Polarising and non-polarising supermirrors with angles of reflection t
heta(c) of m similar or equal to 2 times the critical angle of Ni are
now produced in large quantities mostly by using sputtering techniques
. The coatings can be deposited with such perfection that the surface
morphology of the substrates becomes as important for achieving high r
eflectivities as the perfection of the layer structure itself. As a co
nsequence, m can be increased to similar or equal to 4 simply by incre
asing the number of layers to similar or equal to 1000. However, this
requires that the individual thicknesses of the layers decrease too, a
pproaching the thickness of the interdiffusion zones thus diminishing
the reflectivity at large reflection angles. In addition, the total th
ickness of the coatings ends up to be of the order of typically 5 mu m
. Therefore, the forces on the substrate increase due to the stress wi
thin the layers leading finally to the destruction of the substrates.
Clearly, such supermirrors an of no practical use. The stress within t
he layers can be significantly reduced by properly tuning the partial
pressures of the reactive gases during sputtering. Moreover, by using
anisotropic sputtering it is possible to induce an anisotropic stress
distribution within the plane of the layers. As a consequence, it is p
ossible to fabricate magnetic multilayers that exhibit a well-defined
easy axis of magnetisation due to magnetostriction. This effect is par
ticularly pronounced for polarising FeCoV/TiNx supermirrors, such that
remanent mirrors can be produced that allow the polarisation of neutr
ons in zero magnetic field. (C) 1998 Elsevier Science B.V. All rights
reserved.