Literatura académica sobre el tema "(x)BiScO3-(1-x)PbTiO3"
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Artículos de revistas sobre el tema "(x)BiScO3-(1-x)PbTiO3"
Wu, Youngsoo, Yeryeong Jin, Bongju Kim, Daeyoung Kwon y Bog G. Kim. "Epitaxial growth and piezoelectric characterization of the (1−x)BiScO3−(x)PbTiO3 ultrathin film". Journal of Applied Physics 109, n.º 6 (15 de marzo de 2011): 064109. http://dx.doi.org/10.1063/1.3567297.
Texto completoChen, Yi, De Jun Lan, Qiang Chen, Ding Quan Xiao, Xi Yue y Jian Guo Zhu. "Stability of the Perovskite Structure in BSPT-Based Ferroelectric Ceramics". Key Engineering Materials 336-338 (abril de 2007): 231–34. http://dx.doi.org/10.4028/www.scientific.net/kem.336-338.231.
Texto completoAlekseev, S. G., I. M. Kotelyanskii, G. D. Mansfel’d, A. G. Segalla y E. N. Khazanov. "Structural analysis of the (BiScO3)1−x -(PbTiO3) x ceramic materials using the resonance and phonon spectroscopy". Journal of Communications Technology and Electronics 57, n.º 8 (agosto de 2012): 842–47. http://dx.doi.org/10.1134/s1064226912080116.
Texto completoSun, Yabin, Hua Wang, Guobao Liu, Hang Xie, Ling Yang, Changrong Zhou, Guohua Chen, Changlai Yuan y Jiwen Xu. "Effects of BiScO3 Doping on the Phase Structure, Ferroelectric, Energy Storage, Strain, and Dielectric Properties of Bi0.5Na0.5TiO3 Ceramics". Journal of Nanoelectronics and Optoelectronics 15, n.º 3 (1 de marzo de 2020): 345–52. http://dx.doi.org/10.1166/jno.2020.2746.
Texto completoKowalski, B., A. Sayir y A. Sehirlioglu. "Aliovalent MnTi and GaTi substitution in high-temperature piezoelectric (x)Bi(Zn0.5Zr0.5)O3—(y)BiScO3—(100 – x − y)PbTiO3". Journal of Materials Science 51, n.º 14 (25 de abril de 2016): 6761–69. http://dx.doi.org/10.1007/s10853-016-9963-y.
Texto completoPorokhonskyy, V., S. Kamba, A. Pashkin, M. Savinov, J. Petzelt, R. E. Eitel y C. A. Randall. "Broadband dielectric spectroscopy of (1−x)BiScO3–xPbTiO3 piezoelectrics". Applied Physics Letters 83, n.º 8 (25 de agosto de 2003): 1605–7. http://dx.doi.org/10.1063/1.1604945.
Texto completoTai, C. W., K. Z. Baba-kishi, H. L. W. Chan, F. G. Shin y C. L. Choy. "Characterization of (1-x)[Bi12In0.5O18.75+γ-Bi2O3]:(x)PbTiO3 ceramics". Materials Science and Engineering: B 99, n.º 1-3 (mayo de 2003): 151–54. http://dx.doi.org/10.1016/s0921-5107(02)00460-9.
Texto completoKowalski, Ben A., Alp Sehirlioglu, Fred W. Dynys y Ali Sayir. "Characterization of the High-Temperature Ferroelectric (100−x −y )BiScO3 -(x )Bi(Zr0.5 Zn0.5 )O3 -(y )PbTiO3 Perovskite Ternary Solid Solution". Journal of the American Ceramic Society 97, n.º 2 (5 de diciembre de 2013): 490–97. http://dx.doi.org/10.1111/jace.12648.
Texto completoYang, F., P. Wu y D. C. Sinclair. "Electrical conductivity and conduction mechanisms in (Na0.5Bi0.5TiO3)1−x(BiScO3)x (0.00 ≤ x ≤ 0.25) solid solutions". Journal of Materials Chemistry C 6, n.º 43 (2018): 11598–607. http://dx.doi.org/10.1039/c8tc04679d.
Texto completoZhao, Wei, Xiaohui Wang, Junjie Hao, Hai Wen y Longtu Li. "Preparation and Characterization of Nanocrystalline (1-x)BiScO3-xPbTiO3 Powder". Journal of the American Ceramic Society 89, n.º 4 (abril de 2006): 1200–1204. http://dx.doi.org/10.1111/j.1551-2916.2005.00860.x.
