研究目的
Studying the lattice dynamics of two-layer BaTiO3/Ba50Sr50TiO3 (BT/BST) and three-layer BaTiO3/Ba50Sr50TiO3/SrTiO3 (BT/BST/ST) superlattices grown onto MgO substrates via the pulsed laser deposition. A comparative analysis of their polarized Raman spectra, particularly, within the soft-mode (E(1TO)) range, is of particular interest to establish the structural peculiarities caused by misfits of constituting layers.
研究成果
For a three-layer BaTiO3/Ba50Sr50TiO3/SrTiO3 system, there was established a more pronounced shift of E(TO) and A1(TO) soft mode components in comparison with BaTiO3/Ba50Sr50TiO3. Spectral peculiarities, found for BaTiO3/Ba50Sr50TiO3/SrTiO3 superlattice, evidenced an abrupt increase in 2D compression of BT layers, being in conjugation with ST ones, as well as more pronounced tetragonality of its unit cell against BaTiO3/Ba50Sr50TiO3 structure, presumably owing to substantially risen temperature of transition from ferroelectric to paraelectric phase.
研究不足
The study does not specially consider the effect of MgO substrate on the superlattices, although the influence of substrate/film interface on the behavior of soft modes has been demonstrated in other studies.
1:Experimental Design and Method Selection:
BaTiO3/Ba50Sr50TiO3 (BT/BST) and BaTiO3/Ba50Sr50TiO3/SrTiO3 (BT/BST/ST) SLs were grown onto (001) single-crystal MgO substrates via the pulsed laser deposition by the alternating focus of a laser beam on BT, BST, and ST targets.
2:Sample Selection and Data Sources:
The modulation period Λ of BT/BST layers in a two-layer BT/BST SL was 130 ? (the thickness of individual layers was 65 ?) and that of BT/BST/ST layers in a three-layer BT/BST/ST SL enriched 150 ? (resulting in a 50-? thickness of the constituting layers). The total thickness of heterostructures was 1 μm.
3:List of Experimental Equipment and Materials:
Raman spectra were excited at room temperature with an argon laser (λ =
4:5 nm) and recorded by an Invia Reflex Renishaw spectrometer equipped with a near-excitation tunable (NExT) filter for the low-frequency spectral range analysis. The exciting radiation was focused atop a sample with a Leica optical microscope in a spot with a diameter of 2 μm. Experimental Procedures and Operational Workflow:
5 Polarized Raman spectra were collected on samples oriented with respect to crystallographic axes of substrates as X || 100, Y || 010, and Z ||
5:Spectra with pronounced E-type soft modes were acquired in the side-view backscattering, at which the wave vector of the incident beam is parallel to the substrate, and the polarization of incident and scattered light is parallel or perpendicular to the Z axis of the film. Data Analysis Methods:
0 The analysis focused on the behavior of E(1TO) line which is attributed to the transverse optical vibration of soft modes E that split in various components with reducing symmetry of ABO3-type perovskites.
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