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1.
The cation solubility limits of the n = 2 and n = 3 superconducting phases in the Bi2 (Sr x Ca1 − x ) n +1 Cu n O y system were established along tie lines with compatible phases via electron probe microanalysis on bi- (or poly-) phasic samples prepared at 860°C. Pb additions (15 mol% of the Bi content) were used to facilitate formation of the n = 3 phase. In each case football-shaped volumes in composition space were established as the solubility limits which bordered on the nominal compositions 2212 or 2223 (Bi:Sr:Ca:Cu) with the long axis parallel to the Sr-Ca side of the quaternary (i.e., Sr-to-Ca intersolubility) but also extending toward Bi and Cu. This means that, for the most part, the superconducting phases are alkaline-earth deficient relative to the ideal 2212 and 2223 compositions. The Pb content in the 2223 phase is typically 10% of the Bi content. T c variations could be correlated with variations in Sr or (Sr + Bi) content and the length of the c -axis parameter. 相似文献
2.
Pure and 5 wt% of Ag-doped (La1− x Y x )2 Ba2 CaCu5 Oz superconducting compounds for x =0–0.5 have been prepared. Analysis of X-ray diffraction patterns shows that the samples are essentially in the single-phase form and they could be refined using the P 4 /mmm space group in a tetragonal cell. The typical lattice parameters are found to be a = b =3.879 Å, c =11.646 Å for x =0 and a = b =3.856 Å, c =11.576 Å for x =0.5 samples. The detailed crystal structure parameters are presented. The average grain size values from scanning electron microscope images are found to be in the order of 1–3 μm. Temperature variations of ac susceptibility and electrical resistivity have been measured. Superconducting transitions with diamagnetic T c ranging from 60 to 75 K have been observed, with the maximum T c for the x =0.25 sample. Ag-doped samples exhibit improved inter-granular coupling and homogeneous oxygenation. 相似文献
3.
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
4.
Senlin Leng Guorong Li Liaoying Zheng Tianbao Wang Qingrui Yin 《Journal of the American Ceramic Society》2009,92(11):2772-2775
As a lead-free positive temperature coefficient of resistivity (PTCR) material, (1– x mol%) BaTiO3 – x mol% (Bi1/2 K1/2 ) TiO3 – y mol% Y2 O3 –0.5 mol% TiO2 (BT– x BKT–2 y Y–0.5TiO2 ) systems were prepared by the conventional solid-state reaction method. All samples containing <2 mol% BKT sintered in air possessed relatively low room-temperature resistivity (ρ25 ) and high positive temperature coefficient (PTC) effect. However, when the BKT content exceeded 2 mol%, the sample was not semiconductive after sintering in air. The effects of sintering schedule on the properties of PTCR ceramics were discussed. The results showed that the optimum composition of BT–1BKT–0.2Y–0.5TiO2 , sintered at 1330°C for not-soaking and then fast quenched in air, achieved rather low ρ25 of 28 Ω·cm and a high jump of resistivity (maximum resistivity [ρmax ]/minimum resistivity [ρmin ]) of 4.0 orders of magnitude with T c about 155°C. The ρ25 of the as-sintered sample could be further reduced to about 10 Ω·cm by annealing in N2 at 450°C for 30 min, accompanied decrease on the PTC effect. 相似文献
5.
Jiagang Wu Ting Peng Yuanyu Wang Dingquan Xiao Jumu Zhu Yong Jin Jianguo Zhu Ping Yu Lang Wu Yihang Jiang 《Journal of the American Ceramic Society》2008,91(1):319-321
(1− x )(K0.48 Na0.52 )(Nb0.95 Ta0.05 )O3 – x LiSbO3 [(1− x )KNNT− x LS] lead-free piezoelectric ceramics were prepared by the conventional solid-state sintering method. A morphotropic phase boundary (MPB) between orthorhombic and tetragonal phases was identified in the composition range of 0.03< x <0.05. The ceramics near the MPB exhibit a strong compositional dependence and enhanced electrical properties. The (1− x )KNNT– x LS ( x =0.04) ceramics exhibit good electrical properties ( d 33 =250 pC/N, k p =45.1%, k t =46.3%, T c =348°C, T o − t =74°C, P r =25.9 μC/cm2 , E c =10.7 kV/cm, ɛr ∼1352, tan δ∼3%). These results show that (1− x )KNNT– x LS ceramic is a promising lead-free piezoelectric material. 相似文献
6.
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
7.
