The orthorhombic compound CeNi2Al5 is magnetically ordered below 2.6 K. Kon
dotype interactions together with strong crystal-electric-field (CEF) effec
ts give rise to a complex magnetic structure: (i) its propagation vector is
three dimensional and incommensurate, Ic = (0.500, 0.405. 0.083); (ii) the
Fourier components of the moment associated with this vector are tilted aw
ay from the easy-magnetization axis b. Furthermore, the magnetic structure
is double Ic, as the propagation vectors k = (k(x), k(y), k(z)) and k' = (-
k(x), k(y), k(z)) associated with different magnetic domains are not indepe
ndent.
New experiments have been undertaken to achieve a more precise determinatio
n of the magnetic structure. Magnetic peak intensity measurements with high
er resolution and polarization analysis have both led to the conclusion tha
t the Fourier component of the magnetic moment deviates slightly from the b
-direction. Considering the coupling of the two propagation vectors, the re
sulting moment describes very Bat ellipses with most of the moments very cl
ose to b. Neutron diffraction experiments down to 0.4 K have also been perf
ormed to investigate the evolution of the magnetic structure at low tempera
tures.