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1.
The (YBa2 Cu3 )1−x Nax O7–δ system in the range of x = 0–0.8 was investigated. Experimental data suggest that the sodium doping with x 0.26 does not affect the critical transition temperature Tc , and the crystal structure maintains the orthorhombic lattice with a slightly smaller unit cell. However, sodium doping increases the sintering and grain growth kinetics, resulting in a higher superconducting phase volume and an enhanced Meissner effect. It also lowers the processing temperaturel. The experimental data also suggest that the sodium atoms diffuse into the superconducting YBa2 Cu3 O7−δ crystallites, which stabilizes the orthorhombic phase. The transition temperature (ortho-rhombic to tetragonal) in sodium-doped materials increases with the increasing concentration of sodium. 相似文献
2.
An X-ray and dielectric study of three series of PbNb2 O6 -type solid solutions was carried out. The PbNbZOs-type phase was present up to the following limits: (1) (Pb1−x Bi4 /3x )(Tix Nb2 -x .)O6 , ×= 0.2; (2) (Pbl -x Bi4 3x )(Ti2 Nbl —2)2 06 , ×= 0.2; and (3) (Pb1−x Bi2 /3x )Nb2 O6 ×= 0.3. Orthorhombic distortion b/a and Curie temperature decreased with increasing x. Bi4/3 -Ti2 06 was most effective in this respect and Bi2 , 3 -Nb2 O6 had the least influence. The important role played by ions of different valency located on crystallographically equivalent sites is pointed out. 相似文献
3.
Makoto Takahashi Yuuko Tomioka Toshiyuki Miyauchi Shoji Sato Asami Murai Toshiyuki Ido Koichi Wakita Hiroshi Terada Sadao Ohkido Masanori Matsubara 《Journal of the American Ceramic Society》2007,90(7):2032-2037
A slurry containing YBa2 Cu3 O7− x particles and a fine YBa2 Cu3 (OH) x colloid solution was prepared, and a large-scale bulk YBa2 Cu3 O7− x superconductor (about 50 mm × 35 mm × 2 mm) was produced by plastic forming without high-pressure molding. The samples molded from the slurry were dried and then fired at 1223 K in air. X-ray diffraction data indicated that the samples had the characteristic orthorhombic YBa2 Cu3 O7− x structure. Measurements of electrical resistance were carried out between 300 and 50 K by the standard four-probe DC electrical measurement. The samples began superconducting at an onset temperature around 92 K, and the full-transition temperature (critical temperature) ( T c ) was 88.7±1.4 K. The critical current density ( J c ) measured at 77 K was about 440 A/cm2 , the value of J c was improved by the heat treatment under an oxygen atmosphere, and J c =1.6 × 103 A/cm2 was observed. Under the magnetic field (B=1 T), the sample held its superconductivity, and demonstrated that this method can be used to produce the magnetic shielding used in magnetic resonance imaging diagnosis. 相似文献
4.
Novel Solution-Soaking Method for Adding Dopants to YBa2 Cu3 O7−x to Achieve Higher Sintered Densities
Pottail Umadevi K. Ravindran Nair Alathur D. Damodaran 《Journal of the American Ceramic Society》1989,72(12):2386-2387
YBa2 Cu3 O7−x was doped with various metal ions by a new technique in which a pellet (after binder burnout) was soaked in a solution containing the appropriate ions and then dried. The sintered density of the treated pellets depended on the dopant in the solution, and in many cases it was much higher than that obtained for pure YBa2 Cu3 O7−x (93% to 96% as compared with 85% to 90%). A study of the microstructure revealed that, in those cases where higher sintered densities were obtained, the grain size was much smaller. The grain morphology, however, did not change. It is likely that the high concentration of dopant adsorbed on the grain surface during solution soaking enhanced the rate of sintering. 相似文献
5.
