Previously,
refractory high-entropy alloys (HEAs) with high crystallinity
were synthesized using a configurable target without heat treatment.
This study builds upon prior investigations to develop nonrefractory
elemental HEAs with low crystallinity using a novel target system.
Different targets with various elemental compositions, i.e., Co20Cr20Ni20Mn20Mo20 (target 1), Co30Cr15Ni25Mn15Mo15 (target 2), and Co15Cr25Cu20Mn20Ni20 (target 3), are designed
to modify the phase structure. The elemental composition is varied
to ensure face-centered cubic (FCC) or body-centered cubic (BCC) phase
stabilization. In target 1, the FCC and BCC phases coexist, whereas
targets 2 and 3 are characterized by a single FCC phase. Thin films
based on targets 1 and 2 exhibit crystalline phases followed by annealing,
as indicated by X-ray diffraction (XRD) and transmission electron
microscopy (TEM) analyses. In contrast, target 3 yields crystalline
thin films without any heat treatment. The thin-film coatings are
classified based on the atomic size difference (δ). The δ
value for the target with the elemental composition CoCrMoMnNi is
9.7, i.e., ≥6.6, corresponding to an HEA with an amorphous
phase. However, the annealed thin film is considered a multiprincipal
elemental alloy. In contrast, δ for the CoCrCuMnNi HEA is 5,
i.e., ≤6.6, upon the substitution of Mo with Cu, and a solid
solution phase is formed without any heat treatment. Thus, the degree
of crystallinity can be controlled through heat treatment and the
manipulation of δ in the absence of heat treatment. The XRD
results clarify the crystallinity and phase structure, indicating
the presence of FCC or a combination of FCC and BCC phases. The outcomes
are consistent with those obtained through the analysis of the valence
electron concentration based on X-ray photoelectron spectroscopy.
Furthermore, a selected area electron diffraction analysis confirms
the presence of both amorphous and crystalline structures in the HEA
thin films. Additionally, phase evolution and segregation are observed
at 500 °C.