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1.
Pb(Mg1/3 Ta2/3 )0.7 Ti0.3 O3 thin films of single perovskite phase were successfully synthesized by using the RF sputtering deposition technique, followed by post-thermal annealing. While the perovskite structure of Pb(Mg1/3 Ta2/3 )0.7 Ti0.3 O3 is rather unstable, phase evolution in the thin films was manipulated by controlling both working pressure during the sputtering process and post-thermal annealing temperature. The desirable perovskite phase was promoted by increasing the working pressure in the range of 10–25 mTorr, followed by thermal annealing at 600°C. The ferroelectric, dielectric, and polarization behaviors of Pb(Mg1/3 Ta2/3 )0.7 Ti0.3 O3 films were characterized over a wide range of frequencies. They are strongly affected by the film thickness, where the relative permittivity and remanent polarization increase, while the coercive field decreases with increasing film thickness in the range of 115–360 nm. 相似文献
2.
Xingsen Gao Zhaohui Zhou Junmin Xue John Wang 《Journal of the American Ceramic Society》2005,88(4):1037-1040
Effects of excess Bi2 O3 content on formation of (Bi3.15 Nd0.85 )Ti3 O12 (BNT) films deposited by RF sputtering were investigated. The microstructures and electrical properties of BNT thin films are strongly dependent on the excess Bi2 O3 content and post-sputtering annealing temperature, as examined by XRD, SEM, and P – E hysteresis loops. A small amount of excess bismuth improves the crystallinity and therefore polarization of BNT films, while too much excess bismuth leads to a reduction in polarization and an increase in coercive field. P – E loops of well-established squareness were observed for the BNT films derived from a moderate amount of Bi2 O3 excess (5 mol%), where a remanent polarization 2P r of 25.2 μC/cm2 and 2E c of 161.5 kV/cm were shown. A similar change in dielectric constant with increasing excess Bi2 O3 content was also observed, with the highest dielectric constant of 304.1 being measured for the BNT film derived from 5 mol% excess Bi2 O3 . 相似文献
3.
Elena R. Andrievskaya Lidia M. Lopato Vasily P. Smirnov 《Journal of the American Ceramic Society》1996,79(3):714-720
A mathematical model of the liquidus surface based on a reduced polynomial method was proposed for the system HfO2 -Y2 O3 -Er2 O3 . The results of calculations according to this model agree fairly well with the experimental data. Phase equilibria in the system HfO2 -Y2 O3 -Er2 O3 were studied on melted (as-cast) and annealed samples using X-ray diffraction (at room and high temperatures) and micro-structural and petrographic analyses. The crystallization paths in the system HfO2 -Y2 O3 -Er2 O3 were established. The system HfO2 -Y2 O3 -Er2 O3 is characterized by the formation of extended solid solutions based on the fluorite-type (F) form of HfO2 and cubic (C) and hexagonal (H) forms of Y2 O3 and Er2 O3 . The boundary curves of these solid solutions have the minima at 2370°C (15. 5 mol% HfO2 , 49. 5 mol% Y2 O3 ) and 2360°C (10. 5 mol% HfO2 , 45. 5 mol% Y2 O3 ). No compounds were found to exist in the system investigated. 相似文献
4.
John B. Bates Nancy J. Dudney Chris F. Luck Brian C. Sales Raymond A. Zuhr J. David Robertson 《Journal of the American Ceramic Society》1993,76(4):929-943
Amorphous lithium electrolyte thin films, xLi2 O·ySiO2 ·zP2 O5 , were deposited by rf magnetron sputtering of pure and mixed-phase lithium silicate, lithium phosphate, SiO2 , Li2 O, and Li2 CO3 targets, and their compositions were determined using proton-induced y -ray emission spectroscopy, energy-dispersive X-ray analysis, Rutherford backscattering spectrometry, and atomic-emission spectroscopy. The deposition conditions were chosen to assure thermalization of the sputtered flux, which proved to be necessary in order to obtain a homogeneous distribution of Si and P in the films. Optical absorption and ac impedance measurements showed that glass-in-glass phase separation occurred in a large SiO2 -rich domain of the composition diagram. In contrast to bulk glasses, all of the Li2 O–SiO2 films were phase-separated, including those with lithia contents larger than lithium disilicate. High-performance liquid chromatography measurements revealed that, analogous to bulk glasses, the addition of SiO2 to Li2 O-P2 O5 compositions reduced the number of phosphate anion dimers, trimers, and higher anion polymers in the films through the formation of -Si-O-P-bonds. However, in contrast to bulk glasses, the distribution of phosphate anion polymers followed closely the Flory distribution, with the fraction of anion polymers decreasing monotonically with increasing chain length. 相似文献
5.