Lead-free (K0.44 Na0.52 Li0.04 ) (Nb0.96−x Tax Sb0.04 )O3 piezoelectric ceramics were prepared by the conventional solid-state sintering method. The grain growth of the ceramics was inhibited and the relative density was improved with Ta substituting for Nb. Increasing x led to different variations of dielectric properties before and after poling, and prevented the occurrence of orthorhombic–tetragonal phase transition (at T o − t ). All the ceramics show an intermediate relaxor-like behavior between normal and ideal relaxor ferroelectrics. Significantly enhanced dielectric and piezoelectric properties were obtained in the ceramics with x =0.20. The ceramics are very promising lead-free materials for electromechanical device applications. 相似文献
6.
Hiroaki Takeda Masataka Ohgaki Takashi Kizuki Kazuaki Hashimoto Yoshitomo Toda Shigekazu Udagawa Kimihiro Yamashita 《Journal of the American Ceramic Society》2000,83(11):2884-2886
The formation process of Ba2 La8 (SiO4 )6 O2 was clarified using thermogravimetry–differential thermal analysis (TG-DTA) and a high-temperature powder X-ray diffraction (HT-XRD) method. Phase changes identified from the HT-XRD data surprisingly corresponded to the weight loss and/or endothermic peaks observed in the TG-DTA curves. Raw material with the composition Ba2 La8 (SiO4 )6 O2 was completely reacted at 1400°C and produced only an apatite-type compound without a secondary phase. Moreover, the synthesis of Ba2+ x La8− x (SiO4 )6 O2−δ crystals with x = 0–2 was attempted using a solid-state reaction. 相似文献
7.
Xiuying Guo Ning Zhu Mi Xiao Xiawan Wu 《Journal of the American Ceramic Society》2007,90(8):2467-2471
Sb2 O5 were selected to substitute (Nb0.8 Ta0.2 )2 O5 and the effects of Sb substitution on the dielectric properties of Ag(Nb0.8 Ta0.2 )O3 ceramics were studied. The perovskite Ag(Nb0.8 Ta0.2 )1− x Sb x O3 ceramics showed no obvious change with x value being no more than 0.08, and the pseudoperovskite unit cell parameters a = c , b and monoclinic angle β decrease with Sb concentration increasing. The dielectric properties of Ag(Nb0.8 Ta0.2 )1− x Sb x O3 ceramics were found to be affected greatly by the substitution of Sb for Nb/Ta. The ɛ value of Ag(Nb0.8 Ta0.2 )1− x Sb x O3 ceramics sintered at their densified temperature increased from 480 to 825 with x from 0 to 0.08, the tan δ value decreased sharply from 0.0065 to 0.0023 (at 1 MHz) with x increasing from 0 to 0.04, and then kept a stable lower tan δ value ∼0.0024 with x to 0.08. The temperature coefficient of capacitance values continuously decreased from a positive value of 1450 ppm/°C for x =0 to a negative value of −38.52 ppm/°C for x =0.08. 相似文献
8.
The thermodynamic data for the Y2 O3 –BaO–Cu2 O–CuO quaternary system were optimized from measured thermodynamic data. A two-sublattice model for ionic solution was used to express the Gibbs free energy of the liquid phase, and a two-sublattice regular solution model was used for the nonstoichiometric YBa2 Cu3 O6+δ superconducting compound. The optimized thermodynamic data were used to calculate the phase diagrams of the Cu2 O–CuO binary system and the CuO x –Y2 Cu2 O5 and CuO x –BaCuO2 quasi-binary systems. The results were in good agreement with reported measured data. The liquidus projection and isothermal and vertical sections of the Y2 O3 –BaO-CuO x quasi-ternary system were calculated. The effect of oxygen pressure on some reaction temperatures was predicted by calculating them at various oxygen pressures, and the oxygen contents (6 +δ) in YBa2 Cu3 O6+δ were calculated at various temperatures and oxygen pressures. The results were compared with experimental data. 相似文献
9.
