Pion-nucleon form factors in the unitary three-body model forNNscattering

1986 ◽  
Vol 56 (26) ◽  
pp. 2785-2788 ◽  
Author(s):  
H. Tanabe ◽  
K. Ohta
Keyword(s):  
Form Factors ◽  
Body Model ◽  
Nucleon Form Factors ◽  
Pion Nucleon ◽  
Three Body

Nucleon form factors in a simple three-body quark model

1998 ◽  
Vol 1 (3) ◽  
pp. 307-315 ◽  
Author(s):  
E. Santopinto ◽  
F. Iachello ◽  
M.M. Giannini
Keyword(s):  
Quark Model ◽  
Form Factors ◽  
Nucleon Form Factors ◽  
Three Body

scholarly journals Study of the Density Distributions and Elastic form Factors of the Exotic Nuclei, 8He And 26F, Via the Three-Body Model

2021 ◽  
pp. 2555-2564
Author(s):  
Ghufran M. Sallh ◽  
Ahmed N. Abdullah
Keyword(s):  
Form Factors ◽  
High Energy ◽  
Exotic Nuclei ◽  
Wave Functions ◽  
Glauber Model ◽  
Radial Wave ◽  
Density Distributions ◽  
Body Model ◽  
Elastic Form ◽  
Three Body

    The matter, proton, and neutron density distributions of the ground state, the nuclear root-mean-square (rms) radii, and the elastic form factors of a two- neutron, 8He and 26F, halo nuclei have been studied by the three body model of  within the harmonic oscillator (HO) and Woods-Saxon (WS) radial wave functions. The calculated results show that the two body model within the HO and WS radial wave functions succeeds in reproducing the neutron halo in these exotic nuclei. Moreover, the Glauber model at high energy (above several hundred MeV) has been used to calculate the rms radii and reaction cross sections of these nuclei.

Nuclear structure investigation of some neutron-rich halo nuclei

2017 ◽  
Vol 26 (07) ◽  
pp. 1750048 ◽  
Author(s):  
Ahmed N. Abdullah
Keyword(s):  
Form Factors ◽  
Wave Functions ◽  
Halo Nuclei ◽  
Long Tail ◽  
Halo Structure ◽  
Density Distributions ◽  
The Core ◽  
Body Model ◽  
Realistic Interaction ◽  
Three Body

The ground state proton, neutron and matter densities, the corresponding rms radii and charge form factors of a dripline nuclei 6He, [Formula: see text]Li, [Formula: see text]Be and [Formula: see text]Be have been studied via a three–body model of [Formula: see text]. The core–neutron interaction takes the form of Woods-Saxon (WS) potential. The two valence neutrons of 6He, [Formula: see text]Li and [Formula: see text]Be interact by the realistic interaction of ZBMII while those of [Formula: see text]Be interact via the realistic interaction of VPNP. The core and valence (halo) density distributions are described by the single-particle wave functions of the WS potential. The calculated results are discussed and compared with the experimental data. The long tail performance is clearly noticed in the calculated neutron and matter density distributions of these nuclei. The structure of the two valence neutrons in 6He, [Formula: see text]Li and [Formula: see text]Be is found to be mixed configurations with dominant [Formula: see text] while that for [Formula: see text]Be is mixed configurations with dominant ([Formula: see text]. The analysis of the present study supports the halo structure of these nuclei.

Study of the Isospin Mixing in 6Li with α + p + n Three-Body Model

2013 ◽  
Vol 54 (7-10) ◽  
pp. 1381-1384
Author(s):  
N. Kurihara ◽  
Y. Kikuchi ◽  
K. Katō
Keyword(s):  
Body Model ◽  
Three Body
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