Magnetotransport in H || c of La1.875Ba0.125CuO4 near the charge order (CO) transition

ORAL

Abstract

The nature of the dynamics of charge-ordered states in underdoped cuprates has been of great recent interest. Our work on La2-xBaxCuO4 with x=0.125 (LBCO) in zero magnetic field (H) reveals the presence of dynamic behavior within the charge-ordered state in the form of avalanches, similar to that in La1.48Nd0.4Sr0.12CuO4 (LNSCO). In LNSCO, avalanches were also observed to be asymmetrically driven by H around the concurrent CO and structural transition with an additional onset of negative magnetoresistance (MR), which was attributed to the emergence of CO [1]. In La1.7Eu0.2Sr0.12CuO4 (LESCO) negative MR, albeit with no avalanches, was observed at the onset of CO but not at the higher temperatures around the structural transition [1]. The presence of avalanches and overlap of the CO and structural transitions in LBCO present the opportunity to clarify the role of the LNSCO Nd3+ moments and the origin of the negative MR. Therefore, we report the H = 0 findings and the study of H || c magnetoresistance of LBCO near the CO transition.
[1] P. G. Baity et al., Phys. Rev. Lett. 120, 156602 (2018).

Presenters

  • Lily Stanley

    Department of Physics and National High Magnetic Field Lab, Florida State University, Dept. of Phys. Natl. High Magnetic Field Lab.

Authors

  • Lily Stanley

    Department of Physics and National High Magnetic Field Lab, Florida State University, Dept. of Phys. Natl. High Magnetic Field Lab.

  • Paul G. Baity

    Dept. of Phys. & Natl. High Magnetic Field Lab., Florida State Univ., National High Magnetic Field Lab, Department of Physics and National High Magnetic Field Lab, Florida State University, Dept. of Phys. Natl. High Magnetic Field Lab.

  • Dragana Popovic

    Dept. of Phys. & Natl. High Magnetic Field Lab., Florida State Univ., National High Magnetic Field Lab, Department of Physics and National High Magnetic Field Lab, Florida State University, Dept. of Phys. Natl. High Magnetic Field Lab.

  • John Tranquada

    Brookhaven National Laboratory, CMPMS, Brookhaven National Laboratory, Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Condensed Matter Physics & Materials Science, Brookhaven National Laboratory, Brookhaven Natl Lab

  • Genda Gu

    Brookhaven National Laboratory, Brookhaven National Lab, Department of Condensed Matter Physics and Materials Science, Brookhaven, Brookhaven National Laboratory, Upton, New York 11973-5000, USA., Cond. Matt. Physics and Material Science, Brookhaven Natl Lab, Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Condensed Matter Physics & Materials Science Department, Brookhaven National Laboratory, Brookhaven National Labs, Long Island, NY, USA, 11973, Condensed Matter Physics & Materials Science, Brookhaven National Laboratory, Condensed Matter Physics, Brookhaven National Laboratory, Brookhaven National Laboratories, Chinese Academy of Sciences, Condensed Matter Physics & Materials Science, Brookhaven National Lab, Brookhaven Natl Lab