204 research outputs found
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Phase diagram studies for the growth of (Mg,Zr):SrGa12O19 crystals
By differential thermal analysis, a concentration field suitable for the growth of Zr, Mg co-doped strontium hexagallate crystals was observed that corresponds well with known experimental results. It was shown that the melting point of doped crystal is ca. 60 K higher than that of undoped crystals. This higher melting points indicate hexagallate phase stabilization by Zr, Mg co-doping and increase the growth window of (Mg,Zr):SrGa12O19, compared to undoped SrGa12O19 that grows from SrO–Ga2O3 melts
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REScO3 Substrates—Purveyors of Strain Engineering
The thermodynamic and crystallographic background for the development of substrate crystals that are suitable for the epitaxial deposition of biaxially strained functional perovskite layers is reviewed. In such strained layers the elastic energy delivers an additional contribution to the Gibbs free energy, which allows the tuning of physical properties and phase transition temperatures to desired values. For some oxide systems metastable phases can even be accessed. Rare-earth scandates, REScO3, are well suited as substrate crystals because they combine mechanical and chemical stability in the epitaxy process with an adjustable range of pseudo-cubic lattice parameters in the 3.95 to 4.02 Å range. To further tune the lattice parameters, chemical substitution for the RE or Sc is possible. © 2019 The Authors. Published by WILEY-VCH Verlag GmbH & Co. KGaA, Weinhei
Ti-Sr antisite : An abundant point defect in SrTiO3
We present a systematic study of the positron lifetime as a function of measurement temperature in strontium titanate ( SrTiO 3) single crystals grown in different conditions and by different synthesis methods. We combine our experimental results with state-of-the-art theoretical calculations of positron annihilation parameters. We find that the essentially omnipresent 180-190ps lifetime component is most likely the Ti Sr antisite defect, possibly coupled with one or more oxygen vacancies, supporting the importance of the Ti Sr antisite related defects in SrTiO 3.Peer reviewe
Fingerprints of carbon defects in vibrational spectra of gallium nitride (GaN) consider-ing the isotope effect
This work examines the carbon defects associated with recently reported and
novel peaks of infrared (IR) absorption and Raman scattering appearing in GaN
crystals at carbon () doping in the range of concentrations from
to . 14 unique vibrational modes of defects
are observed in GaN samples grown by hydride vapor phase epitaxy (HVPE) and
then compared with defect properties predicted from first-principles
calculations. The vibrational frequency shift in two enriched samples
related to the effect of the isotope mass indicates six distinct configurations
of the carbon-containing point defects. The effect of the isotope replacement
is well reproduced by the density functional theory (DFT) calculations.
Specific attention is paid to the most pronounced defects, namely tri-carbon
complexes() and carbon substituting for nitrogen . The position
of the transition level (+/0) in the bandgap found for defects by
DFT at 1.1 eV above the valence band maximum, suggest that
provides compensation of . defects are observed to be
prominent, yet have high formation energies in DFT calculations. Regarding
defects, it is shown that the host Ga and N atoms are involved in the
defect's delocalized vibrations and significantly affect the isotopic frequency
shift. Much more faint vibrational modes are found from di-atomic carbon-carbon
and carbon-hydrogen (C-H) complexes. Also, we note changes of vibrational mode
intensities of , , C-H, and defects in the IR
absorption spectra upon irradiation in the defect-related UV/visible absorption
range. Finally, it is demonstrated that the resonant enhancement of the Raman
process in the range of defect absorption above 2.5 eV enables the detection of
defects at carbon doping concentrations as low as
Experimental Hall electron mobility of bulk single crystals of transparent semiconducting oxides
We provide a comparative study of basic electrical properties of bulk single crystals of transparent semiconducting oxides (TSOs) obtained directly from the melt (9 compounds) and from the gas phase (1 compound), including binary (β-Ga2O3, In2O3, ZnO, SnO2), ternary (ZnSnO3, BaSnO3, MgGa2O4, ZnGa2O4), and quaternary (Zn1−xMgxGa2O4, InGaZnO4) systems. Experimental outcome, covering over 200 samples measured at room temperature, revealed n-type conductivity of all TSOs with free electron concentrations (ne) between 5 × 1015 and 5 × 1020 cm−3 and Hall electron mobilities (μH) up to 240 cm2 V−1 s−1. The widest range of ne values was achieved for β-Ga2O3 and In2O3. The most electrically conducting bulk crystals are InGaZnO4 and ZnSnO3 with ne > 1020 cm−3 and μH > 100 cm2 V−1 s−1. The highest μH values > 200 cm2 V−1 s−1 were measured for SnO2, followed by BaSnO3 and In2O3 single crystals. In2O3, ZnO, ZnSnO3, and InGaZnO4 crystals were always conducting, while others could be turned into electrical insulators.Leibniz-Gemeinschaft
http://dx.doi.org/10.13039/501100001664Leibniz-Institut für Kristallzüchtung (IKZ) im Forschungsverbund Berlin e.V. (3477)Peer Reviewe
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Experimental Hall electron mobility of bulk single crystals of transparent semiconducting oxides
We provide a comparative study of basic electrical properties of bulk single crystals of transparent semiconducting oxides (TSOs) obtained directly from the melt (9 compounds) and from the gas phase (1 compound), including binary (β-Ga2O3, In2O3, ZnO, SnO2), ternary (ZnSnO3, BaSnO3, MgGa2O4, ZnGa2O4), and quaternary (Zn1−xMgxGa2O4, InGaZnO4) systems. Experimental outcome, covering over 200 samples measured at room temperature, revealed n-type conductivity of all TSOs with free electron concentrations (ne) between 5 × 1015 and 5 × 1020 cm−3 and Hall electron mobilities (μH) up to 240 cm2 V−1 s−1. The widest range of ne values was achieved for β-Ga2O3 and In2O3. The most electrically conducting bulk crystals are InGaZnO4 and ZnSnO3 with ne > 1020 cm−3 and μH > 100 cm2 V−1 s−1. The highest μH values > 200 cm2 V−1 s−1 were measured for SnO2, followed by BaSnO3 and In2O3 single crystals. In2O3, ZnO, ZnSnO3, and InGaZnO4 crystals were always conducting, while others could be turned into electrical insulators
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