A simple solution accounting for the secondary-extinction correction of the
integrated intensity of the diffracted beam in a mosaic crystal is derived
for the case of symmetrical Bragg reflection from an 'infinitely thick' pl
ane parallel plate. The solution of energy-transfer equations contains a 't
hickness-dependent term' which enables further extension of the problem to
the 'thin' film case. The new formulae are derived assuming a rectangular o
r triangular crystalline block distribution, which leads to exact integrati
on of the diffracted intensity. In addition, a general term for Zachariasen
[Acta Cryst. (1963), 16, 1139-1147] series expansion, assuming Gaussian do
main distribution, is deduced. In fact, the new analytical results represen
t a variety of improved approximations which are simultaneously valid both
for weak and for strong extinction effects usually observed in textured fil
ms. The formulae are used for computing the pole density and secondary exti
nction in electrodeposited nickel films having different texture sharpnesse
s. It may be anticipated that the precision in any X-ray diffraction charac
terization of films could be enhanced using the improved secondary-extincti
on corrections.