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Mn 2 FeWO 6 : A New Ni 3 TeO 6 ‐Type Polar and Magnetic Oxide
Author(s) -
Li ManRong,
Croft Mark,
Stephens Peter W.,
Ye Meng,
Vanderbilt David,
Retuerto Maria,
Deng Zheng,
Grams Christoph P.,
Hemberger Joachim,
Hadermann Joke,
Li WenMin,
Jin ChangQing,
Saouma Felix O.,
Jang Joon I.,
Akamatsu Hirofumi,
Gopalan Venkatraman,
Walker David,
Greenblatt Martha
Publication year - 2016
Publication title -
advanced materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 10.707
H-Index - 527
eISSN - 1521-4095
pISSN - 0935-9648
DOI - 10.1002/adma.201600479
Subject(s) - materials science , oxide , polar , nanotechnology , metallurgy , physics , astronomy
In this work, we present the high pressure and temperature (HPT) synthesis of Mn 2 FeWO 6 —a new magnetic and polar member of the A 2 BB′O 6 -type corundum derivative family, and the results of the crystal structure, SHG activity, magnetic phase diagram, and electrical/dielectric properties. First-principles calculations are also carried out to better understand its structure, polarization, complex magnetic properties, and to point to new materials design with multifunctional properties. Polycrystalline black Mn 2 FeWO 6 was prepared at 1673 K for 1 h at 8 GPa. Original lab powder X-ray diffraction (PXD, Figure S2, Supporting Information) indicates a rhombohedral cell ( a ≈ 5.3 Å, c ≈ 13.9 Å) of the main phase and a small wolframite impurity (Figure S3a,b and Table S1, Supporting Information). Figure 1 a presents the RT synchrotron powder X-ray diffraction (SPXD) patterns of Mn 2 FeWO 6 , which could correspond to any of the R 3 or R -3 structure types discussed above. However, the high-angle annular dark fi eld scanning transmission electron microscopy (HAADF-STEM) images (Figure 1 b and S4, Supporting Information) clearly show Fe/W ordering, and thus rule out IL prototype for Mn 2 FeWO 6 . Polar magnets are one of the most promising materials for multiferroics and spintronics. Recently, the A 2 BB′O 6 -type corundum derivatives have drawn much interest due to their remarkable magnetic and electronic properties with polar structures and multiferroic and second harmonic generation (SHG) behavior. [ 1–6 ] These structures are related to perovskite, but unlike perovskites, which have corner-sharing B site octahedra, in these phases, with unusually small A-site cations, both the A and B sites are octahedrally coordinated. The corner-, face-, and edge-sharing octahedra form a 3D lattice. [ 2,7 ] The A 2 BB′O 6 -type corundum derivatives can crystallize in the centrosymmetric ilmenite (IL, space group R -3), or in non-centrosymmetric LiNbO 3 (LN, R 3 c ) , or ordered ilmenite (OIL, R 3), or Ni 3 TeO 6 (NTO, R 3) structure, as shown in Figure S1 (Supporting Information). The stabilization of any one of these structures depends on the cation arrangement and their ordering/disordering degree, which are affected by the cationic size and charge differences, electron confi guration, and synthesis conditions. [ 1,8–11 ] The general structural features of A 2 BB′O 6 -type corundum derivatives with octahedral coordination of all metal sites favor the formation of practical magnetic and multiferroic/magnetoelectric materials by incorporation of magnetic transition metal ions. Recently, near room temperature (RT) ferrimagnetic (FiM) behavior of Mn 2 FeSbO 6 ( T C ≈ 270 K) [ 1 ] and antiferromagnetic (AFM) Ni 3 TeO 6 with nonhysteretic colossal magnetoelectricity [ 4 ] were reported. More recently, we reported