B. Gottschalk et al., MULTIPLE COULOMB SCATTERING OF 160 MEV PROTONS, Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms, 74(4), 1993, pp. 467-490
We have measured multiple Coulomb scattering of 158.6 MeV protons in f
ourteen materials from beryllium to uranium including brass and severa
l plastics. Targets ranged from thin (negligible energy loss) to very
thick (greater than the mean proton range). The angular distribution w
as measured by means of a single diode dosimeter scanned typically ove
r two decades of dose falloff. Each data set was fitted with a Moliere
scattering distribution (using Bethe's tables) to extract a character
istic angle theta(M) as well as a Gaussian distribution to extract a c
haracteristic angle theta0. As expected in the small angle region, the
Gaussian fits about as well as the Moliere shape. The theta(M) values
were compared with Moliere's predicted value (chi(c) square-root B/sq
uare-root 2) including Fano's correction for scattering by atomic elec
trons and using Moliere's formalism to account for energy loss and/or
compound targets or mixtures. The distribution of the deviation from t
heory for 115 independent measurements is approximately normal, with a
mean value -0.5 +/- 0.4% and an rms spread of 5%. The theta0 values w
ere compared with Highland's formula and with an ''improved Highland''
formula of Lynch and Dahl, using our own generalization to thick targ
ets. The overall accuracy of Highland's formula is slightly worse than
that of Moliere theory. The distribution of the deviation from theory
for 115 independent measurements is normal, with a mean value -2.6 +/
- 0.5% and an rms spread of 6%. The Lynch formula gives nearly the sam
e average statistics though details of the fit are different. Some dat
a were taken for very thick targets (thickness greater than 97% of the
mean proton range) where only a fraction of the incident protons emer
ge. Here the characteristic angle appears to level off or even to fall
slightly with target thickness perhaps due to the filtering out of la
rge-angle protons. These measurements are presented but were excluded
from the comparison with theory.We have reviewed six other published p
roton measurements, partially reanalyzing four whose authors claimed t
hat Moliere theory either did not apply (because of thick targets) or
was incorrect. These experiments range from 1 MeV to 200 GeV incident
energy. Averaging each measurement including our own over everything b
ut target material we obtain 39 independent measurements of the deviat
ion from theory whose distribution is normal with a mean value -0.3 +/
- 0.5% and an rms spread of 3%. We conclude that Moliere theory with t
he Fano correction is accurate to better than 1% on the average for pr
otons. Systematic discrepancies on the order of a few percent with tar
get thickness and/or target material cannot be ruled out at present. I
n particular there is some indication that the theory may be almost-eq
ual-to 4% high for the highest-Z materials.