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Ba3MxTi3xO9 (M=Ir, Rh): A family of 5d/4d-based diluted quantum spin liquids

R. Kumar, D. Sheptyakov, P. Khuntia, K. Rolfs, P. G. Freeman, H. M. Rønnow, Tusharkanti Dey, M. Baenitz, and A. V. Mahajan
Phys. Rev. B 94, 174410 – Published 7 November 2016

Abstract

We report the structural and magnetic properties of the 4d (M = Rh) based and 5d (M = Ir) based systems Ba3MxTi3xO9 (nominally x=0.5, 1). The studied compositions were found to crystallize in a hexagonal structure with the centrosymmetric space group P63/mmc. The structures comprise of A2O9 polyhedra [with the A site (possibly) statistically occupied by M and Ti] in which pairs of transition metal ions are stacked along the crystallographic c axis. These pairs form triangular bilayers in the ab plane. The magnetic Rh and Ir ions occupy these bilayers, diluted by Ti ions even for x=1. These bilayers are separated by a triangular layer which is dominantly occupied by Ti ions. From magnetization measurements we infer strong antiferromagnetic couplings for all of the materials but the absence of any spin-freezing or spin-ordering down to 2 K. Further, specific heat measurements down to 0.35 K show no sign of a phase transition for any of the compounds. Based on these thermodynamic measurements we propose the emergence of a quantum spin liquid ground state for Ba3Rh0.5Ti2.5O9, and Ba3Ir0.5Ti2.5O9, in addition to the already reported Ba3IrTi2O9.

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  • Received 14 April 2016
  • Revised 11 September 2016

DOI:https://doi.org/10.1103/PhysRevB.94.174410

©2016 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

R. Kumar1, D. Sheptyakov2, P. Khuntia3,4, K. Rolfs5, P. G. Freeman6,7, H. M. Rønnow6, Tusharkanti Dey1,8, M. Baenitz4, and A. V. Mahajan1,*

  • 1Department of Physics, Indian Institute of Technology Bombay, Powai, Mumbai 400076, India
  • 2Laboratory for Neutron Scattering and Imaging, Paul Scherrer Institut, 5232 Villigen-PSI, Switzerland
  • 3Laboratoire de Physique des Solides Universite Paris-Sud, UMR CNRS91405 Orsay, France
  • 4Max-Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany
  • 5Laboratory for Developments and Methods, Paul Scherrer Institut, 5232 Villigen PSI, Switzerland
  • 6Laboratory for Quantum Magnetism, Ecole Polytechnique Federale de Lausanne (EPFL), CH 1015, Switzerland
  • 7Jeremiah Horrocks Institute for Mathematics, Physics and Astronomy, University of Central Lancashire, Preston, PR1 2HE United Kingdom
  • 8Experimental Physics VI, Center for Electronic Correlations and Magnetism, University of Augsburg, D-86159 Augsburg, Germany

  • *mahajan@phy.iitb.ac.in

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Vol. 94, Iss. 17 — 1 November 2016

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Images

  • Figure 1
    Figure 1

    Schematic representation of the crystal structure of Ba3MTi2O9 (M=Ir, Rh) in the space group P63/mmc. (a) An ideal unit cell, i.e., with the 4f site equally occupied by Ir (or Rh) and Ti and the 2a site occupied by Ti only. (b) The structure of a A2O9 polyhedron (where A corresponds to M and Ti with a 50% probability each), consisting of two face sharing AO6 octahedra, thus forming the M-Ti, MM, or Ti-Ti dimers. (c) Formation of bitriangular planes containing an equal amount the nonmagnetic Ti and magnetic (Ir or Rh) atoms in the 4f(1/3,2/3,z) positions.

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  • Figure 2
    Figure 2

    Typical Rietveld refinement plots. (a) The neutron diffraction data collected for Ba3IrTi2O9 at 300 K with wavelength λ=1.15Å and (b) with wavelength λ=1.49Å for Ba3Ir0.5Ti2.5O9. Experimental points (black open circles), calculated patterns (red lines) and difference curves (green lines) are shown, the ticks (blue vertical lines) below the graphs indicate the calculated positions of Bragg peaks. It should be noted that the green lines on y axis are shifted for clarity.

