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Tunable strontium titanate terahertz all-dielectric metamaterials
Journal of Physics D: Applied Physics, 2020Based on SrTiO3 (STO) elliptical metamaterials (MMs) structures, the tunable propagation properties have been systematically investigated in the THz regime, including the effects of temperatures, incident angles, operation frequencies, and graphene Fermi
Xiaoyong He, F. Lin, Feng Liu, W. Shi
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Journal of Applied Physics, 2013
In order to enhance the permittivity and tunability of the dielectric component, a thin film dielectric composite consisting of a radio frequency sputtered SrTiO3 (STO) buffer layer and metalorganic solution deposited Mg-doped BaxSr1−xTiO3 (Mg-BST) thin film overgrowth was developed using affordable industry standard processes and materials. The effect
M. W. Cole +7 more
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In order to enhance the permittivity and tunability of the dielectric component, a thin film dielectric composite consisting of a radio frequency sputtered SrTiO3 (STO) buffer layer and metalorganic solution deposited Mg-doped BaxSr1−xTiO3 (Mg-BST) thin film overgrowth was developed using affordable industry standard processes and materials. The effect
M. W. Cole +7 more
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Preparation of Barium Titanate/Strontium Titanate Multilayered Nanoparticles
Key Engineering Materials, 2011Nucleation and particle growth conditions of barium titanate (BaTiO3, BT) were investigated for preparation of the BT/strontium titanate (SrTiO3, ST) multilayered nanoparticles. The conditions with and without BT nucleation were clarified. Epitaxial growth of the BT layer on the ST substrate particles was studied using both conditions. The formation of
Takayuki Goto +5 more
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Driving strontium titanate ferroelectric
Science, 2019Physics Hidden phases are metastable collective states of matter that are typically not accessible on equilibrium phase diagrams. Nova et al. used infrared pulses to excite higher-frequency lattice modes that drive the crystal into a metastable ferroelectric phase, a phase that can persist for many hours. X. Li et al. used terahertz fields to drive the
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Scaling behaviour of strontium titanate
Journal of Physics: Condensed Matter, 1999The dielectric susceptibility, = ´ - i´´, of nominally pure strontium titanate is measured between 4 and 70 K as a function of an external bias field. Static scaling analysis of the susceptibility reveals a very good scaling behaviour with a quasi-critical exponent a = /( - 1) = 2.00 ± 0.02 extracted consistently from two different experiments.
J Dec, W Kleemann, B Westwanski
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CrysteEngComm, 2019
Strontium titanate (SrTiO3) with a perovskite structure is widely applied to hydrogen production by photolysis water splitting.
Yuan Ma +10 more
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Strontium titanate (SrTiO3) with a perovskite structure is widely applied to hydrogen production by photolysis water splitting.
Yuan Ma +10 more
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1997
Publisher Summary Strontium Titanate (SrTiO3) crystallizes in the cubic perovskite structure. Therefore, the optical properties of this material are isotropic. SrTiO3 behaves like a ferroelectric material in the paraelectric phase. This property is referred to as incipient ferroelectric.
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Publisher Summary Strontium Titanate (SrTiO3) crystallizes in the cubic perovskite structure. Therefore, the optical properties of this material are isotropic. SrTiO3 behaves like a ferroelectric material in the paraelectric phase. This property is referred to as incipient ferroelectric.
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Electronic Transport in Strontium Titanate
Physical Review, 1964The conductivity and the Hall and Seebeck coefficients of reduced and doped strontium titanate were measured over the temperature range 4.2-300\ifmmode^\circ\else\textdegree\fi{}K. An average effective mass of about 10 ${m}_{0}$ was deduced from these experiments.
H. P. R. Frederikse +2 more
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Unique Features of Strontium Titanate
Ferroelectrics, 2005Some novel features of strontium titanate are presented. First, it reveals secondary ferroicity when exposed to an external electric field in its tetragonal paraelectric state. It is shown on isotopically doped SrTi 18 O 3 (STO18) that odd-oriented ferroelastic domains can be switched under anomalously large electrostriction such as to create a perfect
J. Dec +3 more
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