In this paper we propose a fitting procedure to describe the bandpass
effect on all x radiation that passes through a focusing graphite mono
chromator used on the diffracted beam. The proposed bandpass function
is: M(2 theta)=1/(1+K(mon1)s(Kmon2)), with s=(2 sin theta)/lambda, whe
re K-mon1 and K-mon2 are constants which have been refined by means of
a Rietveld analysis, using a physically modeled background (Riello et
al., J. Appl. Crystallogr. 28, 115-120). We have investigated two pol
ycrystalline powders: alpha-Al2O3, and a mixture of alpha and beta-Si3
N4. The so-obtained bandpass functions for these materials are close e
nough to conclude that they depend only on the used experimental setup
(in the present case the S-Pert-Philips diffractometer with a graphit
e focusing manochromator). Knowledge of the bandpass function is impor
tant to suitably model the Compton scattering, which is a component of
the background scattering. The present procedure allows one to avoid
the direct experimental determination of the bandpass function, which
requires the use of another monochromator (analyzer) and another tube
with an intense white spectrum. (C) 1997 International Centre for Diff
raction Data.