Jiagang Wu Dingquan Xiao Yuanyu Wang Lang Wu Yihang Jiang Jianguo Zhu 《Journal of the American Ceramic Society》2008,91(7):2385-2387
[(K x Na1 − x )0.95 Li0.05 ](Nb0.95 Ta0.05 )O3 (K x NLNT) ( x= 0.40–0.60) lead-free piezoelectric ceramics were prepared by conventional solid-state sintering. The effects of K/Na ratio on the dielectric, piezoelectric, and ferroelectric properties of the K x NLNT ceramics were studied. The experimental results show that the electrical properties strongly depend on the K/Na ratio in the K x NLNT ceramics. The K x NLNT ( x =0.42) ceramics exhibit enhanced properties ( d 33 ∼242 pC/N, k p ∼45.7%, k t ∼47%, T c ∼432°C, T o−t =48°C, ɛr ∼1040, tanδ∼2.0%, P r ∼26.4 μC/cm2 , E c ∼10.3 kV/cm). Enhanced electrical properties of the K x NLNT ( x =0.42) ceramics could be attributed to the polymorphic phase transition near room temperature. These results show that the K x NLNT ( x =0.42) ceramic is a promising lead-free piezoelectric material. 相似文献
8.
Teen-Hang Meen Ying-Chung Chen Ken-Whie Liaw Hung-Duen Yang 《Journal of the American Ceramic Society》1993,76(8):1948-1952
X-ray diffraction patterns show that most samples of Y1-x Prx Ba2 Cu4 O8 examined in the present study contained a single YBa2 Cu4 O8 (1-2-4) superconductive phase for x<0.7.Lattice parameters a and b increased with Pr concentration, suggesting that most of the Pr is trivalent in Y1-x Prx- Ba2 Cu4 O8 . The zero-resistance temperature, T co , decreases monotonically from 80 K at x=0 to 12 K at x=0.65, and superconducting transition widths tend to broaden for x>0. The room-temperature resistivity changes linearly until x=0.7 and increases abruptly at x=-0.75. The critical concentration, xcr , thus was estimated to be 0.7. The effective magnetic moments of Pr in Y 1-x Prx Ba2 Cu4 O8 were 3.63., 3.35, and 3.23, μB for x=0.2, 0.4 and 0.6, respectively. In the R0.8 Pr0.2 Ba2 Cu4 O8 system, the depression of Tc weakly depends on the ionic radius of rare-earth elements. Similarities and differences between Y 1-x Prx Ba2 Cu4 O8 and Y1-x Prx- Ba2 Cu3 O7-y also were noted and are discussed in this paper. 相似文献
9.
Sintering YBa2 Cu3 O7- x bulk forms at 1050°C followed by annealing at 980°C causes the development of a thick oriented surface layer (Lotgering factor = 0.7). The thickness of the layer depends on the thermal treatment, which is a two-step sintering process. Firing at 1050°C for 2.5 h followed by 30 h at 980°C leads to the development of a 0.1-mm-thick surface layer, with clear indication that longer annealing would result in a thicker film. Some orientation develops during un-axial compaction of the powders. Lotgering orientation factor calculation from X-ray diffraction analysis. SEM, and TEM were used to characterize the microstructure of these samples. T c was similar to that of conventionally processed high-density samples, between 83 and 87 K. Some thermal treatments resulted in samples that displayed high resistivity above T c , possibly caused by segregation of Cu to the grain boundaries. 相似文献
10.
Sandeep Butee Ajit Kulkarni Om Prakash Ramnath P.R.C. Aiyar Sumesh George Mailadi Sebastian 《Journal of the American Ceramic Society》2009,92(5):1047-1053
(Ni1− x Zn x )Nb2 O6 , 0≤ x ≤1.0, ceramics with >97% density were prepared by a conventional solid-state reaction, followed by sintering at 1200°–1300°C (depending on the value of x ). The XRD patterns of the sintered samples (0≤ x ≤1.0) revealed single-phase formation with a columbite ( Pbcn ) structure. The unit cell volume slightly increased with increasing Zn content ( x ). All the compositions showed high electrical resistivity (ρdc =1.6±0.3 × 1011 Ω·cm). The microwave (4–5 GHz) dielectric properties of (Ni1− x Zn x )Nb2 O6 ceramics exhibited a significant dependence on the Zn content and to some extent on the morphology of the grains. As x was increased from 0 to 1, the average grain size monotonically increased from 7.6 to 21.2 μm and the microwave dielectric constant (ɛ'r ) increased from 23.6 to 26.1, while the quality factors ( Q u × f ) increased from 18 900 to 103 730 GHz and the temperature coefficient of resonant frequency (τf ) increased from −62 to −73 ppm/°C. In the present work, we report the highest observed values of Q u × f =103 730 GHz, and ɛ'r =26.1 for the ZnNb2 O6 -sintered ceramics. 相似文献
11.