Texto completoTesis sobre el tema "(x)BiScO3-(1-x)PbTiO3"
Duan, Runrun. "Investigation of xBi(B')O₃-(1 -- x)PbTiO₃ and xBi(B',B")O3-(1 -- x)PbTiO3 perovskite solid solutions with high transition temperatures". Diss., Georgia Institute of Technology, 2007. http://hdl.handle.net/1853/24688.
Texto completoKhatua, Dipak Kumar. "Insights into the Influence of Electric Field on the Structural Evolution and its Correlation with the Properties in the Lead-based BiScO3-PbTiO3 and the Lead-free Na0.5Bi0.5TiO3 based Piezoceramics". Thesis, 2017. http://etd.iisc.ac.in/handle/2005/4121.
Texto completoHung, Li-Wei y 洪立維. "Polarization Rotation through Monoclinic Distortions in Ferroelectric Crystals (PbMg1/3Nb2/3O3)1-x-(PbTiO3)x (PMN-x%PT)". Thesis, 2003. http://ndltd.ncl.edu.tw/handle/70753366116600817424.
Texto completo輔仁大學
物理學系
91
Because of the ultrahigh piezoelectric response in (PbMn1/3Nb2/3O3)1-x(PbTiO3)x crystals, especially near the morphotropic phase boundary. It is important to have a better understanding of these origins. The structure transition can be driven by temperature and electric field. We believe that the path of polarization rotation is associated with high-strain performance in PMN-PT system. For technological applications, it is necessary to select the right PT concentrate, temperature and electric field in order to ensure the best performance. Domain structures and dielectric permittivity have been measured as functions of temperature, frequency and electric field on (001)-cut PMN-37%PT, (001)-cut PMN-24%PT, (102)-cut PMN-31%PT and(211)-cut PMN-33%Ptsingle crystals. By using relations of optical indicatrices and extinction, we found the structure and polarization rotation with temperature and electric field changing. The domain structures show a strong hysteresis behavior during processes of increasing and decreasing electric field.
Huang, Jun-Lin y 黃俊霖. "Hysteresis Loop of Polarization vs. Electric-Field in (PbMg1/3Nb2/3O3)1-x(PbTiO3)x Crystals". Thesis, 2003. http://ndltd.ncl.edu.tw/handle/89225904070886228074.
Texto completo輔仁大學
物理學系
91
The dielectric constant and polarization-electric field ( P-E) hysteresis loops have been measured as a function of temperature in relaxor ferroelectric single crystals (PbMg1/3Nb2/3O3)1-x(PbTiO3)x , PMN-28%PT[001], PMN-26%PT[110], PMN-31%PT[111], PMN-29%PT[102] . We found that the coervive field Ec and polarization of P-E hysteresis loop increases with increasing PT content. A sharp ferroelectric transition with an abrupt strp-like discontinuity in polarization was observed near 403K for PMN-28%PT[001], 384K for PMN-26%PT[110], 416K for PMN-31%PT[111], 410K for PMN-29%PT[102], respectively. Both thermal hysteresis and discontinous behavior of polarization imply a metastable state at the phase transition temperature, which can only exist theoretically for first-order transition but not second-order transition.
Chih-Hung, Chen y 陳志洪. "Phase Transitions and Electric-Field Effects in Relaxor—Based Ferroelectric Single Crystals (PbZn1/3Nb2/3O3)1-x(PbTiO3)x". Thesis, 2002. http://ndltd.ncl.edu.tw/handle/00722933631130246761.
Texto completoTsai, Chih-Long y 蔡志龍. "Electric-Field Effects on Dielectric Permittivity and Domain Structures of Relaxor-Based Ferroelectric Crystals (PbMg1/3Nb2/3O3)1-x(PbTiO3)x". Thesis, 2001. http://ndltd.ncl.edu.tw/handle/94970103790044748444.
Texto completo輔仁大學
物理學系
89
Dielectric Permittivity and domain structures have been measured as a function of temperature in relaxor-based ferroelectric single crystals (PbMg1/3Nb2/3O3)1-x(PbTiO3)x(PMN-x%PT) for x = 0.32 and 0.33 along [001], [110]and[122] orientations, respectively. As temperature increases, PMN-32%PT and PMN-33%PT undergo successive phase transitions: rhombohedral phase ® coexistence of rhombohedral and tetragonal phases ® tetragonal phase ® coexistence of tetragonal and cubic phases ® cubic phase. A relaxation mechanism which is responsible for the so-called diffuse transition, crossovers a wide-temperature region of ~340-400 K, and may result from partial microdomains conversion from rhombohedral to the tetragonal phase. Extra peak dielectric anomalies were observed in each crystal, possibly due to the percolating polar cluster induced by an external electric field. A field-induced tetragonal symmetry was evidenced and coexists with rhombohedral symmetry in the low-temperature region. In addition, field-induce tetragonal phase along the external field was observed.
