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    Structural, magnetic, and spin dynamical properties of the polar antiferromagnets Ni3−xCoxTeO6(x=1,2)

    Stella Skiadopoulou1,2,3,*, Maria Retuerto4, Fedir Borodavka1, Christelle Kadlec1, Filip Kadlec1, Martin Míšek1, Jan Prokleška5, Zheng Deng4, Xiaoyan Tan4,† et al.

    Corey Frank4, Jose A. Alonso6, Maria Tereza Fernandez-Diaz7, Mark Croft8, Fabio Orlandi9, Pascal Manuel9, Emma McCabe10, Dominik Legut2, Martha Greenblatt4, and Stanislav Kamba1

    • 1Institute of Physics,Czech Academy of Sciences, Na Slovance 2, 18221 Prague 8, Czech Republic
    • 2IT4Innovations, VSB Technical University of Ostrava, 17, Listopadu 2172/15, CZ-708 00 Ostrava-Poruba, Czech Republic
    • 3School of Physics, CRANN, Trinity College, Dublin 2, Ireland
    • 4Department of Chemistry and Chemical Biology, Rutgers, The State University of New Jersey, 610 Taylor Road, Piscataway, New Jersey 08854, USA
    • 5Department of Condensed Matter Physics, Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 121 16 Prague 2, Czech Republic
    • 6Instituto de Ciencia de Materiales de Madrid, C.S.I.C., Cantoblanco, E-28049 Madrid, Spain
    • 7Institut Laue Langevin, BP 156X, Grenoble, F-38042, France
    • 8Department of Physics and Astronomy, Rutgers, the State University of New Jersey, 136 Frelinghusen Road, Piscataway, New Jersey 08854, USA
    • 9ISIS Facility, STFC, Rutherford Appleton Laboratory, Chilton, Didcot, Oxfordshire, OX11 0QX, United Kingdom
    • 10School of Physical Sciences, University of Kent, Canterbury, Kent, CT2 7NH, United Kingdom

    • *Corresponding author: skiadops@tcd.ie
    • †Present address: Department of Chemistry and Biochemistry, George Mason University, 4400 University Dr, Fairfax, Virginia 22030, USA.

    Phys. Rev. B 101, 014429 – Published 21 January, 2020

    DOI: https://doi.org/10.1103/PhysRevB.101.014429

    Abstract

    We present results of a multimethod investigation of the polar antiferromagnets Ni2CoTeO6 and NiCo2TeO6, inspired by the colossal magnetoelectric effect present in Ni3TeO6. Both compounds crystalize in the same polar space group R3 as Ni3TeO6, preserving the crystal symmetry at least from room temperature down to 2 K. Ni2CoTeO6 and NiCo2TeO6 undergo antiferromagnetic phase transitions at TN=55 and 52 K, and spin-flop transitions at an external magnetic field of approximately 8 and 4 T, respectively. Both compounds present an incommensurate antiferromagnetic helical structure with spins lying in the ab plane, in contrast to the collinear one along the c axis in Ni3TeO6. Moreover, dielectric anomalies are observed at their antiferromagnetic phase transitions, suggesting a magnetoelectric behavior. Spin and lattice dynamics studies by a combination of infrared, Raman, and terahertz spectroscopies were performed. Below TN, in both Ni2CoTeO6 and NiCo2TeO6, low-frequency spin excitations extremely sensitive to external magnetic field were observed. At least one of these magnons was simultaneously seen in Raman and THz spectra of both compounds, therefore we propose to assign them to electromagnons.

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