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Ultrafast terahertz-field-driven ionic response in ferroelectric BaTiO3

F. Chen et al.
Phys. Rev. B 94, 180104(R) – Published 22 November 2016
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Abstract

The dynamical processes associated with electric field manipulation of the polarization in a ferroelectric remain largely unknown but fundamentally determine the speed and functionality of ferroelectric materials and devices. Here we apply subpicosecond duration, single-cycle terahertz pulses as an ultrafast electric field bias to prototypical BaTiO3 ferroelectric thin films with the atomic-scale response probed by femtosecond x-ray-scattering techniques. We show that electric fields applied perpendicular to the ferroelectric polarization drive large-amplitude displacements of the titanium atoms along the ferroelectric polarization axis, comparable to that of the built-in displacements associated with the intrinsic polarization and incoherent across unit cells. This effect is associated with a dynamic rotation of the ferroelectric polarization switching on and then off on picosecond time scales. These transient polarization modulations are followed by long-lived vibrational heating effects driven by resonant excitation of the ferroelectric soft mode, as reflected in changes in the c-axis tetragonality. The ultrafast structural characterization described here enables a direct comparison with first-principles-based molecular-dynamics simulations, with good agreement obtained.

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  • Received 27 January 2016
  • Revised 24 October 2016

DOI:https://doi.org/10.1103/PhysRevB.94.180104

©2016 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

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Vol. 94, Iss. 18 — 1 November 2016

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  • Figure 1
    Figure 1

    Experimental setup, applied THz field, and enhancement electrode structure. (a) Sample schematic showing ferroelectric polarization perpendicular to the film along [001]. The field is applied with light polarization orthogonal to the ferroelectric polarization. The inset shows the pseudocubic unit cell of BTO. (b) Applied THz electric field as a function of time, measured by electro-optic sampling at the sample position at LCLS.

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  • Figure 2
    Figure 2

    Terahertz-pump x-ray probe measurements and field dependence. (a) Static BTO (003) rocking curve at room temperature, with three specific incident angles marked as 1, 2, and 3 corresponding to the angles where the time scans (b), (c), and (d) were measured. Red curves are simulations using dynamical diffraction theory based on calculated THz-driven strains and structure factor modulations. (e) The differential rocking curve at t=5 and 15 ps comparing the rocking curves measured with and without THz excitation. (f) Dependence of change in diffracted intensity on the THz peak field, measured at t=15 ps on the high-angle side of the rocking curve. The red curve is the quadratic fit.

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  • Figure 3
    Figure 3

    Terahertz-pump x-ray probe measurements within split-ring resonator structure. (a) (002) rocking curve before (t=900 ps) and after (t=100 ps) time zero showing large-amplitude field-induced tensile strain. (b) Nanosecond time-dependent intensity measured at the low-angle side of the rocking curve below and above the Curie temperature. Also shown (solid line) are fits to a thermal model for the cooling of the BTO film in the paraelectric phase into the substrate, described in the Supplemental Material.

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  • Figure 4
    Figure 4

    MD simulation results. (a) Schematic showing how a rotation of the polarization leads to an increase in out-of-plane rms displacements. (b) The angle of the net polarization with respect to the c axis. (c) The rms displacement of the Ti atom along the in-plane and out-of-plane direction after in-plane THz excitation. (d) Corresponding histograms showing distributions of in-plane and out-of-plane displacements before and at the peak of the THz field. The inset shows the MD simulation supercell from which these histograms are calculated. (e) Calculated structure factor modulation for the (003) reflection. (f) Projected net polarization along the c axis as a function of time.

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