Lijie Zhang Jie Chen Helen M. Chan Martin P. Harmer 《Journal of the American Ceramic Society》1989,72(10):1997-2000
In situ annealing studies of YBa2 Cu3 O6+x performed in an optical hot stage revealed that, at temperatures ∧450°, localized melting occurred. On subsequent cooling, a discrete second phase was observed at the YBa2 Cu3 O6+x grain boundaries. Quantitative chemical analysis using X-ray wavelength dispersive spectroscopy indicated that the second phase was composed of a barium oxycarbonate. The source of the carbon in the second phase was identified to be CO2 in the atmosphere. 相似文献
10.
Effects of La on Dielectric and Piezoelectric Properties of Pb1−x La2x/3 (Nb0.95 Ti0.0625 )2 O6 Ceramics
Gao-li Men Peng Liu Ruo-xi Zhang Hong Chen Bo Wang Jian-ping Zhou Gang-qiang Zhu 《Journal of the American Ceramic Society》2009,92(8):1753-1757
Ceramics with the chemical compositions of Pb1− x La2 x /3 (Nb0.95 Ti0.0625 )2 O6 (0≤ x ≤0.060) (PLTN) were prepared by the conventional solid-state reaction method. X-ray diffraction analysis indicated that Ti and La doping not only decreased the rhombohedral–tetragonal phase transformation temperature, but also stabilized the orthorhombic phase of PLTN ceramics. All ceramics sintered at 1190°–1250°C had shown the pure orthorhombic ferroelectric phase. La doping suppresses grain growth and inhibits the formation of pores and cracks, resulting in an increase in relative density up to 97%. The amount of La doping to PLTN ceramics obviously affect ceramics' piezoelectric constant ( d 33 ) and dielectric loss (tanδ). The sample with x =0.015 possesses high Curie temperature ( T c =560°C), low dielectric loss (tanδ=0.0054), and excellent piezoelectric constant ( d 33 =92 pC/N), presenting a high potential to be used in high-temperature applications as piezoelectric transducers. 相似文献
11.
Mari Lou Balmer Fred F. Lange Vikram Jayaram Carlos G. Levi 《Journal of the American Ceramic Society》1995,78(6):1489-1494
Aqueous mixtures of zirconium acetate and aluminum nitrate were pyrolyzed and crystallized to form a metastable solid solution, Zr1- x Al x O2− x /2 ( x < 0.57). The initial, metastable phase partitions at higher temperatures to form two metastable phases, viz., t −ZrO2 +γ-Al2 O3 with a nano-scale microstructure. The microstructural observations associated with the γ- →α-Al2 O3 phase transformation in the t -ZrO2 matrix are reported for compositions containing 10, 20, and 40 mol% A12 O3 . During this phase transformation, the α-Al2 O3 grains take the form of a colony of irregular, platelike grains, all with a common crystallographic orientation. The plates contain ZrO2 inclusions and are separated by ZrO2 grains. The volume fraction of A12 O3 and the heat treatment conditions influence the final microstructure. At lower volume fractions of A12 O3 , the colonies coarsen to single, irregular plates, surrounded by polycrystalline ZrO2 . Interpenetrating microstructures produced at high volume fractions of A12 O3 exhibit very little grain growth for periods up to 24 h at 1400°C. 相似文献
12.
Solid-state sintering was used to make YBa2 Cu3 O7−δ superconducting bulk materials. Corrosion of the YBa2 Cu3 O7−δ superconductor material was investigated in a humid environment. The superconducting materials exhibited significant corrosion after 4 h at 80° and 100% relative humidity. A grain-boundary phase was formed, and the percent superconducting phase in the material decreased by approximately 60%. The transition temperature (Tc ) decreased with corrosion time. After 2 h of corrosion, Tc decreased from 87 to 81 K. 相似文献
13.
