APS Logo

Magnetic correlations in the semimetallic hyperkagome iridate Na<sub>3</sub>Ir<sub>3</sub>O<sub>8</sub>: a rare case of doping in a quantum spin liquid

ORAL

Abstract

A decade ago the first realization of an effective spin 1/2 hyper-kagome lattice was discovered in the form of Na4Ir3O8, which is an insulator and was found to exhibit spin freezing at ~7 K .

Na3Ir3O8 has a different crystal structure, but the underlying hyperkagome arrangement of iridium ions is preserved. Moreover, the iridium valence in this system is 4.33+ and not 4+ like in the parent compound. Therefore, it can be seen as a 1/3 hole doped hyper-kagome spin system, a rare example of efficient doping achieved in a quantum spin liquid, following P.W. Anderson's seminal idea. Due to a complex interplay between inter-site hopping, Coulomb repulsion, crystal field splitting and spin-orbit coupling, it is a semi-metal.

We present a microscopic 23Na NMR study of the Na3Ir3O8 compound. The uniform q = 0 susceptibility is determined via shift measurements and the dynamical response by probing the spin-lattice relaxation rate. The susceptibility is consistent with a semimetal behavior, though with electronic bands substantially modified by correlations. Remarkably, the antiferromagnetic fluctuations present in the insulating parent compound Na4Ir3O8 survive in the studied compound. The spin dynamics are consistent with 120° excitations modes displaying short-range correlations.

Publication: G. Simutis et al., Magnetic correlations in the semimetallic hyperkagome iridate Na3Ir3O8, Phys. Rev. B 103, L100404 (2021).

Presenters

  • Philippe Mendels

    Université Paris-Saclay, Université Paris-Saclay, CNRS, Laboratoire de Physique des Solides, 91405, Orsay, France, Laboratoire de Physique des Solides, Paris-Saclay University and CNRS, France, Universit?© Paris-Sud 11, Universit?© Pa

Authors

  • Philippe Mendels

    Université Paris-Saclay, Université Paris-Saclay, CNRS, Laboratoire de Physique des Solides, 91405, Orsay, France, Laboratoire de Physique des Solides, Paris-Saclay University and CNRS, France, Universit?© Paris-Sud 11, Universit?© Pa

  • Gediminas Simutis

    Laboratoire de Physique des Solides, Paris-Saclay University and CNRS, France, Laboratory for Neutron and Muon Instrumentation, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland

  • Tomohiro Takayama

    Max Planck Institute for Solid State Physics

  • Quentin Barthélemy

    Laboratoire de Physique des Solides, Paris-Saclay University and CNRS, France, Université de Sherbooke, Université de Sherbrooke

  • Fabrice Bert

    Université Paris-Saclay, Université Paris-Saclay, CNRS, Laboratoire de Physique des Solides, 91405, Orsay, France, Laboratoire de Physique des Solides, Paris-Saclay University and CNRS, France, Université Paris-Saclay, CNRS, Laboratoire de Physique des Solides, Orsay, France

  • HIDENORI TAKAGI

    Max Planck Institute for Solid State Physics