Giant electrocaloric response in the prototypical Pb(Mg,Nb)O3 relaxor ferroelectric from atomistic simulations

Zhijun Jiang, Y. Nahas, S. Prokhorenko, S. Prosandeev, D. Wang, Jorge Íñiguez, and L. Bellaiche
Phys. Rev. B 97, 104110 – Published 30 March 2018
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Abstract

An atomistic effective Hamiltonian is used to investigate electrocaloric (EC) effects of Pb(Mg1/3Nb2/3)O3 relaxor ferroelectrics in its ergodic regime, and subject to electric fields applied along the pseudocubic [111] direction. Such a Hamiltonian qualitatively reproduces (i) the electric field-versus-temperature phase diagram, including the existence of a critical point where first-order and second-order transitions meet each other; and (ii) a giant EC response near such a critical point. It also reveals that such giant response around this critical point is microscopically induced by field-induced percolation of polar nanoregions. Moreover, it is also found that, for any temperature above the critical point, the EC coefficient-versus-electric-field curve adopts a maximum (and thus larger electrocaloric response too), that can be well described by the general Landau-like model proposed by Jiang et al., [Phys. Rev. B 96, 014114 (2017)], and that is further correlated with specific microscopic features related to dipoles lying along different rhombohedral directions. Furthermore, for temperatures being at least 40 K higher than the critical temperature, the (electric field, temperature) line associated with this maximal EC coefficient is below both the Widom line and the line representing percolation of polar nanoregions.

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  • Received 5 February 2018

DOI:https://doi.org/10.1103/PhysRevB.97.104110

©2018 American Physical Society

Physics Subject Headings (PhySH)

  1. Research Areas
  1. Physical Systems
Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Zhijun Jiang1,2,*, Y. Nahas2, S. Prokhorenko2,3, S. Prosandeev2,4, D. Wang1, Jorge Íñiguez5, and L. Bellaiche2,†

  • 1School of Microelectronics and State Key Laboratory for Mechanical Behaviour of Materials, Xi'an Jiaotong University, Xi'an 710049, China
  • 2Physics Department and Institute for Nanoscience and Engineering, University of Arkansas, Fayetteville, Arkansas 72701, USA
  • 3Theoretical Materials Physics, Q-MAT CESAM, University of Liège, B-4000 Sart Tilman, Belgium
  • 4Research Institute of Physics and Physics Department, Southern Federal University, Rostov-on-Don 344090, Russia
  • 5Materials Research and Technology Department, Luxembourg Institute of Science and Technology, 5 Avenue des Hauts-Fourneaux, L-4362 Esch/Alzette, Luxembourg

  • *zhijun.jiang.phy@gmail.com
  • laurent@uark.edu

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Issue

Vol. 97, Iss. 10 — 1 March 2018

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