scholarly journals The dependence of the nuclear charge form factor on short-range correlations and surface fluctuation effects

1996 ◽  
Vol 597 (1) ◽  
pp. 19-34 ◽  
Author(s):  
S.E. Massen ◽  
V.P. Garistov ◽  
M.E. Grypeos
Keyword(s):  
Form Factor ◽  
Short Range ◽  
Nuclear Charge ◽  
Charge Form Factor ◽  
Charge Form ◽  
Surface Fluctuation ◽  
Fluctuation Effects ◽  
Short Range Correlations

Nuclear charge form factor in the topological soliton model

1988 ◽  
Vol 490 (3) ◽  
pp. 585-601 ◽  
Author(s):  
S. Boffi ◽  
O. Nicrosini ◽  
M. Radici
Keyword(s):  
Form Factor ◽  
Nuclear Charge ◽  
Charge Form Factor ◽  
Topological Soliton ◽  
Soliton Model ◽  
Charge Form

Short-range form of the charge distribution of4He and its charge form factor

1989 ◽  
Vol 101 (2) ◽  
pp. 155-162 ◽  
Author(s):  
M. A. K. Lodhi ◽  
A. K. Ray ◽  
C. Yalçin
Keyword(s):  
Form Factor ◽  
Charge Distribution ◽  
Short Range ◽  
Charge Form Factor ◽  
Charge Form

scholarly journals The dependence of the nuclear charge form factor on short range correlations and surface fluctuation effects

2020 ◽  
Vol 4 ◽  
pp. 26
Author(s):  
S. E. Massen ◽  
V. P. Garistov ◽  
M. E. Grypeos
Keyword(s):  
Form Factor ◽  
Short Range ◽  
Body Part ◽  
Correlation Factor ◽  
Charge Form Factor ◽  
Light Nuclei ◽  
Proton Form Factor ◽  
Nuclear Surface ◽  
Charge Form

An investigation is carried out in order to study effects, originating from fluctuations of the nuclear surface, to the elastic charge form factor of light nuclei in which the two-body part of the short range correlation factor is also included through a Jastrow-type correlation function. It is found that if these effects are taken into account in the uncorrected (harmonic oscillator) part of such a form-factor for the 4He, l6O and 40Ca nuclei, the quality of the fitting is improved. In addition, they lead to a drastic change in the asymptotic behaviour of the point-proton form factor which now drops off for large values of the momentum transfer q quite slowly that is as const.•q^-4.

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