ISSN 0036ꢀ0236, Russian Journal of Inorganic Chemistry, 2015, Vol. 60, No. 12, pp. 1578–1582. © Pleiades Publishing, Ltd., 2015.
Original Russian Text © S.F. Marenkin, I.V. Fedorchenko, V.M. Trukhan, S.V. Trukhanov, T.V. Shoukavaya, P.N. Vasil’ev, A.L. Zhaludkevich, 2015, published in Zhurnal Neorganꢀ
icheskoi Khimii, 2015, Vol. 60, No. 12, pp. 1723–1727.
PHYSICOCHEMICAL ANALYSIS
OF INORGANIC SYSTEMS
State Diagram of the Zn3As2–MnAs System
S. F. Marenkina, b, I. V. Fedorchenkoa, b, V. M. Trukhanc, S. V. Trukhanovc,
T. V. Shoukavayac, P. N. Vasil’eva, b, and A. L. Zhaludkevichc
a MISiS National Research Technological University, Leninskii pr. 4, Moscow, 119991 Russia
b Kurnakov Institute of General and Inorganic Chemistry, Russian Academy of Sciences,
Leninskii pr. 31, Moscow, 119991 Russia
c SSPA “Scientific and Practical Material Research Centre of NAS of Belarus”,
National Academy of Sciences of Belarus, ul. P. Brovki 19, Minsk, 22072 Belarus
eꢀmail: marenkin@rambler.ru
Received March 23, 2015
Abstract—The Zn3As2–MnAs system was studied by Xꢀray powder diffraction, differential thermal, and
microstructural analyses. This system is of the eutectic type with the eutectic coordinates (30 wt % (50 mol %)
Zn3As2, 70 wt % (50 mol %) MnAs, Tmelt = 815°C). The MnAs solubility boundary on the side of Zn3As2 is
10 wt %. Zn3As2 alloys containing more than 10 wt % MnAs are ferromagnetic with Tc ~ 320 K. Their magꢀ
netization increases with increasing MnAs content.
DOI: 10.1134/S0036023615120189
Alloys of zinc and manganese arsenides are considꢀ components were Zn3As2 and MnAs, which were synꢀ
ered promising materials for granulated structures thesized in a vacuum in doubleꢀwall quartz ampoules
with giant magnetoresistance [1]. Granulated strucꢀ from highꢀpurity elemental substances Zn, As, and
tures are of interest owing to their possible use in spinꢀ Mn taken in stoichiometric ratios [10]. The reactants
tronics [2].
were placed in the inner ampoule, the inner walls of
which were lined with pyrolytic carbon for preventing
quartz from interacting with melts of components.
The processes were carried out in a furnace with autoꢀ
Alloys of zinc and manganese arsenides were studꢀ
ied as magnetic materials [3–5], and in those studies
they were regarded as solid solutions (Zn1 – xMnx)3As2
within the concentration range
lished [4] temperature dependences of the magnetizaꢀ
tion of these alloys are characteristic of superparamagꢀ
nets [6]. From the curves, paramagnetic and ferroꢀ
magnetic components can be separated. It is well
matic temperature control with an accuracy of
1°С.
0
≤
х 0.13. The pubꢀ
≤
To avoid escape of highly volatile components from
the evaporation zone because of their evaporation, the
ampoules were positioned in the isothermal part of the
furnace. The temperature–time conditions of the synꢀ
thesis were the following: heating at a rate of 50 deg/h
known that introduction of atoms of dꢀelements, in
to 600
heating to 1015
°
С
and treatment at this temperature for 2 h,
for Zn3As2 and to 950 for MnAs
particular, manganese, to a semiconductor leads to
a transition of the semiconductor from the diamagꢀ
netic to the paramagnetic state. The ferromagꢀ
netism of (Cd1 – xMnx)3As2, which is isostructural to
(Zn1 – xMnx)3As2, was attributed [7] to manganese
clusters. In our opinion, the samples studied in the disꢀ
cussed works [3–6] were inhomogeneous and conꢀ
tained not only the solid solution (Zn1 – xMnx)3As2 but
also MnAs nanoinclusions. We believe that the presꢀ
ence of such nanoinclusions accounts for the ferroꢀ
magnetic properties of manganeseꢀcontaining zinc
arsenide alloys [8, 9]. In this context, it was of interest
to continue to study alloys of zinc and manganese arsꢀ
enides, in particular, to determine the nature of the
interaction between Zn3As2 and MnAs.
°С
°С
and treatment of melts for better homogenization for
no less than 3 h, and cooling of ampoules in switchedꢀ
off furnace mode. The samples of intermediate comꢀ
positions were obtained under the temperature–time
conditions similar to those of the Zn3As2 synthesis.
The samples were investigated by Xꢀray powder difꢀ
fraction, differential thermal, and microstructural
analyses.
The Xꢀray powder diffraction analysis was perꢀ
formed with a Bruker D8 ADVANCE diffractometer
(
Cu
K
radiation, = 0.1540 nm, graphite monochroꢀ
λ
α
mator). Phases were identified based on the ICDD
PDFꢀ2 powder diffraction file database using the Difꢀ
frac.Suite EVA and Topaz software at the Research
Equipment Sharing Center for Physical Methods for
Studying Substances and Materials, Kurnakov Instiꢀ
EXPERIMENTAL
Samples for studying the phase diagram were preꢀ tute of General and Inorganic Chemistry, Russian
pared at an interval of 10 mol % MnAs. The initial Academy of Sciences, Moscow, Russia. The Xꢀray
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