386 research outputs found

    Sequential pulsed laser deposition of homoepitaxial SrTiO3_3 thin films

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    Control of thin film stoichiometry is of primary relevance to achieve desired functionality. Pulsed laser deposition ablating from binary-oxide targets (sequential deposition) can be applied to precisely control the film composition, offsetting the importance of growth conditions on the film stoichiometry. In this work, we demonstrate that the cation stoichiometry of SrTiO3_3 thin films can be finely tuned by sequential deposition from SrO and TiO2_2 targets. Homoepitaxial SrTiO3_3 films were deposited at different substrate temperatures and Ti/Sr pulse ratios, allowing the establishment of a growth window for stoichiometric SrTiO3_3. The growth kinetics and nucleation processes were studied by reflection high-energy electron diffraction and atomic force microscopy, providing information about the growth mode and the degree of off-stoichiometry. At the optimal (stoichiometric) growth conditions, films exhibit atomically flat surfaces, whereas off-stoichiometry is accommodated by crystal defects, 3D islands and/or surface precipitates depending on the substrate temperature and the excess cation. This technique opens the way to precisely control stoichiometry and doping of oxide thin films.Comment: 6 pages, 5 figure

    Large phonon-drag enhancement induced by narrow quantum confinement at the LaAlO3/SrTiO3 interface

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    The thermoelectric power of the two-dimensional electron system (2DES) at the LaAlO3/SrTiO3 interface is explored below room temperature, in comparison with that of Nb-doped SrTiO3 single crystals. For the interface we find a region below T =50 K where thermopower is dominated by phonon-drag, whose amplitude is hugely amplified with respect to the corresponding bulk value, reaching values ~mV/K and above. The phonon-drag enhancement at the interface is traced back to the tight carrier confinement of the 2DES, and represents a sharp signature of strong electron-acoustic phonon coupling at the interface

    Large modulation of the Shubnikov-de Haas oscillations by the Rashba interaction at the LaAlO3_{3}/SrTiO3_{3} interface

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    We investigate the 2-dimensional Fermi surface of high-mobility LaAlO3_3/SrTiO3_3 interfaces using Shubnikov-de Haas oscillations. Our analysis of the oscillation pattern underscores the key role played by the Rashba spin-orbit interaction brought about by the breaking of inversion symmetry, as well as the dominant contribution of the heavy dxzd_{xz}/dyzd_{yz} orbitals on electrical transport. We furthermore bring into light the complex evolution of the oscillations with the carrier density, which is tuned by the field effect

    Growth-induced electron mobility enhancement at the LaAlO3_3/SrTiO3_3 interface

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    We have studied the electronic properties of the 2D electron liquid present at the LaAlO3_3/SrTiO3_3 interface in series of samples prepared at different growth temperatures. We observe that interfaces fabricated at 650{\deg}C exhibit the highest low temperature mobility (10000 cm2/Vs\approx 10000 \textrm{ cm}^2/\textrm{Vs}) and the lowest sheet carrier density (5×1012 cm2\approx 5\times 10^{12} \textrm{ cm}^{-2}). These samples show metallic behavior and Shubnikov-de Haas oscillations in their magnetoresistance. Samples grown at higher temperatures (800-900{\deg}C) display carrier densities in the range of 25×1013 cm2\approx 2-5 \times 10^{13} \textrm{ cm}^{-2} and mobilities of 1000 cm2/Vs\approx 1000 \textrm{ cm}^2/\textrm{Vs} at 4K. Reducing their carrier density by field effect to 8×1012 cm28\times 10^{12} \textrm{ cm}^{-2} lowers their mobilites to 50 cm2/Vs\approx 50 \textrm{ cm}^2/\textrm{Vs} bringing the conductance to the weak-localization regime

    Shear effects in lateral piezoresponse force microscopy at 180^\circ ferroelectric domain walls

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    In studies using piezoresponse force microscopy, we observe a non-zero lateral piezoresponse at 180^\circ domain walls in out-of-plane polarized, c-axis-oriented tetragonal ferroelectric Pb(Zr0.2_{0.2}Ti0.8_{0.8})O3_3 epitaxial thin films. We attribute these observations to a shear strain effect linked to the sign change of the d33d_{33} piezoelectric coefficient through the domain wall, in agreement with theoretical predictions. We show that in monoclinically distorted tetragonal BiFeO3_3 films, this effect is superimposed on the lateral piezoresponse due to actual in-plane polarization, and has to be taken into account in order to correctly interpret the ferroelectric domain configuration.Comment: 4 pages, 3 figure

    Magneto-transport study of top- and back-gated LaAlO3_3/SrTiO3_3 heterostructures

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    We report a detailed analysis of magneto-transport properties of top- and back-gated LaAlO3_3/SrTiO3_3 heterostructures. Efficient modulation in magneto-resistance, carrier density, and mobility of the two-dimensional electron liquid present at the interface is achieved by sweeping top and back gate voltages. Analyzing those changes with respect to the carrier density tuning, we observe that the back gate strongly modifies the electron mobility while the top gate mainly varies the carrier density. The evolution of the spin-orbit interaction is also followed as a function of top and back gating.Comment: 15 pages, 6 figure

    Tunable Rashba spin-orbit interaction at oxide interfaces

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    The quasi-two-dimensional electron gas found at the LaAlO3/SrTiO3 interface offers exciting new functionalities, such as tunable superconductivity, and has been proposed as a new nanoelectronics fabrication platform. Here we lay out a new example of an electronic property arising from the interfacial breaking of inversion symmetry, namely a large Rashba spin-orbit interaction, whose magnitude can be modulated by the application of an external electric field. By means of magnetotransport experiments we explore the evolution of the spin-orbit coupling across the phase diagram of the system. We uncover a steep rise in Rashba interaction occurring around the doping level where a quantum critical point separates the insulating and superconducting ground states of the system
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