Erratum: Nucleon form factors and root-mean-square radii on a 
(10.8  fm)4
 lattice at the physical point [Phys. Rev. D 
99
, 014510 (2019)]

The two-neutron halo-nuclei (17B, 11Li, 8He) was investigated using a two-body nucleon density distribution (2BNDD) with two frequency shell model (TFSM). The structure of valence two-neutron of 17B nucleus in a pure (1d5/2) state and in a pure (1p1/2) state for 11L and 8He nuclei. For our tested nucleus, an efficient (2BNDD's) operator for point nucleon system folded with two-body correlation operator's functions was used to investigate nuclear matter density distributions, root-mean square (rms) radii, and elastic electron scattering form factors. In the nucleon-nucleon forces the correlation took account of the effect for the strong tensor force (TC's). The wave functions of single particle harmonic oscillator are used with two different oscillator size parameters βc and βv, where the former is for the core (inner) orbits and the latter is for the valence (halo) orbits. The measured matter density distributions of these nuclei clearly showed long tail results. To investigate elastic electron scattering form factors the plane wave born approximation (PWBA) with two body nucleon density distribution (2BNDD's) was use.

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Nucleon structure from 2+1 flavor lattice QCD near the physical point

EPJ Web of Conferences ◽

10.1051/epjconf/201817506007 ◽

2018 ◽

Vol 175 ◽

pp. 06007 ◽

Cited By ~ 6

Author(s):

Natsuki Tsukamoto ◽

Ken-Ichi Ishikawa ◽

Yoshinobu Kuramashi ◽

Shoichi Sasaki ◽

Takeshi Yamazaki

Keyword(s):

Lattice Spacing ◽

Pion Mass ◽

Axial Vector ◽

Form Factors ◽

Nucleon Structure ◽

Matrix Elements ◽

Physical Point ◽

Nucleon Form Factors ◽

Pseudo Scalar ◽

Simulation Point

We present an update on our results of nucleon form factors measured on a large-volume lattice (8:1fm)4 at almost the physical point in 2+1 flavor QCD. The configurations are generated with the stout-smeared O(a) improved Wilson quark action and Iwasaki gauge action at β = 1:82, which corresponds to the lattice spacing of 0.085 fm. The pion mass at the simulation point is about 145 MeV. We determine the isovector electric radius and magnetic moment from nucleon electric (GE) and magnetic (GM) form factors. We also report on preliminary results of the axial-vector (FA), induced pseudo-scalar (FP) and pseudo-scalar (GP) form factors in order to verify the axial Ward-Takahashi identity in terms of the nucleon matrix elements, which may be called as the generalized Goldberger-Treiman relation.

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Charge form factors and root mean square radii ofHe3andH3with the new Bonn potential

Physical Review C ◽

10.1103/physrevc.38.2366 ◽

1988 ◽

Vol 38 (5) ◽

pp. 2366-2376 ◽

Cited By ~ 13

Author(s):

Kr. T. Kim ◽

Y. E. Kim ◽

D. J. Klepacki ◽

Richard A. Brandenburg ◽

E. P. Harper ◽

...

Keyword(s):

Root Mean Square ◽

Form Factors ◽

Mean Square ◽

Charge Form ◽

Bonn Potential

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Study of charge density distributions, elastic charge form factors and root-mean square radii for 4He, 12C and 16O nuclei using Woods- Saxon and harmonic-oscillator potentials

Iraqi Journal of Physics (IJP) ◽

10.30723/ijp.v14i30.199 ◽

2019 ◽

Vol 14 (30) ◽

pp. 42-50

Author(s):

Arkan R. Ridha

Keyword(s):

Harmonic Oscillator ◽

Charge Density ◽

Root Mean Square ◽

Form Factors ◽

Mean Square ◽

Oscillator Potential ◽

Radial Wave ◽

Charge Form ◽

Density Distributions ◽

Proton Charge

The nuclear charge density distributions, form factors andcorresponding proton, charge, neutron, and matter root mean squareradii for stable 4He, 12C, and 16O nuclei have been calculated usingsingle-particle radial wave functions of Woods-Saxon potential andharmonic-oscillator potential for comparison. The calculations for theground charge density distributions using the Woods-Saxon potentialshow good agreement with experimental data for 4He nucleus whilethe results for 12C and 16O nuclei are better in harmonic-oscillatorpotential. The calculated elastic charge form factors in Woods-Saxonpotential are better than the results of harmonic-oscillator potential.Finally, the calculated root mean square radii usingWoods-Saxonpotentials how overestimation in comparison with experimental dataon contrary to the results of harmonic-oscillator potential.

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