Jakob Nagl, Kirill Yu Povarov, Benjamin Duncan, Catharina Näppi, Dmitry Khalyavin, Pascal Manuel, Fabio Orlandi, Jeremy Sourd, Beat Valentin Schwarze, Freya Husstedt, Sergei A Zvyagin, Oksana Zaharko, Paul Steffens, Arno Hiess, David R Allan, Sarah A Barnett, Zewu Yan, Severian Gvasaliya, Andrey Zheludev
The prospect of merging the paradigms of geometric frustration on a triangular lattice and bond anisotropies in the strong spin-orbit coupling limit holds tremendous promise in the search for exotic quantum materials. Here we identify a new candidate system to realize such physics, the organic quantum antiferromagnet (CD3ND3)2NaRuCl6. We report a combination of thermodynamic, magneto-elastic and neutron scattering experiments on single-crystals to determine the phase diagram in axial magnetic fields H∥c and propose a minimal model Hamiltonian. (CD3ND3)2NaRuCl6 displays an ideal triangular arrangement of Ru3+ ions adopting the spin-orbital entangled j eff = 1/2 state. It hosts residual magnetic order below T N = 0.23 K and a highly unusual H - T phase diagram including three different incommensurate states. Spin-waves in the high-field polarized regime are described by a Heisenberg triangular lattice Hamiltonian with a potential sub-leading bond dependent anisotropy term J ±±. We argue that the multi-q ground state in zero magnetic field is a prime candidate for hosting the Z 2 vortex crystal proposed on the triangular Heisenberg-Kitaev model. (CD3ND3)2NaRuCl6 is the first member in an extended family of quantum triangular lattice magnets, providing a new playground to study the interplay of geometric frustration and spin-orbit effects.