Effects of in-plane compressive stress on electrical properties of (Ba,Sr)TiO3 thin film capacitors prepared by on- and off-axis rf magnetron sputtering
Abstract:This study investigated the structural and electrical properties of (Ba,Sr)TiO3 (BST) thin film capacitors with thicknesses ranging from 18 to 215 nm, which were prepared by on- and off-axis rf magnetron sputtering technique on Pt/SiO2/Si substrates. The deposition rate and cation composition ratios of the films were controlled to be the same regardless of the sputtering geometry. All the films show elongations in the out-of-plane lattice spacing, suggesting the presence of compressive stress with a smaller va… Show more
“…Obviously, a narrow band gap is beneficial to enhance the photovoltaic effect of BFO. However, polycrystalline BFO films prepared by a conventional chemical solution deposition process (CSD) based on using 2-methoxyethanol and acetic acid as solvent mainly show pseudocubic structure [8,12] due to tensile stress [13] within the ferroelectric films. As we know, except the kinds of substrates, the kinds of solvents in the precursor solution also have high effect on the structure of the as-prepared films.…”
“…Obviously, a narrow band gap is beneficial to enhance the photovoltaic effect of BFO. However, polycrystalline BFO films prepared by a conventional chemical solution deposition process (CSD) based on using 2-methoxyethanol and acetic acid as solvent mainly show pseudocubic structure [8,12] due to tensile stress [13] within the ferroelectric films. As we know, except the kinds of substrates, the kinds of solvents in the precursor solution also have high effect on the structure of the as-prepared films.…”
“…Of particular note is a process referred to as "shot peening", in which compressive strain arises as a result of the sample being bombarded by energetic particles during growth. Compressive in-plane strain in sputtered oxide films is often attributed to this effect 28,29 . Thermal strain from the mismatch of the coefficient of thermal expansion between the film and substrate may also be present.…”
Vanadium dioxide (VO 2 ) undergoes a phase transition between an insulating monoclinic (M 1 ) phase and a conducting rutile phase. Like other correlated electron systems, the properties of VO 2 can be extremely sensitive to small changes in external parameters such as strain. In this work, we investigate a compressively strained VO 2 film grown on [001] quartz substrate in which the phase transition temperature (T c ) has been depressed to 325K from the bulk value of 340K. Infrared and optical spectroscopy reveals that the lattice dynamics of this strained film are very similar to unstrained VO 2 . However, some of the electronic inter-band transitions of the strained VO 2 film are significantly shifted in energy from those in unstrained VO 2 . That the lattice dynamics remain largely unchanged, while the T c and some of the electronic inter-band transitions differ substantially from the bulk values highlight the role of electronic correlations in driving this metal-insulator phase transition.
“…However, when thin BST films is being produced, a common problem involving the decrease of dielectric constant with respect to film thickness is still an unsolved problem [10]. At present, there are assumptions that such phenomenon is caused by the presence of an intrinsic dead layer [11], defects leading to electrode polarization [12], and film stress from the substrate [13]. Thus, accurately quantifying the characteristics such as the thickness dependence of the dielectric constant in the ferroelectric film and understanding its origin is an important task to be solved before practical applications.…”
Ferroelectric Ba 0.5 Sr 0.5 TiO 3 (BST) films were prepared on Pt/Ti/SiO 2 /Si substrates by the sol-gel process. The films were spin-coated at 2000 rpm for 30 secs and then pyrolysed for 5 mins at the temperature of 350 • C. This coating procedure was repeated for 3, 4, 5 and 6 times to obtain BST films with different thicknesses. After coating the films with the desired repetition times, the films were finally annealed in a conventional furnace at temperatures ranging from 600 • C to 800 • C with a 50 • C interval in between. The films obtained with an annealing procedure of 750 • C were polycrystalline with the presence of an impurity BaCO 3 phase. The capacitance and leakage current were measured and used to extract information on the metal-BST interface. With the series capacitance model and modified Schottky emission equation, the thickness of the dead layers for Au/BST and Pt/BST interfaces were calculated to be less than 6 nm and 5 nm, respectively.
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