  On the received coefficients of the analytical forms for deuteron wave
function in coordinate representation in form r^(l+1)*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 in the denominator. The further use of deuteron form factors for
obtaining polarization observables in processes involving deuteron as a
projectile is discussed.
