Consider the Newton equation in the relativistic case (that is the
Newton-Einstein equation) \eqalign{\dot p = F(x),& F(x)=-\nabla V(x),\cr
p={\dot x \over \sqrt{1-{|\dot x|^2 \over c^2}}},& \dot p={dp\over dt}, \dot
x={dx\over dt}, x\in C^1(\R,\R^d),}\eqno{(*)}{\rm where\}V \in
C^2(\R^d,\R), |\pa^j\_x V(x)| \le \beta\_{|j|}(1+|x|)^{-(\alpha+|j|)} for
∣j∣≤2 and some α>1. We give estimates and asymptotics for
scattering solutions and scattering data for the equation (∗) for the case of
small angle scattering. We show that at high energies the velocity valued
component of the scattering operator uniquely determines the X-ray transform
PF. Applying results on inversion of the X-ray transform P we obtain that
for d≥2 the velocity valued component of the scattering operator at high
energies uniquely determines F. In addition we show that our high energy
asymptotics found for the configuration valued component of the scattering
operator doesn't determine uniquely F. The results of the present work were
obtained in the process of generalizing some results of Novikov [R.G. Novikov,
Small angle scattering and X-ray transform in classical mechanics, Ark. Mat.
37, pp. 141-169 (1999)] to the relativistic case