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Neutron scattering studies of the ferroelectric distortion and spin dynamics in the type-1 multiferroic perovskite Sr0.56Ba0.44MnO3

Daniel K. Pratt, Jeffrey W. Lynn, James Mais, Omar Chmaissem, Dennis E. Brown, Stanislaw Kolesnik, and Bogdan Dabrowski
Phys. Rev. B 90, 140401(R) – Published 9 October 2014

Abstract

The magnetic order, spin dynamics, and crystal structure of the multiferroic Sr0.56Ba0.44MnO3 have been investigated using neutron and x-ray scattering. Ferroelectricity develops at TC=305 K with a polarization of 4.2 µC/cm2 associated with the displacements of the Mn ions, while the Mn4+ spins order below TN200 K into a simple G-type commensurate magnetic structure. Below TN the ferroelectric order decreases dramatically, demonstrating that the two order parameters are strongly coupled. The ground state spin dynamics is characterized by a spin gap of 4.6(5) meV and the magnon density of states peaking at 43 meV. Detailed spin wave simulations with a gap and isotropic exchange of J=4.8(2) meV describe the excitation spectrum well. Above TN strong spin correlations coexist with robust ferroelectric order.

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  • Received 12 June 2014
  • Revised 19 September 2014

DOI:https://doi.org/10.1103/PhysRevB.90.140401

©2014 American Physical Society

Authors & Affiliations

Daniel K. Pratt1, Jeffrey W. Lynn1,*, James Mais2, Omar Chmaissem2,3, Dennis E. Brown2, Stanislaw Kolesnik2, and Bogdan Dabrowski2

  • 1NIST Center for Neutron Research, National Institute of Standards and Technology, Gaithersburg, Maryland 20899-6102, USA
  • 2Department of Physics, Northern Illinois University, DeKalb, Illinois 60115, USA
  • 3Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA

  • *Corresponding author: Jeffrey.Lynn@nist.gov

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Vol. 90, Iss. 14 — 1 October 2014

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  • Figure 1
    Figure 1

    (a) Phase diagram for Sr1xBaxMnO3 showing the concentration region where ferroelectric (FE) and multiferroic (MF) behavior develop. The point for x=1/2 is from Sakai et al. [11]. The present multiferroic sample studied in this work is Sr0.56Ba0.44MnO3. The inset shows the smooth development of the integrated intensity of the {1/2,1/2,1/2} antiferromagnetic peak of this G-type magnetic structure obtained on BT-7. The curve is a simple mean field order parameter fit of the square of the magnetic order parameter to estimate the antiferromagnetic transition TN of 196(3) K. (b) X-ray diffraction data taken at the Advanced Photon Source demonstrating the crystallographic distortion associated with the ferroelectric transition at TC=305 K. The size of the ferroelectric distortion indicates a maximum polarization of 13 μC/cm2 at this composition. Note that the distortion is dramatically reduced as the magnetic order develops, demonstrating that the two order parameters are strongly coupled.

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  • Figure 2
    Figure 2

    (a) Contour plot of the BT-7 experimental data for the ground state spin dynamics at low energies, which can be directly compared with the calculated magnon density of states shown in (b). (c) Constant energy cuts through the low temperature data (points). Data have been offset by 150 counts for each energy for clarity. The solid curves through the data are the calculated results from the model. Uncertainties where indicated are statistical in origin and represent one standard deviation.

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  • Figure 3
    Figure 3

    (a) Calculated contour map of the overall polycrystalline spin wave scattering, convoluted with the instrumental resolution, using the final parameters of J=4.8 meV and ΔAFM=4.6 meV. The wave vector and energy ranges shown in Figs. 2 and 2 are indicated by the bounded box. (b) Calculated spin wave dispersion expected for a single crystal. (c) Inelastic neutron scattering measurement showing the top of the band of magnetic excitations at 43(1) meV. The solid curve shows the fit to the Heisenberg model described in the text, powder averaged and convoluted with the experimental resolution. (d) High resolution inelastic measurement using the cold triple axis spectrometer SPINS to determine the ground state spin wave gap of ΔAFM=4.6 meV, which was determined by fitting the observed scattering intensity to a Heaviside function convoluted with the instrumental resolution [solid (red) curve].

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  • Figure 4
    Figure 4

    Temperature dependence of the scattering at an energy transfer of 5 meV. The scattering is resolution limited at low temperature. With increasing temperature the intensity increases due to the Bose-Einstein population factor for bosons. We also observe that the spin gap decreases and approaches zero as the transition is approached from below, while the wave vector width broadens in approaching and exceeding TN. In the paramagnetic state the data reveal that there are substantial spin-spin correlations up to at least 1.5TN.

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