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NiRh2O4: A spin-orbit entangled diamond-lattice paramagnet

Shreya Das, Dhani Nafday, Tanusri Saha-Dasgupta, and Arun Paramekanti
Phys. Rev. B 100, 140408(R) – Published 14 October 2019
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Abstract

Motivated by the interest in topological quantum paramagnets in candidate spin-1 magnets, we investigate the diamond-lattice compound NiRh2O4 using ab initio theory and model Hamiltonian approaches. Our density functional study, taking into account the unquenched orbital degrees of freedom, shows stabilization of S=1, L=1 state. We highlight the importance of spin-orbit coupling, in addition to Coulomb correlations, in driving the insulating gap, and uncover frustrating large second-neighbor exchange mediated by Ni-Rh covalency. A single-site model Hamiltonian incorporating the large tetragonal distortion is shown to give rise to a spin-orbit entangled nonmagnetic ground state, largely accounting for the entropy, magnetic susceptibility, and inelastic neutron scattering results. Incorporating intersite exchange within a slave-boson theory, we show that exchange frustration can suppress exciton condensation. We capture the dispersive gapped magnetic modes, uncover “dark states” invisible to neutrons, and make predictions.

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  • Received 27 May 2019
  • Revised 23 September 2019

DOI:https://doi.org/10.1103/PhysRevB.100.140408

©2019 American Physical Society

Physics Subject Headings (PhySH)

  1. Physical Systems
  1. Techniques
Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Shreya Das1, Dhani Nafday2, Tanusri Saha-Dasgupta1,2, and Arun Paramekanti3,*

  • 1Department of Condensed Matter Physics and Materials Science, S.N. Bose National Centre for Basic Sciences, Kolkata 700098, India
  • 2School of Mathematical and Computational Sciences, Indian Association for the Cultivation of Science, Kolkata 700 032, India
  • 3Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7

  • *arunp@physics.utoronto.ca

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Issue

Vol. 100, Iss. 14 — 1 October 2019

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Images

  • Figure 1
    Figure 1

    (a) The GGA + U electronic structure of NiRh2O4 in low-temperature tetragonal phase. States projected onto Ni d, Rh d, and O p characters are shown as gray-shaded, black-solid line, and hatched areas, respectively. (b) The GGA + U + SOC electronic structure of NiRh2O4 in tetragonal phase. (c) The energy level positions for the spin-split and the crystal-field-split Ni d and Rh d states. For clarity, small splittings around 0.1 eV are not marked in the figure.

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  • Figure 2
    Figure 2

    The exchange pathways for first neighbor (J1) and inequivalent second neighbors (J2,J2) in the low-temperature tetragonal phase of NiRh2O4. Shown are the overlap of effective Ni Wannier functions placed at NN, in-plane NNN, and out-of-plane NNN Ni sites, with circles indicating nonzero weight at Rh sites in the pathway. Opposite sign parts of each Wannier function are colored differently.

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  • Figure 3
    Figure 3

    (a) Local dynamical spin correlation function Sloc(ω) within single-site model. Peaks are labeled by relevant excited states, and arrows indicate “dark states” invisible to neutrons due to vanishing matrix elements. (b) Intensity plot (arbitrary units) of powder-averaged INS spin structure factor, S(Q,ω), as a function of wave vector Q and energy ω (with 1meV broadening to mimic experimental resolution); see text for details.

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