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  • Figure 3
    Figure 3

    The left y-axis shows the temperature dependent susceptibility of nominal Ba3Ir0.5Ti2.5O9 measured in 500 Oe in the temperature range 2400 K and the black solid line represents the Curie-Weiss fit in the temperature range 150400 K. The right y-axis depicts the T dependence of inverse dc susceptibility of the parent compound Ba3IrTi2O9(nominal) and its diluted variant Ba3Ir0.5Ti2.5O9. Inset shows the ZFC and FC data recorded in the temperature range 220 K at 25 Oe for Ba3Ir0.5Ti2.5O9 in a linear-log plot.

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  • Figure 4
    Figure 4

    (a) The Cp(T) data for Ba3Ir0.5Ti2.5O9 (baked) is depicted in the log-log plot as a function of temperature at different fields. (b) The magnetic heat capacity Cm is shown in a log-log plot and the solid lines are fits to the power law: Cm=γTα (explained in the text). The obtained exponent values are written against the Cm data.

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  • Figure 5
    Figure 5

    A few representative plots of [CP(H)CP(H=0)]/T or (CP/T) for Ba3Ir0.5Ti2.5O9 at various values of the field H (as given in the legend) and their fit to Eq. (1) (black lines). (Inset) Variation of the Schottky gap as a function of magnetic field for orphan spins.

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  • Figure 6
    Figure 6

    The neutron diffraction data collected at 300 K for (a) nominal Ba3RhTi2O9 (in actuality Ba3Rh0.593Ti2.407O9) with λ=1.15Å and (b) nominal Ba3Rh0.5Ti2.5O9 (in actuality Ba3Rh0.432Ti2.568O9) with λ=1.49Å, are shown with open black circles and the red solid lines represent the Rietveld refined patterns. The Bragg positions for main and impurity phases (Ba9Rh8O24) are shown by vertical blue and purple lines and the difference patterns are depicted with green lines, respectively. It should be noted that Ba3RhTi2O9 (nominal) contains roughly 12% of impurity phase Ba9Rh8O24, whereas its diluted variant Ba3Rh0.5Ti2.5O9 (nominal) possesses less than 1.5% of impurity phase of Ba9Rh8O24. The inset shows a comparison of the low-angle ranges of the experimental neutron diffraction patterns of Ba3RhTi2O9 at 20 and at 2 K with λ=1.886Å, indicating that no additional (magnetic) intensity can be observed at the lowest achieved temperature.

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  • Figure 7
    Figure 7

    The main figure shows the temperature dependent susceptibilities of nominal Ba3Rh0.5Ti2.5O9 (AP) (cyan, open circles) and a month older batch of nominal Ba3Rh0.5Ti2.5O9 (ML) (orange, open triangles) measured in 5 kOe in the temperature range 2400 K and the brown solid line represents the Curie-Weiss fit in the temperature range 150400 K. Inset (a) and (b) depict the ZFC and FC data of nominal Ba3Rh0.5Ti2.5O9 (AP) and nominal Ba3Rh0.5Ti2.5O9 (ML) measured at 100 Oe, respectively.

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  • Figure 8
    Figure 8

    (a) The heat capacity data for nominal Ba3Rh0.5Ti2.5O9 (AP/Baked) in log-log plot as a function of temperature at different fields. (b) The magnetic heat capacity Cm is shown in a log-log plot and the solid lines are fits to the power law: Cm=γTα. The obtained exponent values are written against the Cm data.

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  • Figure 9
    Figure 9

    A few representative plots of [CP(H)CP(H=0)]/T or (CP/T) for nominal Ba3Rh0.5Ti2.5O9 at various values of the field H (as given in the legend) and their fit to Eq. (1) (black lines). (Inset) Variation of the Schottky gap as a function of magnetic field for orphan spins.

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  • Figure 10
    Figure 10

    Entropy change as a function of temperature for Ir and Rh variants at zero magnetic field for the nominal compositions of Ba3Ir0.5Ti2.5O9 and Ba3Rh0.5Ti2.5O9.

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  • Figure 11
    Figure 11

    Inverse susceptibility plots for Ir, Rh, and their variant samples (nominal composition) as a function of temperature. The data for Ba3IrTi2O9 are taken from Ref. [4].

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