Electric and magnetic polarizabilities of hexagonal Ln2CuTiO6(Ln=Y, Dy, Ho, Er, and Yb)

Debraj Choudhury, Abhijit Hazarika, Adyam Venimadhav, Chandrasekhar Kakarla, Kris T. Delaney, P. Sujatha Devi, P. Mondal, R. Nirmala, J. Gopalakrishnan, Nicola A. Spaldin, Umesh V. Waghmare, and D. D. Sarma
Phys. Rev. B 82, 134203 – Published 5 October 2010

Abstract

We investigated the rare-earth transition-metal oxide series, Ln2CuTiO6 (Ln=Y, Dy, Ho, Er, and Yb), crystallizing in the hexagonal structure with noncentrosymmetric P63cm space group for possible occurrences of multiferroic properties. Our results show that while these compounds, except Ln=Y, exhibit a low-temperature antiferromagnetic transition due to the ordering of the rare-earth moments, the expected ferroelectric transition is frustrated by the large size difference between Cu and Ti at the B site. Interestingly, this leads these compounds to attain a rare and unique combination of desirable paraelectric properties with high dielectric constants, low losses, and weak temperature and frequency dependencies. First-principles calculations establish these exceptional properties result from a combination of two effects. A significant difference in the MO5 polyhedral sizes for M=Cu and M=Ti suppress the expected cooperative tilt pattern of these polyhedra, required for the ferroelectric transition, leading to relatively large values of the dielectric constant for every compound investigated in this series. Additionally, it is shown that the majority contribution to the dielectric constant arises from intermediate-frequency polar vibrational modes, making it relatively stable against any temperature variation. Changes in the temperature stability of the dielectric constant among different members of this series are shown to arise from changes in relative contributions from soft polar modes.

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  • Received 7 June 2010

DOI:https://doi.org/10.1103/PhysRevB.82.134203

©2010 American Physical Society

Authors & Affiliations

Debraj Choudhury1,2, Abhijit Hazarika1, Adyam Venimadhav3, Chandrasekhar Kakarla3, Kris T. Delaney4, P. Sujatha Devi5, P. Mondal5, R. Nirmala1, J. Gopalakrishnan1, Nicola A. Spaldin4, Umesh V. Waghmare6, and D. D. Sarma1,*

  • 1Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560012, India
  • 2Department of Physics, Indian Institute of Science, Bangalore 560012, India
  • 3Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India
  • 4University of California, Santa Barbara, California 93106-5050, USA
  • 5Central Glass and Ceramic Research Institute, Kolkata 700032, India
  • 6Jawaharlal Nehru Centre for Advanced Scientific Research, Bangalore 560064, India

  • *Also at JNCASR, Bangalore 560054, India; sarma@sscu.iisc.ernet.in

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Issue

Vol. 82, Iss. 13 — 1 October 2010

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