Abstract
Cu2TSiS4 (T = Mn and Fe) polycrystalline and single-crystal materials were prepared with high-temperature solid-state and chemical vapor transport methods, respectively. The polar crystal structure (space group Pmn21) consists of chains of corner-sharing and distorted CuS4, Mn/FeS4, and SiS4 tetrahedra, which is confirmed by Rietveld refinement using neutron powder diffraction data, X-ray single-crystal refinement, electron diffraction, energy-dispersive X-ray spectroscopy, and second harmonic generation (SHG) techniques. Magnetic measurements indicate that both compounds order antiferromagnetically at 8 and 14 K, respectively, which is supported by the temperature-dependent (100-2 K) neutron powder diffraction data. Additional magnetic reflections observed at 2 K can be modeled by magnetic propagation vectors k = (1/2,0,1/2) and k = (1/2,1/2,1/2) for Cu2MnSiS4 and Cu2FeSiS4, respectively. The refined antiferromagnetic structure reveals that the Mn/Fe spins are canted away from the ac plane by about 14°, with the total magnetic moments of Mn and Fe being 4.1(1) and 2.9(1) μB, respectively. Both compounds exhibit an SHG response with relatively modest second-order nonlinear susceptibilities. Density functional theory calculations are used to describe the electronic band structures.
Original language | English |
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Pages (from-to) | 530-542 |
Number of pages | 13 |
Journal | Inorganic Chemistry |
Volume | 62 |
Issue number | 1 |
DOIs | |
State | Published - Jan 9 2023 |
Funding
Z.T.M. and X.T. were supported by start-up funding from George Mason University. J.A.A. and A.J.C. recognize funding provided by the United States National Science Foundation, DMR-1611198. J.I.J. acknowledges support from the Basic Science Research Programs (2021R1A2C2013625) through the National Research Foundation of Korea (NRF), funded by the Korean government. Special thanks to G&H Cleveland for donating the optical-grade AGS and AGSe reference materials that were used for NLO studies. N.J.G. acknowledges the support from the National Science Foundation (NSF) CAREER award DMR-2143903. Magnetic measurements at Argonne National Laboratory were supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Science and Engineering Division. C.J.K. was supported by the NRF grant (NRF-2022R1C1C1008200). This work used resources at the Spallation Neutron Source, DOE Office of Science Facilities operated by the Oak Ridge National Laboratory. TEM work was performed at the National High Magnetic Field Laboratory, which is supported by National Science Foundation Cooperative agreement no. DMR-1644779 and the State of Florida. We thank Dr. Thomas J. Emge (Rutgers, The State University of New Jersey) for helping with single-crystal refinements.
Funders | Funder number |
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Basic Science Research Programs | 2021R1A2C2013625 |
State University of New Jersey | |
State of Florida | |
National Science Foundation | DMR-1611198, DMR-2143903 |
U.S. Department of Energy | |
Office of Science | |
Basic Energy Sciences | |
Oak Ridge National Laboratory | |
George Mason University | |
Division of Materials Sciences and Engineering | DMR-1644779, NRF-2022R1C1C1008200 |
National Research Foundation of Korea |