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971.
Piezoelectric properties of (Na0.5K0.5)(Nb1‐xSbx)O3‐SrTiO3 ceramics with tetragonal‐pseudocubic PPB structure
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Dae‐Hyeon Kim Tae‐Gon Lee Sung‐Hoon Cho Ku‐Tak Lee Tae‐Ho Lee Youn‐Woo Hong Chang‐Hyo Hong Jeong‐Seog Kim Sahn Nahm 《Journal of the American Ceramic Society》2018,101(9):3997-4010
CuO‐added 0.96(Na0.5K0.5)(Nb1‐xSbx)O3‐0.04SrTiO3 ceramics sintered at the low temperature of 960°C for 10 hours showed dense microstructures and high relative densities. The specimens with 0.0 ≤ x ≤ 0.04 had orthorhombic‐tetragonal polymorphic phase boundary (PPB) structure. Tetragonal‐pseudocubic PPB structure was observed in specimens with 0.05 ≤ x ≤ 0.07, while the specimen with x = 0.08 has a pseudocubic structure. The structural variation in the specimens is explained by the decreases in the orthorhombic‐tetragonal transition temperature and Curie temperature with the addition of Sb5+ ions. The specimens with 0.05 ≤ x ≤ 0.07, which have tetragonal‐pseudocubic PPB structure, had large electric field‐induced strains of 0.14%‐0.016%. Moreover, these specimens also showed increased d33 values between 280 pC/N and 358 pC/N. In particular, the specimen with x = 0.055 showed particularly enhanced piezoelectric properties: d33 of 358 pC/N, kp of 0.45, and the electric field‐induced strain of 0.16% at 4.5 kV/mm. 相似文献
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基于多层C/S结构的标准网上虚拟学校的研究和设计 总被引:4,自引:2,他引:4
由于开发课件工程的不同,以及网上教学系统实现的差异,所以不同系统之间的课件很难通用。该文结合XML技术和IEEE LTSC(Learning Technolgy Stendards Committee)标准,介绍了能在不同网上教学系统间通用的标准课件的设计,以及基于Web的多层C/S结构的能应用标准课件进行智能教学的CMI系统的研究和设计。并且对于IEEE LTSC中对CMI系统只准对B/S两层结构的设计拓广到C/S多层结构的设计。 相似文献
974.
Biing-Feng Wang Shan-Chyun Ku Keng-Hua Shil 《Parallel and Distributed Systems, IEEE Transactions on》2001,12(9):888-898
An edge is a bisector of a simple path if it contains the middle point of the path. Let T=(V,E) be a tree. Given a source vertex s ∈ V, the single-source tree bisector problem is to find, for every vertex υ ∈ V, a bisector of the simple path from s to υ. The all-pairs tree bisector problem is to find for, every pair of vertices u, υ ∈ V, a bisector of the simple path from u to υ. In this paper, it is first shown that solving the single-source tree bisector problem of a weighted tree has a time lower bound Ω(n log n) in the sequential case. Then, efficient parallel algorithms are proposed on the EREW PRAM for the single-source and all-pairs tree bisector problems. Two O(log n) time single-source algorithms are proposed. One uses O(n) work and is for unweighted trees. The other uses O(n log n) work and is for weighted trees. Previous algorithms for the single-source problem could achieve the same time O(log n) and the same optimal work, O(n) for unweighted trees and O(n log n) for weighted trees, on the CRCW PRAM. The contribution of our single-source algorithms is the improvement from CRCW to EREW. One all-pairs parallel algorithm is proposed. It requires O(log n) time using O(n2) work. All the proposed algorithms are cost-optimal. Efficient tree bisector algorithms have practical applications to several location problems on trees. Using the proposed algorithms, efficient parallel solutions for those problems are also presented 相似文献
975.
T. L. Hung I. A. Chen C. H. Huang C. Y. Lin C. W. Chen Y. B. You S. T. Jian M. C. Yang Y. Y. Hsu J. C. Ho Y. Y. Chen H. C. Ku 《Journal of Low Temperature Physics》2013,171(1-2):148-155
Low-temperature heat capacity C(T) of the weakly electron-correlated SrNi2Ge2 122-layer compound undergoes a superconducting transition with onset at 1.4 K and a bulk T c =0.75 K, where heat-capacity jump ratio ΔC(T c )/γT c =0.88–1.05. A small average superconducting energy gap E g (ave)=2.21 kT c =0.14 meV is derived for this multi-gap superconductor. Similar results for isostructural SrPd2Ge2 include T c (onset)=3.5 K, bulk T c of 2.92 K, ΔC(T c )/γT c =0.70 and E g (ave)=2.54 kT c =0.64 meV. The higher T c onset could be associated with stoichiometric 1:2:2 grains in the polycrystalline samples. In addition, deviations of E g /kT c from the BCS ratio of 3.5 suggest that, just like their iron-based counterpart, these 122-layer germanides may also exhibit an unconventional, fully-opened multi-gap s-wave superconductivity. 相似文献
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