John Niska Bengt Loberg Kenneth Easterling 《Journal of the American Ceramic Society》1989,72(8):1508-1510
Hot isostatic pressing of the high-Tc superconductor YBa2 Cu3 O7−δ can lead to loss of oxygen and transformation of the material from the high-Tc orthorhombic phase to the nonsuperconducting tetragonal phase. It is shown that glass encapsulation helps retain the orthorhombic structure, whereas steel encapsulation resulted in formation of the tetragonal phase. Reasons for this phenomenon are discussed. The equilibrium oxygen gas pressure for the oxygen decomposition reaction in YBa2 Cu3 O7 , however, prevents full densification of this material in glass when employing hot isostatic pressing conditions of 200 MPa and 845°C. 相似文献
14.
Ji-Ping Zhou Charles C. Sorrell Shi-Xue Dou Miles H. Apperley 《Journal of the American Ceramic Society》1991,74(7):1541-1546
The present work describes a new technique to synthesize aligned YBa2 Cu3 O7- x and Ag─YBa2 Cu3 O7- x superconducting composites from Ba- and Cu-deficient compositions (relative to YBa2 Cu3 O7- x ) plus BaCuO2 . For YBa2 Cu3 O7- x , high transition temperature midpoint Tc (91 K), temperature of zero resistivity T 0 (90 K), and critical current density Jc (>3000 A°Cm−2 at 77 K) were achieved by using this technique. This procedure provides the potential for using a reliable and reproducible densification and alignment technique alternative to partial or full melting. The composite is highly aligned, with an average grain size of ∼1 to 2 mm and domains of width greater than 5 mm. The initial phase assemblage consists of YBa2 Cu3 O7- x (123) as the major phase plus YBa2 CuO5 (211) CuO as minor phases. The BaCuO2 is added to the Ba- and Cu-deficient starting composition in order to assist in the formation of a CuO-rich liquid as well as to compensate for the Ba and Cu deficiences in 123. Since the liquid forms at ∼900°C and is compatible with 123, it can be used to facilitate alignment of 123 at ∼930°C. The addition of Ag to the system results in eutectic formation with the (solidified) liquid, substantial filling of the pores during sintering, and improved alignment. 相似文献
15.
Zhong Zhuang Xian Ping Wang Dan Li Tao Zhang Qian Feng Fang 《Journal of the American Ceramic Society》2009,92(4):839-844
Dense, crack-free, and uniform La2 Mo2− x W x O9 ( x =0, 0.1, and 0.2) nanocrystalline films were successfully synthesized on poly-alumina substrates via a modified sol–gel method, with inorganic salt of La(NO3 )3 ·6H2 O, (NH4 )6 Mo7 O24 ·4H2 O, and (NH4 )6 H2 W12 O24 as precursors. Pure La2 Mo2 O9 phase was confirmed by X-ray diffractometer when the annealing temperature was >500°C. The average grain size of the La2 Mo2− x W x O9 films is in the range of 90–400 nm, depending upon the conditions of thermal treatment, and the thickness of films can reach 1 μm by repetitive spin-coating. The electrical conductivity increases with decreasing grain size and reaches 0.074 S/cm at 600°C in the film with a grain size of 90 nm, which is one order of magnitude higher than that in the corresponding bulk materials. W-doping can suppress the phase transition that occurs at 580°C in pure La2 Mo2 O9 and enhance the low-temperature ionic conductivity. Furthermore, the activation energy of conductivity in the nanocrystalline La2 Mo2 O9 films decreases to about 0.6 eV in comparison with 1.0 eV in the bulk ones, which implies that the grain resistance prevails in the total resistance, when grain size reduces to nanometer domain. 相似文献
16.
Roger C. Baetzold 《Journal of the American Ceramic Society》1990,73(11):3185-3188
Simulation techniques are applied to the orthorhombic YBa2 Cu3 O7 crystal in order to describe possible polaron and bipolaron species in the crystal. Perfect crystal properties are fitted well with a two- and three-body potential model. The O− polaron state is significantly stabilized by the presence of holes in the CuO plane. A bipolaron O2− 2 is slightly stable on the O4 and O2 or O3 lattice ion sites of oxygen. The oxidation reaction leading to O− and involving Cu+ and oxygen vacancies is exothermic. 相似文献
17.