The coordination and bond character of the cations in amorphous SiO2 -Al2 O3 films prepared by rf sputtering were examined by studying chemical shifts in the SiK and AlK X-ray emission spectra. The coordination number of Si ions in these films was always 4, regardless of composition, whereas the average coordination number of Al ions changed from 4 to 5, depending onAl2 O3 content. TheSi-O-Al bond type seemed to appear as Al2 O3 was introduced into amorphous SiO2 films or vice versa. 相似文献
6.
The quenching technique was used to study subliquidus and subsolidus phase relations in the pseudobinary system Na2 Ti2 Si2 O11 -Na2 Ti2 Si2 O9 . Both narsarukite (Na2 TiSi4 O11 ) and lorenzenite (Na2 Ti2 Si2 O9 ) melt incongruently. Narsarsukite melts at 911°±°C to SiO2 +liquid, with the liquidus at 1016°C. Lorenzenite melts at 910°±5°C to Na2 Ti6 O13 +liquid; Na2 Ti6 O13 reacts with liquid to form TiO2 and is thus consumed by 985°±5°C. The liquidus occurs at 1252°C. 相似文献
7.
Kentaro Fukuda Teiichi Hanada Setsuhisa Tanabe Takeshi Yao 《Journal of the American Ceramic Society》2002,85(4):915-920
Amorphous films in the system Al2 O3 –Y2 O3 were prepared by the rf sputtering method in the range of 0–76 mol% Y2 O3 , and their density, refractive index, and elastic constants were measured. All of the physical properties of the amorphous Al2 O3 –Y2 O3 films had a similar compositional dependence; that is, they increased continuously, but not linearly with increasing Y2 O3 content. To confirm the coordination states of aluminum and yttrium ions in the amorphous Al2 O3 –Y2 O3 films, the Al K α X-ray emission spectra and the X-ray absorption near edge structures (XANES) were measured. The average coordination number of aluminum ions in the amorphous films containing up to about 40 mol% Y2 O3 content was 5, that is a mixture of 4-fold- and 6-fold-coordinated states. In the region of more than about 50 mol% Y2 O3 , the fraction of the 6-fold-coordinated aluminum ions increased with increasing Y2 O3 content, while the results led to the conclusion that the coordination number of yttrium ions was always 6, regardless of composition. These results indicate that, in amorphous films in the system Al2 O3 –Y2 O3 , the change of the coordination state of aluminum ions has an important effect on physical properties. 相似文献
8.
The standard Gibbs free energies of formation of CuAlO2 and CuAl2 O4 were determined in the range 700° to 1100°C, using emf measurements on the galvanic cells (1) Pt,CuO +] Cu2 O/CaO-ZrO2 /O2 ,Pt; (2) Pt,Cu +] CuAlO2 +] Al2 O3 /CaO-ZrO2 / Cu +] Cu2 O,Pt; and (3) Pt,CuAl2 O4 +] CuAlO2 +]Al2 O3 /CaO-ZrO2 /O2 ,Pt. The results are compared with published information on the stability of these compounds. The entropy of transformation of CuO from tenorite to the rock-salt structure is evaluated from the present results and from earlier studies on the entropy of formation of spinels from oxides of the rock-salt and corundum structures. The temperatures corresponding to 3-phase equilibria in the system Cu2 O-CuO-Al2 O3 at specified O2 pressures calculated from the present results are discussed in reference to available phase diagrams. 相似文献
9.
The crystallization of MgO-Al2 O3 -SiO2 -ZrO2 glasses at 1000°C was studied. Isothermal heat treatments of a cordierite-based glass (2MgO.2Al2 O3 .5SiO2 = Mg2 Al4 Si5 O18 ) with 7 wt% ZrO2 produced surface crystallization of α-cordierite and tetragonal ZrO2 ( t -ZrO2 ). These phases advanced into the glass by cocrystallization of t -ZrO2 rods in an α-cordierite matrix with a well-defined orientation relation. The t -ZrO2 rods were unstable with respect to diffusional breakup (a Rayleigh instability) and decomposed into rows of aligned ellipsoidal and spheroidal particles. The t -ZrO2 was very resistant to transformation to monoclinic symmetry. With a similar glass containing 15 wt% ZrO2 , surface crystallization of α-cordierite and t -ZrO2 was accompanied by internal crystallization of t -ZrO2 dendrites. Transformation of the dendrites to mono-clinic symmetry was observed under some conditions. 相似文献
10.
