
Extra electron reflections in concentrated alloys do not necessitate short-range order
Flynn Walsh,1, 2 Mingwei Zhang,1, 3, 4 Robert O. Ritchie,1, 4 Andrew M. Minor,1, 3, 4 and Mark Asta1, 4, 5
1Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
2Graduate Group in Applied Science & Technology, University of California, Berkeley, CA, USA
3National Center for Electron Microscopy, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
4Department of Materials Science & Engineering, University of California, Berkeley, CA, USA
5Corresponding author: mdasta@berkeley.edu
In many concentrated alloys of current interest, the observation of diffuse superlattice intensities
by transmission electron microscopy has been attributed to chemical short-range order. We briefly
review these findings and comment on the plausibility of widespread interpretations, noting the
absence of expected peaks, conflicts with theoretical predictions, and the possibility of alternative
explanations.
The nature of chemical short-range order (SRO) in
face-centered cubic (fcc) alloys containing several 3d
principal elements, such as “medium-entropy” VCoNi
and CrCoNi, has been intensively investigated in recent
years [1–18]. While there may be little evidence that SRO
can be controlled to tailor the bulk mechanical properties
of these materials [5,6,13,17], it has been argued that
an essentially ubiquitous degree of ˚
A-scale order could
nonetheless play an important role in a wide range of
properties [1,7]. For example, many alloys containing Co
are predicted to form hexagonal close-packed lattices at
ambient conditions [19,20], but quenched-in SRO could
account for the persistent metastability of the fcc phase
[1,7,11].
This view appears to be corroborated by recent trans-
mission electron microscopy (TEM) purporting the pres-
ence of local order in a variety of samples subject to mini-
mal thermal processing beyond high-temperature homog-
enization. For example, the observation of SRO in VCoNi
was proposed [8] on the basis of diffuse intensities at
1
2{311}superlattice sites in reciprocal space while imag-
ing in the [¯
112] zone axis (ZA), which indicates the crys-
tallographic direction of electron incidence. An equiva-
lent electron diffraction pattern is shown in Fig. 1. Addi-
tional 1
3{422}intensities were later reported in the [¯
111]
ZA [9]. Similar observations have been at various points
attribtued to SRO in a Cr-Ni-based alloy [21], Mn-Fe-
based alloys [22–25], CrCoNi [10,13], CrMnFeCoNi [15],
and VFeCoNi [18]. The same features have also been
reported without the assumption of SRO [5,17,26–28].
Some of these reflections are consistent with the par-
tial formation of a CuPt-type (L11) concentration wave
involving the compositional enrichment and depletion of
alternating {111}(and simultaneously {311}) planes, as
illustrated in Fig. 2a. Diffuse intensities in VCoNi and
CrCoNi have been interpreted to reflect modulations of
V or Cr concentrations in this manner [8–10], largely
on the basis of electronic structure calculations indicat-
ing repulsive interactions between V-V and Cr-Cr neigh-
bors, although we note that CuPt-type ordering has the
same nearest-neighbor pair frequencies as a random al-
loy. Some efforts have been made to support this theory
with atomic-scale composition mapping [8,10,18], but,
FIG. 1: Electron diffraction of CrCoNi in the
[¯
112] ZA. This pattern, which is based on experimental
data from a previous study [13], is representative of
literature results for alloys discussed in the text. Diffuse
intensities at 1
2{311}superlattice positions are marked
with arrows, but there are no peaks at 1
2{111}sites, as
highlighted by the dotted circles.
in contrast to the diffuse intensities themselves, these
measurements are noisy and susceptible to local fluctua-
tions, making it difficult to draw statistical conclusions.
Regardless of chemical specifics, the presence of su-
perlattice reflections should not be regarded as incontro-
vertible evidence for ordering. In fact, widespread inter-
pretations of SRO are questionable on several accounts,
such as the absence of additional expected peaks. By
the symmetry of the fcc lattice, a CuPt-type decoration
arXiv:2210.01277v2 [cond-mat.mtrl-sci] 21 Aug 2023