Abstract:
Invariant description of the particle spatial distribution is introduced on the basis
of relativistic configurational representation obtained with the aid of expansions
over unitary representations of the Lorentz group. A formula which gives the correct
“almost dipole” asymptotical behaviour of the proton form-factor $\displaystyle{F_P(t)\to\frac{\ln |t|/M^2}{t^2}}$
at large $-t$ is obtained.
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