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@ARTICLE{Vrtnik:826018,
author = {Vrtnik, S. and Koželj, P. and Meden, A. and Maiti, S. and
Steurer, W. and Feuerbacher, M. and Dolinšek, J.},
title = {{S}uperconductivity in thermally annealed
{T}a-{N}b-{H}f-{Z}r-{T}i high-entropy alloys},
journal = {Journal of alloys and compounds},
volume = {695},
issn = {0925-8388},
address = {Lausanne},
publisher = {Elsevier},
reportid = {FZJ-2017-00287},
pages = {3530 - 3540},
year = {2017},
abstract = {We present a study of superconductivity in Ta-Nb-Hf-Zr-Ti
high-entropy alloys (HEAs) by investigating four samples of
different atomic concentrations (equimolar and
off-equimolar) and number of components (4 and 5), subjected
to different thermal treatments. The structure of the
samples varied between a homogeneous random solid solution
and a partially ordered nanostructure in the form of a
three-dimensional grid of short-range ordered atomic
clusters enriched in Zr and Hf that has developed during
long-time annealing. Superconductivity was found to be a
robust phenomenon, being quite insensitive to the actual
structure of the material. All investigated samples were
superconducting in the entirety of their volumes. The
superconducting transition temperatures TC of the samples
are scattered in the range between 5.0 and 7.3 K and this
scatter could be related to the degree of structural and
chemical inhomogeneity of the samples. In the samples with
partially ordered nanostructure, short-range atomic clusters
possess a slightly different TC than the Ta- and Nb-rich
matrix. Our results also demonstrate the important fact that
the formation, stability and structure of a regular
(non-ideal) HEA mixture are determined by both, the
minimization of the mixing enthalpy that favors local atomic
ordering and the maximization of the mixing entropy that
favors a random solid solution. The actual equilibrium state
achieved during long-time thermal annealing via the atomic
diffusion is generally partially ordered, and the resulting
nanostructure is a sensitive function of the number of
components constituting the HEA, their concentrations, the
differences in the atomic radii and the annealing
temperature and time. This nanostructure essentially
determines the electronic properties of HEA materials.},
cin = {PGI-5},
ddc = {670},
cid = {I:(DE-Juel1)PGI-5-20110106},
pnm = {143 - Controlling Configuration-Based Phenomena (POF3-143)},
pid = {G:(DE-HGF)POF3-143},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000391818100074},
doi = {10.1016/j.jallcom.2016.11.417},
url = {https://juser.fz-juelich.de/record/826018},
}