Abstract:A single-crystalline double-layered structure of a pure (80-microm)/doped (39-microm)/pure Bi(12)SiO(20) (BSO) substrate was grown for the first time by a new liquid-phase epitaxial growth to form an optical waveguide. The waveguide layer is BSO doped with CaCO(3) (0.1 wt. %) and Ga(2)O(3) (0.197 wt. %) and has a refractive index 0.07% higher than the substrate. The optical absorption coefficients were decreased by more than 1 order of magnitude by doping with the elements Ca and Ga. The high-sensitive photoco… Show more
“…Their experiments showed that the bismuth oxide phase at high temperature (δ-Bi 2 O 3 (FCC)) can be stabilized by SiO 2 and kept at room temperature by heating the bismuth silicon oxide to 800-1000 • C for 15-60 min and then quenching. However, their results were reproduced neither by Levin and Roth [10], who reported the phase diagram of Bi 2 O 3 -SiO 2 in 1964, nor cited by Tada et al [16] in 1982 although most of this phase diagram was conjectural. According to their phase diagram, there is no metastable δ-Bi 12 SiO 20 which could be solidified from the stoichiometric melt of 6Bi 2 O 3 • SiO 2 .…”
Solidification characteristics of metastable and stable from melts were systematically investigated by x-ray diffraction, differential thermal analysis and thermogravimetry. The experimental results show that the solidification either of metastable or of stable directly from melts appears to be dependent both on the melt temperature and on the cooling rate. In general, high melt temperatures and high cooling rates tend to solidify metastable . Otherwise, low melt temperatures and low cooling rates tend to solidify stable . To produce stable single-crystal , the melt temperature should be controlled to be less than and the cooling rate near the solidifying temperature should be less than .
“…Their experiments showed that the bismuth oxide phase at high temperature (δ-Bi 2 O 3 (FCC)) can be stabilized by SiO 2 and kept at room temperature by heating the bismuth silicon oxide to 800-1000 • C for 15-60 min and then quenching. However, their results were reproduced neither by Levin and Roth [10], who reported the phase diagram of Bi 2 O 3 -SiO 2 in 1964, nor cited by Tada et al [16] in 1982 although most of this phase diagram was conjectural. According to their phase diagram, there is no metastable δ-Bi 12 SiO 20 which could be solidified from the stoichiometric melt of 6Bi 2 O 3 • SiO 2 .…”
Solidification characteristics of metastable and stable from melts were systematically investigated by x-ray diffraction, differential thermal analysis and thermogravimetry. The experimental results show that the solidification either of metastable or of stable directly from melts appears to be dependent both on the melt temperature and on the cooling rate. In general, high melt temperatures and high cooling rates tend to solidify metastable . Otherwise, low melt temperatures and low cooling rates tend to solidify stable . To produce stable single-crystal , the melt temperature should be controlled to be less than and the cooling rate near the solidifying temperature should be less than .
“…The processes for epitaxial growth of Bi 12 MO 20 plates and waveguides were described in [81][82][83][84][85][86][87]. Single-crystal BSO ribbons can be produced by the Stepanov method or EFG process [88][89][90].…”
Section: Preparation Of Bi 12 Mo 20 -Based Epitaxial Structures and Pmentioning
confidence: 99%
“…In epitaxial growth, special attention must be paid to the surface condition of the substrate and the homogeneity of the hot zone on the melt surface. A similar process was used by Tada et al [82] to produce BSO layers codoped with Al and Ca. LPE growth of bismuth titanate layers, undoped and doped with V, Cu, and Ca + Ga, on (100), (110), and (111) BGO and BSO substrates (20 × 30 × 2 mm) was described by Bondarev et al [84] and Kargin et al [87].…”
Section: Preparation Of Bi 12 Mo 20 -Based Epitaxial Structures and Pmentioning
The main processes for preparing bulk single crystals and films of photorefractive and piezoelectric Bi 12 M x O 20 ± δ (M = Group II-VIII elements) sillenite compounds are considered. Experimental data are summarized on the crystal growth of Bi 12 M x O 20 ± δ from the melt and under hydrothermal conditions, and the key morphological features of sillenites are analyzed. Various types of macroscopic growth defects in sillenite-type crystals are described, and their origin is discussed. The compositions of second-phase inclusions in undoped and doped (Group I-VIII elements) Bi 12 SiO 20 , Bi 12 GeO 20 , and Bi 12 TiO 20 single crystals are presented, and the main physicochemical properties of various Bi 12 M x O 20 ± δ crystals are summarized.
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