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Quantum phases diagram of the the Shastry-Sutherland compound SrCu<sub>2</sub>(BO<sub>3</sub>)<sub>2</sub> at high magnetic field and high pressure

ORAL

Abstract

In the Shastry-Sutherland model, the ground state is expected to change from a spin dimer singlet state to a novel, intermediate 4-spin plaquette singlet state, then to an antiferromagnet state, when the relative strength of the nearest neighbor and next-nearest neighbor interactions (J/J’) is tuned. SrCu2(BO3)2 realizes the Shastry-Sutherland model at ambient pressure and can be tuned to other phases by application of high pressure, thus attracting considerable interests. Recent experimental advances have revealed the presence of an intermediate ground state with signatures of a 4-spin plaquette singlet state at high pressure. However, this intermediate phase also feature signatures that clearly deviate from the prediction of the ideal Shastry-Sutherland model. Therefore, the nature of this plaquette phase and how it evolves into other phases remain unclear. Here, we report a comprehensive study of the quantum phase diagram of the plaquette state by tuning the pressure and magnetic field, using a highly sensitive magnetization measurement technique. Our results reveal the emergence of a sequence of ground states once the spin dimer singlet and the plaquette singlet phase are suppressed by the field, which are further corroborated by our theoretical simulations.

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Presenters

  • Zhenzhong Shi

    Department of Physics, Duke University, Duke University

Authors

  • Zhenzhong Shi

    Department of Physics, Duke University, Duke University

  • Sachith Dissanayake

    Department of Physics, Duke University, Oak Ridge National Lab, Duke University, Oak Ridge National Laboratory

  • David E Graf

    National High Magnetic Field Laboratory, Florida State University, National High Magnetic Field Lab, Florida State University, National High Magnetic Field Laboratory, Tallahassee and Florida State University, National High Magnetic Field Laboratory, Florida State University, National High Magnetic Field Laboratory (FSU), Department of Physics, Florida State University, National High Magnetic Field Laboratory and Department of Physics, Florida State University, National High Magnetic Field Lab, National High Magnetic Field Laboratory, Tallahassee, FL, CMS, National High Magnetic Laboratory

  • Philippe Corboz

    Institute for Theoretical Physics and Delta Institute for Theoretical Physics, University of Amsterdam

  • Daniel Marc Silevitch

    Caltech, California Institute of Technology

  • Hanna Dabkowska

    McMaster University

  • Thomas F Rosenbaum

    Caltech, California Institute of Technology

  • Frederic Mila

    Institute of Physics, Ecole Polytechnique Federale de Lausanne

  • Sara Haravifard

    Department of Physics and Department of Mechanical Engineering & Materials Science, Duke University, Department of Physics and Department of Mechanical Engineering and Materials Science, Duke University, Duke University, Department of Physics, Duke University, Physics & Mechanical Engineering and Material Sciences, Duke University, Department of Physics and Department of Mechanical Engineering & Materials, Duke University