Nanolayered
metallic alloys are promising materials for nuclear
applications thanks to their resistance to radiation damage. Here,
we investigate the effect of ion (C, Si, and Cu) irradiation at room
temperature with different fluences into sputtered Zr/Nb metallic
multilayer films with periods 27 nm (thin) and 96 nm (thick). After
irradiation, while a high strain in the entire thin nanoscale metallic
multilayer (NMM) is observed, a quite small strain in the entire thick
NMM is established. This difference is further analyzed by a semianalytical
model, and the reasons behind it are revealed, which are also validated
by local strain mapping. Both methods show that within a thick layer,
two opposite distortions occur, making the overall strain small, whereas
in a thin layer, all the atomic planes are affected by the interface
and are subjected to only a single type of distortion (Nbtension
and Zrcompression). In both thin and thick NMMs, with increasing
damage, the strain around the interface increases, resulting in a
release of the elastic energy at the interface (decrease in the lattice
mismatch), and the radiation-induced transition of the Zr/Nb interfaces
from incoherent to partially coherent occurs. Density functional theory
simulations decipher that the inequality of point defect diffusion
flux from the inner to the interface-affected region is responsible
for the presence of opposite distortions within a layer. Technologically,
based on this work, we estimated that Zr/Nb55 with thicknesses around
Zr = 24 nm and Nb = 31 nm is the most promising multilayer system
with the high radiation damage resistance and minimum swelling for
nuclear applications.