Intrinsic anomalous Hall conductivity and field-enhanced diamagnetism in untwinned Weyl metal SrRuO3 thin films

ORAL

Abstract

The anomalous Hall effect (AHE) manifests in solids with broken time-reversal symmetry. In a ferromagnetic metal, intrinsic and extrinsic AHE can contribute to the Hall signal. In this report, we studied the low-temperature magnetotransport properties of ferromagnetic untwinned SrRuO3 (SRO) thin films grown on SrTiO3 (001) substrates with low residual resistivity for various thicknesses (ts) ranging from 3.9 nm to 37.1 nm. The magnitude of the Hall conductivity |σxy| at zero magnetic fields in the low-temperature regime was found to be nearly t-independent and approaching a constant value of about 2×104 Ω-1m-1, which is close to the estimated intrinsic anomalous Hall conductivity due to Berry curvatures of the bulk band of about e2/hco ≈ 5×104 Ω-1m-1 (co being the lattice constant). The negligible variation of |σxy| with σxx in the low-temperature regime at zero magnetic field reveals that the |σxy| is nearly independent of the electron scattering lifetime. This suggests a small contribution of extrinsic skew scattering effect to the AHE, and the intrinsic AHE dominates the zero-field Hall signals in SRO at low temperatures. Interestingly, a rigorous magnetization measurement on a SRO film using a SQUID magnetometer reveals a field-enhanced diamagnetic response that increases as the temperature drops. The intrinsic value of the |σxy|~ e2/hco and the field-enhanced diamagnetic response in the SRO film in the low-temperature regime strongly support the presence of the Weyl metal phase in SRO. A systematic study on the temperature and thickness-dependent Hall conductivity and magnetization will be presented and discussed.

* National Science and Technology Council of Taiwan, Academia Sinica and National Taiwan University

Presenters

  • Uddipta Kar

    Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan

Authors

  • Uddipta Kar

    Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan

  • Cho-Hao Lu

    Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan, Inst. of Physics, Academia Sinica

  • Akhilesh K Singh

    Academia Sinica, Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan, Inst. of Physics, Academia Sinica

  • P.V. Sreenivasa Reddy

    Department of Physics, National Taiwan University, Taipei 10617, Taiwan, Dept. of Physics, National Taiwan University

  • Cheng-Tung Cheng

    Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan, Inst. of Physics, Academia Sinica

  • Wei-Cheng Lee

    Department of Physics, Applied Physics and Astronomy, Binghamton University, Binghamton, New York 13902, USA, Binghamton University

  • Guang-Yu Guo

    Department of Physics, Department of Physics, National Taiwan University, Taipei 10617, Taiwan, Dept. of Physics, National Taiwan University, National Taiwan University

  • Wei-Li Lee

    Inst. of Physics, Academia Sinica, Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan