Based on a detailed analysis of the Boltzmann equation for ion transpo
rt in solids, it has been shown that for low-energy ions incident on a
heavy element target the distribution function of the ions can be det
ermined by one single parameter, called the scaled transport cross-sec
tion, which was defined earlier [1]. This means that the transport qua
ntities of different ion-target-energy combinations should be similar
only when their scaled transport cross-section is the same. To test th
is significant conclusion, we undertook a set of systematic and extens
ive calculations of reflection coefficients using the improved biparti
tion model of ion transport. The systematic calculations include 3410
ion-target-energy combinations, namely H, D, T, He, Li, B, C, N, O, Ne
ions with energy ranges from 10 eV to 1 MeV normally incident to C, A
l, Cu, Mo, Ag, W, Au, Pb, U targets. The only restrictions is M(1)/M(2
) < 1/6. The calculations verify that particle and energy reflection c
oefficients present an excellent one-to-one correspondence to the scal
ed transport cross-section. Furthermore, based on the calculations, un
iversal expressions for both particle reflection coefficients and ener
gy reflection coefficients for normal ion incidence have been obtained
by fitting the numerical data. By comparing the results calculated by
the universal expressions with experimental and Monte Carlo data, it
is shown that the expression can describe reflection coefficients well
.