio ◽  
Weakly Bound ◽  
Universal Scaling ◽  
Body Model ◽  
Zero Range ◽  
Three Body ◽  
Universal Scaling Function

The general properties of exotic carbon systems, considered as a core with a two-neutron (n - n) halo, are described within a renormalized zero-range three-body model. In particular, it is addressed the cases with a core of 18C and 20C. In such a three-body framework, 20C has a bound subsystem (19C), whereas 22C has a Borromean structure with all subsystems unbound. 22C is also known as the heaviest carbon halo nucleus discovered. The spatial distributions of such weakly-bound three-body systems are studied in terms of a universal scaling function, which depends on the mass ratio of the particles, as well as on the nature of the subsystems.

Nuclear structure study of two-neutron halo nucleus 19B in microscopic cluster model

2017 ◽  
Vol 32 (11) ◽  
pp. 1750065 ◽  
Author(s):  
Fitri Hakeem M. Salih ◽  
Chun Hao Lee ◽  
Shahidan Radiman ◽  
Kok Siong Khoo
Keyword(s):  
Experimental Data ◽  
Cluster Model ◽  
Halo Nucleus ◽  
Structure Study ◽  
Neutron Halo ◽  
Mean Square ◽  
Body Model ◽  
Computational Calculations ◽  
Nuclear Structure Study ◽  
Three Body

The structure nucleus [Formula: see text] is investigated in the Microscopic Cluster Model, using three-body model [Formula: see text]. This model is used to investigate neutron halo features such as binding energy of neutron valence, root-mean-square (rms) of radius and core deformation. All the features are studied in configuration-T and -Y. In this study, theoretical framework is used in the MATLAB software to run the computational calculations. The results are compared with the experimental data.

scholarly journals Impact of uncertainties of unbound 10Li on the ground state of two-neutron halo 11Li

2020 ◽  
Author(s):  
Jagit Singh ◽  
Wataru Horiuchi
Keyword(s):  
Ground State ◽  
Halo Nucleus ◽  
Transfer Reaction ◽  
Neutron Halo ◽  
Structure Model ◽  
Continuum States ◽  
Normal Core ◽  
Configuration Mixing ◽  
Three Body ◽  
Neutron Transfer Reaction

Recently, the energy spectrum of \boldsymbol{^{10}}10Li was measured upto \boldsymbol{4.6}4.6 MeV, via one-neutron transfer reaction \boldsymbol{d(^{9}\textrm{Li},~p)^{10}\textrm{Li}}𝐝(9Li,𝐩)10Li. Considering the ambiguities on the \boldsymbol{^{10}}10Li continuum spectrum with reference to new data, we report the configuration mixing in the ground state of the two-neutron halo nucleus \boldsymbol{^{11}}11Li for two different choices of the \boldsymbol{^{9}{\textrm{Li}}+n}9Li+𝐧 potential. For the present study, we employ a three-body (\boldsymbol{\textrm{core}+n+n}core+𝐧+𝐧) structure model developed for describing the two-neutron halo system by explicit coupling of unbound continuum states of the subsystem (\boldsymbol{\textrm{core}+n}core+𝐧), and discuss the two-neutron correlations in the ground state of \boldsymbol{^{11}}11Li.

scholarly journals Exploring two-neutron halo formation in the ground state of F29 within a three-body model

2020 ◽  
Vol 101 (2) ◽  
Author(s):  
Jagjit Singh ◽  
J. Casal ◽  
W. Horiuchi ◽  
L. Fortunato ◽  
A. Vitturi
Keyword(s):  
Ground State ◽  
Neutron Halo ◽  
Halo Formation ◽  
Body Model ◽  
Three Body

DINEUTRON CORRELATION IN THE GROUND STATE AND E1 EXCITATIONS OF BORROMEAN NUCLEI

2010 ◽  
Vol 25 (21n23) ◽  
pp. 1842-1845
Author(s):  
K. HAGINO ◽  
H. SAGAWA ◽  
T. OISHI
Keyword(s):  
Contact Interaction ◽  
Ground State ◽  
Energy Distributions ◽  
Weakly Bound ◽  
Density Dependent ◽  
Body Model ◽  
Dipole Excitation ◽  
Ground State Properties ◽  
Three Body

Using a three-body model with density-dependent contact interaction, we discuss the role of dineutron correlation in the ground state properties as well as in the dipole excitation of typical weakly-bound Borromean nuclei, 11 Li and 6 He . We show that, while both the nuclei manifest themselves similar strong dineutron correlations to each other in the ground state, the energy distributions for the two emitted neutrons from the dipole excitation are considerably different. We also discuss briefly the diproton correlation in a proton-rich Borromean nucleus, 17 Ne .

scholarly journals Two-neutron halo state of 15 B around 3.48 MeV by a three-body model

2018 ◽  
Vol 42 (6) ◽  
pp. 064103
Author(s):  
Dong Bai ◽  
Zhongzhou Ren ◽  
Tiekuang Dong
Keyword(s):  
Neutron Halo ◽  
Body Model ◽  
Three Body

THEORETICAL STUDY OF THE 11Li β DECAY INTO THE DEUTERON CHANNEL IN A CLUSTER MODEL

2011 ◽  
Vol 20 (04) ◽  
pp. 803-806 ◽  
Author(s):  
ERGASH M. TURSUNOV ◽  
DANIEL BAYE ◽  
PIERRE DESCOUVEMONT
Keyword(s):  
Halo Nucleus ◽  
Theoretical Study ◽  
Transition Probability ◽  
Broad Resonance ◽  
Hyperspherical Coordinates ◽  
Β Decay ◽  
Body Model ◽  
Final Channel ◽  
Three Body ◽  
Time And Energy

The β-decay process of the 11 Li halo nucleus into 9 Li and d is reanalyzed within a three-body model. The 11 Li nucleus is described as a 9 Li +n+n system in hyperspherical coordinates. The transition probability per time and energy units measured in a recent experiment can be reproduced with a broad resonance located around 0.8 MeV and a weak absorption from the 9 Li + d final channel.

Universal scaling function for domain growth in the Glauber-Ising chain

1992 ◽  
Vol 45 (14) ◽  
pp. 8131-8133 ◽  
Author(s):  
Zhifang Lin ◽  
Xiaomin Wang ◽  
Ruibao Tao
Keyword(s):  
Scaling Function ◽  
Domain Growth ◽  
Ising Chain ◽  
Universal Scaling ◽  
Universal Scaling Function

Three-body model for neutron-halo nuclei

2008 ◽  
Vol 32 (12) ◽  
pp. 972-975 ◽  
Author(s):  
Chu Yan-Yun ◽  
Chen Shuang ◽  
Ren Zhong-Zhou
Keyword(s):  
Halo Nuclei ◽  
Neutron Halo ◽  
Body Model ◽  
Three Body
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