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On the received coefficients of the analytical forms for deuteron
wave function in coordinate representation in form rl +
1\textit{*exp(-A*r)} for the modern realistic nucleon-nucleon
potentials NijmI, NijmII, Nijm93, Reid93 and Argonne v18 are
calculated charge GC(p), quadrupole GQ(p) and magnetic
GM(p) deuteron form factors. An original dipole fit for
proton and neutron isoscalar electric and magnetic form factors is
used for calculations. Theoretical calculations of values of the
deuteron form factor are compared with their experimental data of
world collaborations (Bates, BLAST, Bonn, JLab, Mainz, Naval
Research Lab, NIKHEF, Orsay, Saclay, SLAC, Stanford, VEPP3 and
VEPP4) and reviews (Abbott, Boden, Garcon and Karpius). The change
of the sign of form factors is in the pulse regions at 4.7-4.9
fm-1 for GC; at 12.8-14.7 fm-1 for GQ; at
6.3-8.1 and 11.4-12.2 fm-1 for GM. The theoretical
values for the form factors GQ(0) and GM(0) were
calculated at the boundary condition for the momentum at
p2=0. Calculated positions of the zero for deuteron form
factors are compared with values for other potential models. The
peculiarities of parametrizations of deuteron form factors for
theoretical approaches and fits of theoretical calculations to
experimental values, which are described in the cited literature,
are analyzed. Formulas for spherical and quadrupole form factors
are writed, which are expressed in terms of the coefficients for
the indicated deuteron wave function. At large values of momentum
the asymptotics of the deuteron form factors are determined by the
coefficients of the analytical forms for deuteron wave function,
nucleon isoscalar form factors and the order of momentum. The
further use of deuteron form factors for obtaining polarization
observables in processes involving deuteron as a projectile is
discussed.
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