Peter J. Majewski Stefanie Kaesche Fritz Aldinger 《Journal of the American Ceramic Society》1997,80(5):1174-1180
Phase equilibria of the quasi-quinary system Bi3 O3 -PbO-SrO-CaO-CuO were studied between 650° and 900°C in air with emphasis on the high-temperature superconducting phase (Bi,Pb)2+ x Sr2 Ca2 Cu3 O10+ d (2223). The 2223 phase lies in equilibrium with a number of nonsuperconducting phases and also with the superconducting phase (Bi,Pb)2 Sr2 CaCu2 O8+ d (2212). The single-phase region was found to be very limited. The Pb solubility of the 2223 phase is strongly temperature dependent. The phase relations are very sensitive to variations of the cation concentration and temperature. This effect significantly influences the preparation of 2223 ceramics. 相似文献
12.
Makoto Takahashi Toshiyuki Miyauchi Kengo Sawada Hiroyuki Ishikawa Shoji Sato Masahiro Tahashi Koichi Wakita Sadao Ohkido Motohisa Honda Asami Murai Masato Kamiya Masanori Matubara 《Journal of the American Ceramic Society》2009,92(3):578-584
The preparation of large-scale YBa2 Cu3 O7− x superconductor samples was investigated. This method is based on plastic forming using a slurry consisting of YBa2 Cu3 O7− x particles and a sol solution made up of multimetallic hydroxide particles (YBa2 Cu3 (OH) x colloidal particles) and poly(vinyl) alcohol (PVA). The effects of adding PVA on the product, the crystallinity, and the superconducting properties of the sample were investigated. It was found that PVA acted as a protective colloid in the sol solution and stabilized YBa2 Cu3 (OH) x colloidal particles, and that the role of PVA changed from a thickener to a flocculant during drying so that the formability/workability of the green sheet sample was improved and large samples (about 80 mm × 80 mm × 3 mm) without large cracks were obtained after firing. The samples became superconducting at 91.5±0.5 K ( T con ) and the full transition temperature ( T coff ) was 88.5±1.5 K. The critical current density ( J c ) of the sample prepared from the slurry containing 1 wt% PVA was 713±150 A/cm2 at 77 K. This J c value was improved to 2300 A/cm2 by heat treatment at 773 K under an oxygen atmosphere. 相似文献
13.
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
14.
Porous glass-ceramics with a skeleton of the fast-lithium-conducting crystal Li1+ x Ti2− x Al x (PO4 )3 (where x = 0.3–0.5) were prepared by crystallization of glasses in the Li2 O─CaO─TiO2 ─Al2 O3 –P2 O5 system and subsequent acid leaching of the resulting dense glass-ceramics composed of the interlocking of Li1+ x Ti2− x Al x (PO4 )3 and β-Ca3 (PO4 )2 phases. The median pore diameter and surface area of the resulting porous Li1+ x Ti2− x Al x (PO4 )3 glass-ceramics were approximately 0.2 μm and 50 m2 /g, respectively. The electrical conductivity of the porous glass-ceramics after heating in LiNO3 aqueous solution was 8 × 10−5 S/cm at 300 K or 2 × 10−2 S/cm at 600 K. 相似文献
15.
Yuan Chang Guo Hua Kun Liu Shi Xue Dou 《Journal of the American Ceramic Society》2000,83(7):1675-1680
(Bi,Pb)2 Sr2 Ca2 Cu3 O10 (Bi2223) precursor powders with large and small amounts of Ca2 PbO4 phase were prepared and used to make superconductor/silver composite tapes. The melting behavior of the powders and tapes was examined by differential thermal analysis (DTA). The influence of Ca2 PbO4 on the formation and microstructure of Bi2223, and electrical properties of the tapes, was investigated by X-ray diffraction (XRD), scanning electron microscopy (SEM), and critical current measurements. It was found that the melting onset temperature ( T m,onset ) of precursor powders and composite tapes was strongly dependent on the amount of Ca2 PbO4 . Tapes with a small amount of Ca2 PbO4 had a higher T m,onset and a higher optimum sintering temperature compared with tapes with a large amount of Ca2 PbO4 . Also because of the higher sintering temperature, the total sintering time required for the former tapes was drastically shortened compared with the latter ones (250 vs 110 h). Furthermore, the microstructure and the current-carrying capacity of the tapes were significantly improved by reducing the Ca2 PbO4 content of the precursor powders. These results are of practical significance for the commercialization of Bi-based high-temperature superconductors. 相似文献
16.