Yoshihito Mizoguchi Masahiro Kagawa Yasuhiko Syono Toshio Hirai 《Journal of the American Ceramic Society》2001,84(3):651-653
Thin films of yttrium aluminum garnet (YAG, Y3 Al5 O12 ) and yttrium iron garnet (YIG, Y3 Fe5 O12 ) were synthesized on single-crystal Al2 O3 substrates by a modification of spray pyrolysis using a high-temperature inductively coupled plasma at atmospheric pressure (spray–ICP technique). Using this technique, films could be grown at faster rates (0.12 μm/min for YAG and 0.10 μm/min for YIG) than using chemical vapor deposition (0.005–0.008 μm/min for YAG) or sputtering (0.003–0.005 μm/min for YIG). The films were dense and revealed a preferred orientation of (211). The growth of YIG was accompanied by coprecipitation of α-Fe2 O3 . The coprecipitation, however, could be largely suppressed by preliminary formation of a Y2 O3 layer on the substrate. 相似文献
11.
The phase relations in the systems MgO-Y2 O3 -ZrO2 and CaO-MgO-ZrO2 were established at 1220° and 1420°C. The system MgO-Y2 O3 -ZrO2 possesses a much-larger cubic ZrO2 solid solution phase field than the system CaO-MgO-ZrO2 at both temperatures. The ordered δ phase (Zr3 Y4 O12 ) was found to be stable in the system ZrO2 -Y2 O3 at 1220°C. Two ordered phases φ1 (CaZr4 O9 ) and φ2 (Ca6 Zr19 O44 ) were stable at 1220°C in the system ZrO2 -CaO. At 1420°C no ordered phase appears in either system, in agreement with the previously determined temperature limits of the stability for the δ, φ1 , and φ2 phases. The existence of the compound Mg3 Yz O6 could not be confirmed. 相似文献
12.
Subsolidus phase relations were established in the system Si3 N4 -SiO2 -Y2 O3 . Four ternary compounds were confirmed, with compositions of Y4 Si2 O7 N2 , Y2 Si3 O3 N4 , YSiO2 N, and Y10 (SiO4 )6 N2 . The eutectic in the triangle Si3 N4 -Y2 Si2 O7 -Y10 (SiO4 )6 N2 melts at 1500°C and that in the triangle Si2 N2 O-SiO2 -Y2 Si2 O7 at 1550°C. The eutectic temperature of the Si3 N4 -Y2 Si2 O7 join was ∼ 1520°C. 相似文献
13.
Zn2 SnO4 , an inverse spinel, and ZnFe2 O4 , a normal spinel, form a complete series of solid solutions in the system ZnO-Fe2 O3 3nO2 . The variation of cell dimensions with composition varies from 0.8439 nm (ZnS2 nO4 ) to 0.8660 nm (ZnS2 nO4 ) and exhibits a positive deviation from a linear relationship. Mg2 SnO4 and MgFe2 O4 , both predominantly inverse in nature, have only an incomplete series. 相似文献
14.
Steven A. Markgraf Shiv K. Sharma Amar S. Bhalla 《Journal of the American Ceramic Society》1992,75(9):2630-2632
Raman spectra are reported for fresnoite (Ba2 Ti(Si,Ge)2 O8 glasses, and comparison is made between the Raman spectra of the corresponding crystalline powders and glasses of Ba2 TiSi2 O8 and Ba2 TiGe2 O8 . The Ba2 TiGe2 O8 glass spectra show correspondence with the Ba2 TiGe2 O8 crystalline Raman spectra; the v s (Ge–O–Ge) mode occurs at 518 cm−1 in the glass and at 521 cm−1 in the crystalline material. Five-fold coordinated titanium is the majority species present in the Ba2 TiGe2 O8 glass as revealed by a strong band at 824 cm−1 in the I glass spectrum. The Ba2 TiSi2 O8 glass spectra are similar to the Ba2 TiSi2 O8 crystalline spectrum; the strongest band is found at 836 cm−1 in the I glass spectrum. Through comparison with the previous Raman data of other titania silicate glasses, we conclude that the Ba2 TiSi2 O8 glass has a structure similar to the crystalline phase. 相似文献
15.
Tsuyoshi Honma Yasuhiko Benino Takumi Fujiwara Takayuki Komatsu Ryuji Sato 《Journal of the American Ceramic Society》2005,88(4):989-992
The glass formation region, crystalline phases, second harmonic (SH) generation, and Nd:yttrium aluminum garnet (YAG) laser-induced crystallization in the Sm2 O3 –Bi2 O3 –B2 O3 system were clarified. The crystalline phases of Bi4 B2 O9 , Bi3 B5 O12 , BiBO3 , Sm x Bi1− x BO3 , and SmB3 O6 were formed through the usual crystallization in an electric furnace. The crystallized glasses consisting of BiBO3 and Sm x Bi1− x BO3 showed SH generations. The formation of the nonlinear optical BiB3 O6 phase was not confirmed. The formation (writing) region of crystal lines consisting of Sm x Bi1− x BO3 by YAG laser irradiation was determined, in which Sm2 O3 contents were∼10 mol%. The present study demonstrates that Sm2 O3 –Bi2 O3 –B2 O3 glasses are promising materials for optical functional applications. 相似文献
16.
