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Electron- and Hole-Doping Effects on the Metal-Insulator Transition in “113” Nickelates [<i>R</i>NiO<sub>3</sub>, <i>R </i>= Pr, Nd, (La,Y)] Prepared at High Oxygen Pressure*

ORAL

Abstract

We report x-ray diffraction, electrical resistivity, and other data on bulk polycrystalline materials prepared under high oxygen pressure (150–200 bar) at high temperature (T ≈ 1000°C). These conditions stabilize the nearly simple-perovskite “113” structure, RNiO3. For the orthorhombic parent compounds with the largest rare-earth ions that exhibit a metal-insulator transition, R = Pr and Nd, we dope with divalent Sr and Ba (hole doping) and tetravalent Ce and Th (electron doping). Results for Nd1–xAxNiO3 (A= Sr, Ce, Th) have been reported previously1: for example, for Ce4+, the net effect on the metal-insulator transition, ∂TMI/∂x ≈ –220 K, was corrected for size effects to obtain a bare electron-doping effect, ∂TMI/∂xelec ≈ –1100 K. Remarkably in our study, we find that, for Pr1–xCexNiO3, the shift in the metal-insulator transition temperature with concentration x is positive, with a net ∂TMI/∂x ≈ +225 K. Also, we find hysteresis in the metallic resistivity of rhombohedral La1–xCexNiO3, perhaps a signature of low-T pseudogap monoclinic short-range order.2
1J. L. García-Munoz et al., Phys. Rev. B 52, 13563 (1995). 2B. Li et al., Advanced Electronic Materials 2, 1500261 (2016).

Presenters

  • John T. Markert

    Department of Physics, University of Texas at Austin, Department of Physics, The University of Texas at Austin

Authors

  • Gregorio Ponti

    Department of Physics, University of Texas at Austin

  • Zachary P. Kuklinski

    Department of Physics, University of Texas at Austin

  • Quinn D. B. Timmers

    Department of Physics, University of Texas at Austin

  • John T. Markert

    Department of Physics, University of Texas at Austin, Department of Physics, The University of Texas at Austin