Takayuki Komatsu Michiko Ueta Tomohiro Ohki Ryuji Sato Kazumasa Matusita 《Journal of the American Ceramic Society》1992,75(7):1864-1869
The Ba-doped superconducting (Bi,Pb)2 Sr2- x Ba x Ca2 Cu3 O y and (Bi,Pb)2 Sr2 Ca2- x Ba x Cu3 O y (0 ≦ x ≦ 1.0) were prepared by using a melt-quenching method, and the effect of Ba additions on the glass-forming ability and the crystalline phase was examined. The glass-forming ability was not improved by substitution of Ba for Sr or Ca, and particularly BaPbO3 as well as CaO was observed in the melt-quenched sample of (Bi,Pb)2 SrBaCa2 Cu3 O y . BaPbO3 crystals were precipitated in all glass-ceramics with Ba substituted for Sr or Ca. The partial substitution of Ba substituted for Sr was effective for the formation of the high- T c phase, and (Bi,Pb)2 Sr1.4 Ba0.6 Ca2 Cu3 O y glass-ceramics obtained by annealing at 830°C for 100 h exhibited superconductivity with a T c of 103 K, although BaPbO3 and the low- T c phase were still largely present. 相似文献
17.
A. D. McLEOD J. S. HAGGERTY D. R. SADOWAY 《Journal of the American Ceramic Society》1984,67(11):705-708
The electrical resistivity of monocrystalline and polycrystalline TiB2 , was measured under an inert atmosphere by a four-point ac impedance technique over the range 298 to 1373 K. The results are expressed in the form ρ-ρ298 = m(T -298). The following values of ρ298 (μω.cm) and m (nω.cm-K-1 ) were determined: for polycrystalline TiB2 (69% dense) 18.2 and 95; for polycrystalline TiB2 (99% dense) 7.4 and 42; and for monocrystalline TiB2 , 6.6 and 34.9. 相似文献
18.
Equilibrium partial pressures of SiF4 were measured for the reactions 2SiO2 ( c )+2BeF2 ( d )⇋SiF4 ( g )+Be2 SiO4 ( c ) (log P siF4 (mm) = [8.790 - 7620/ T ] ±0.06(500°–640°C)) and Be2 SiO4 ( c ) +2BeF2 ( d )⇋SiF4 ( g ) +4BeO( c )(log P siF4 (mm) = [9.530–9400/T] ±0.04 (700°–780°C)), wherein BeF2 was present in solution with LiF as molten Li2 BeF4 . The solubility of SiF4 was low (∼0.04 mol kg-1 atm-1 ) in the melt. The results for the first equilibrium were combined with available thermochemical data to calculate improved Δ Hf and Δ Gf values for phenacite (–497.57 ±2.2 and –470.22±2.2 kcal, respectively, at 298°K). The few measurements above 700°C for the second equilibrium are consistent with the temperature of the subsolidus decomposition of phenacite to BeO and SiO2 and with the heat of this decomposition as determined by Holm and Kleppa. Below 700°C, the pressures of SiF4 generated showed an increasing positive deviation from the expression given for the equilibrium involving Be2 SiO4 and BeO. This deviation might have been caused by the formation of an unidentified phase below 700°C which replaced the BeO; it more likely resulted from a metastable equilibrium involving BeO and SiO2 . 相似文献
19.
Xuebin Zhu Shoubao Zhang Hechang Lei Xiangde Zhu Gang Li Bosen Wang Wenhai Song Zhaorong Yang Jianming Dai Yuping Sun Dongqi Shi Shixue Dou 《Journal of the American Ceramic Society》2009,92(4):800-804
Metallic and transparent La0.5 Sr0.5 TiO3+ x /2 films were prepared by the chemical solution deposition (CSD) method using topotactic reduction processing. The use of Si powder as the reducing agent was facile and allowed easy manipulation. It was observed that metallic (resistivity at 300 K ∼2.43 mΩ cm) and transparent (∼80% transmittance at visible light) La0.5 Sr0.5 TiO3+ x /2 films could be obtained with an annealing temperature of 900°C, which was significantly lower than the hydrogen reduction temperature (∼1400°C). The successful preparation of metallic and transparent La0.5 Sr0.5 TiO3+ x /2 films using CSD has provided a feasible route for depositing other perovskite-structured functional layers on La0.5 Sr0.5 TiO3+ x /2 films using this low-cost all CSD method. 相似文献
20.
Pertinent works of previous investigators are reviewed briefly. A superior technique for the preparation of experimental glasses of high purity and chemical homogeneity is presented. Devitrification growth-rate data and traction-viscosity data are reported for high-silica glasses of the system Al2 O3 -SiO2 . Glasses with added Al2 O3 were found to devitrify to cristobalite more rapidly than ultrapure silica glasses at a given temperature, and yet their fluidities (i.e., reciprocal viscosities) were found to be less. The devitrification growth rate, g, was found to be of zero order and to follow the temperature dependence In( g/T ) = -(B/T) + In A over the temperature range 1561°K. T 1730°K. 相似文献