Shara S. Shoup ‡ Carlos E. Bamberger § Richard G. Haire 《Journal of the American Ceramic Society》1996,79(6):1489-1493
The compounds SrPu2 Ti4 O12 , Pu2 Ti3 O8.79 , and Pu2 Ti2 O7 , where plutonium is in the (III) oxidation state, were prepared and identified via X-ray diffraction (XRD). The solid solubility limit of Pu2 Ti2 O7 in Ln2 Ti2 O7 (Ln = Gd, Er, or Lu) was also studied via XRD; it was determined that the solubility of Pu2 Ti2 O7 increased as the radius of the lanthanide ion in the host compound decreased. Attempts to synthesize Sr2 Pu2 Ti5 O16 and Sr2 Ce2–y Puy Ti5 O16 solid solutions, where plutonium is in the (IV) oxidation state, were unsuccessful. 相似文献
17.
Quadrupole interactions of 11 B and 27 Al in SiO2 -B2 O3 -Al2 O3 -R2 O glass systems were investigated to determine the structure of these glasses, which should be amenable to chemical strengthening. The ratio of BO4 units to BO3 units approached unity as the R2 O/Al2 O3 ratio for compounds having fixed B2 O3 contents approached unity. Nuclear quadrupole coupling constants ( e2 Qq/h =2.73 to 2.93 MHz) were measured for the NMR spectra of 11 B triangles. The line shapes of 27 Al spectra varied with chemical composition, but a few glasses exhibited 27 Al line shapes similar to those of the AlO4 triclusters in SiO2 -Al2 O3 -Na2 O glasses. Compositional trends in the formation of BO4 and AlO4 were deduced from the NMR spectra. 相似文献
18.
E. F. RIEBLING 《Journal of the American Ceramic Society》1973,56(6):303-309
Binary Sb2 O3 -GeO2 glasses containing 45 mol% Sb2 O3 and ternary Sb2 O3 -B2 O3 -GeO2 glasses containing 50 mol% GeO2 were prepared. Their densities (volumes), refractive indices, and infrared spectra were determined, and their colors and high-temperature viscosities were estimated visually. Small amounts of Sb2 O3 (∼10 mol%) appear to perturb neither the Ge-O-Ge network nor those B-O-Ge networks with small B/Ge ratios (∼0.2). The B-O-Ge networks with larger B/Ge ratios (∼1.0) depolymerize in the presence of even less Sb2 O3 . Amounts of Sb2 O3 >10 mol% appear to depolymerize the Ge-O-Ge and Ge-O-B networks progressively, possibly with the formation of chains. A structurally sensitive ir isofrequency contour technique developed for ternary glass systems was applied successfully to these Sb2 O3 -B2 O3 -GeO2 glasses. These contours can thus readily detect significant network depolymerization in the absence of the usual network modifiers. 相似文献
19.
Carlos E. Bamberger Tamara J. Havedock Otto C. Kopp† 《Journal of the American Ceramic Society》1994,77(6):1659-1661
The ternary system SrO-CeO2 -TiO2 was investigated using X-ray diffractometry. The formation of a new compound, Sr2 Ce2 Ti5 O16 , was established, and its compatibilities with SrO, SrCeO3 , and SrTiO3 were studied. The results revealed the existence of a series of compounds Sr6–12x Ce6x Ti5 O16 and solid solutions Sr2+n Ce2 Ti5+n O16+3n ( n ≤ 6). 相似文献
20.
Jae Ryong Kim Do-Hyeong Kim Chong Hee Kim 《Journal of the American Ceramic Society》1990,73(8):2567-2569
The effects of ZrO2 and Y2 O3 on the densification of hotpressed Si3 N4 -Zr(Y)O2 composites have been studied. High density could not be obtained by the addition of pure or 3-mol%-Y2 O3 -doped ZrO2 in this composite; however, nearly full density (>97%) could be obtained in Si3 N4 using 6- and 8-mol%-Y2 O3 -doped ZrO2 . It is concluded that Y2 O3 diffusing out from the added Zr(Y)O2 promoted the densification and that ZrO2 also had some role in the formation of an oxynitride glass. 相似文献