Hyun-Cheol Song Kyung-Hoon Cho Hwi-Yeol Park Cheol-Woo Ahn Sahn Nahm Kenji Uchino Seung-Ho Park Hyeung-Gyu Lee 《Journal of the American Ceramic Society》2007,90(6):1812-1816
(1− x )(Na0.5 K0.5 )NbO3 – x LiNbO3 [(1− x )NKN– x LN] ceramics were produced by the conventional solid-state sintering method, and their microstructure and piezoelectric properties were investigated. The formation of the liquid phase and K6 Li4 Nb10 O30 second phase that were observed in the (1− x )NKN– x LN ceramics was explained by the evaporation of Na2 O during the sintering. A morphotropic phase boundary (MPB) was observed in the specimens with 0.05< x <0.08. Promising piezoelectric properties were obtained for the specimens with x =0.07. Therefore, the piezoelectric properties of this 0.93NKN–0.07LN ceramic were further investigated and were found to be influenced by their relative density and grain size. In particular, grain size considerably affected the d 33 value. Two-step sintering was conducted at different temperatures to increase the grain size. Piezoelectric properties of d 33 =240 (pC/N) and k p =0.35 were obtained for the 0.93NKN–0.07LN ceramics sintered at 1030°C and subsequently annealed at 1050°C. 相似文献
18.
A narrow region of Zn-vacancy-containing cubic perovskites was formed in the (1− x )Ba3 (ZnNb2 )O9 −( x )Ba3 W2 O9 system up to 2 mol% substitution ( x =0.02). The introduction of cation vacancies enhanced the stability of the 1:2 B-site ordered form of the structure, Ba(Zn1− x □ x )1/3 (Nb1− x W x )2/3 O3 , which underwent an order–disorder transition at 1410°C, ∼35° higher than pure Ba(Zn1/3 Nb2/3 )O3 . The Zn vacancies also accelerated the kinetics of the ordering reaction, and samples with x =0.006 comprised large ordered domains with a high lattice distortion ( c/a =1.226) after a 12 h anneal at 1300°C. The tungstate-containing solid solutions can be sintered to a high density at 1390°C, and the resultant ordered ceramics exhibit some of the highest microwave dielectric Q factors ( Q × f =1 18 000 at 8 GHz) reported for a niobate-based perovskite. 相似文献
19.
E. C. SUBBARAO 《Journal of the American Ceramic Society》1960,43(9):439-442
The phase transitions in PbNb2 O6 and in compositions of the type Pb1+x (Bx Nb1-x )O6 , where B = Ti4+ , Zr4+ , or Sn4+ , have been investigated between 25° and 650°C. using X-ray and dilatometric techniques. The modified PbNb2 o6 compositions possess orthorhombic PbNb2 O6 -type structure, with the additional Pb2+ ions occupying vacant lattice sites. The lattice parameters a and c expand and b contracts during heating until, at the ferroelectric Curie temperature, a and b suddenly coincide and c expands slightly. Besides this phase change at the Curie temperature, the nonstoichiometric compounds show an additional phase transition in the range 450° to 300°C. depending on composition. The intermediate phase of Pbl+x (Ti2 Nb1-z )2 O6 appears to possess orthorhombic symmetry. 相似文献
20.
Two cubic pyrochlore phases exist in the system ZnO–Bi2 O3 –Sb2 O5 . Neither has the supposed "ideal" stoichiometry, Zn2 Bi3 Sb3 O14 . One, P 1 , is a solid solution phase, Zn2+ x Bi2.96−( x − y ) Sb3.04− y O14.04+δ where 0< x <0.13(1), 0< y <0.017(2) and a =10.4285(9)−10.451(1) Å. The other, P 2 , is a line phase, Zn2 Bi3.08 Sb2.92 O13.92 with a =10.462(2) Å. Subsolidus phase relations at 950°C involving phases P 1 and P 2 in the ZnO–Bi2 O3 –Sb2 O5 phase diagram have been determined. 相似文献