Hsu, Chi Cheng y 徐嘉誠. "The La2O3 Doping Effects on the Characteristics of (1-x)Pb(Fe2/3W1/3)O3-PbTiO3 Relaxor Ferroelectric Ceramics". Thesis, 2008. http://ndltd.ncl.edu.tw/handle/92793085191523630219.
Texto completo國立成功大學
電機工程學系碩博士班
96
0.7Pb(Fe2/3W1/3)O3(PFW)-0.3PbTiO3(PT) is one of the classic relaxors with little diffuse-phase-transition(DPT) in normal temperature and lots of dielectric loss caused by space charge appearance. In present work, the 0.7PFW-0.3PT relaxor is synthesized with the conventional solid solution. To decrease the dielectric loss and make the dielectric diffusion property increases we doped the dopant La2O3 for the 0.7PFW-0.3PT. Although, the broader peak dielectric constant is obtained as doping La2O3, the curie point moves to lower temperature. According to the experimental results, the very lower dielectric loss is observed as doping 5at% La2O3. The smoothest dielectric constant in the normal temperature range is obtained between x=0.3 to 0.4 in (1-x)PFW-xPT doped the 5at% dopant La2O3. To discuss dielectric loss and DPT in different ratio Pb(0.95)La0.05(Fe2/3W1/3)0.65Ti0.35O3 prepared by ball-milled method in two steps and direct method also in this present work .
Su, Wen-Chang y 蘇文璋. "The MnO doping effects on the Characteristics and Applications of (1-x)Pb(Fe2/3W1/3)O3-PbTiO3 Relaxor Ferroelectric Ceramics". Thesis, 2006. http://ndltd.ncl.edu.tw/handle/34992536242077803760.
Texto completo國立成功大學
電機工程學系碩博士班
94
Pb(Fe2/3W1/3)O3(PFW) is one of the classic relaxors, with the phase transition temperature of -90℃. Since the phase transition temperature of the PbTiO3-PT is 490℃, the phase transition temperature can be adjusted to higher temperature in need by increasing the x ratio for the (1-x)PFW-xPT solid solution. In present work, the (1-x)PFW-xPT relaxor system is synthesized with the conventional solid solution. The dielectric loss decreases and the dielectric diffusion property increases as doping the dopant MnO for the (1-x)PFW-xPT. Although, the broader peak dielectric constant is obtained as doping MnO, the improvement is not sufficient for the application of capacitor. A great improvement on the temperature dependence of the dielectric constant has been done by using the temperature-compensation method, where the two-layer-structure capacitor is stacked with two heterogeneous dielectric materials of 0.8PFW-0.2PT-0.15w%MnO and 0.7PFW-0.3PT-0.15w%MnO ceramics. According to the experimental results, the very lower dielectric loss is observed as doping 0.15w% MnO. The smoothest dielectric constant in the temperature range between -10℃ and 40℃ has been accomplished for the two-layer-structure capacitor with the weight ratio of 2:1 the0.8PFW-0.2PT-0.15w%MnO and the 0.7PFW-0.3PT-0.15w%MnO.
Capítulos de libros sobre el tema "(x)BiScO3-(1-x)PbTiO3"
Lente, M. H., A. L. Zanin, I. A. Santos, D. Garcia y J. A. Eiras. "Composition and Sintering Process Effects on Ferroelectric Fatigue in (1-x)Pb(Mg1/3 Nb2/3 )O3 -x PbTiO3 Ceramics". En Ceramic Transactions Series, 143–50. Hoboken, NJ, USA: John Wiley & Sons, Inc., 2012. http://dx.doi.org/10.1002/9781118380802.ch13.
Texto completoActas de conferencias sobre el tema "(x)BiScO3-(1-x)PbTiO3"
Raengthon, Natthaphon, Jason Nikkel, Troy Ansell y David P. Cann. "Dielectric and Piezoelectric Ceramics for High Temperature Applications". En ASME 2011 International Manufacturing Science and Engineering Conference. ASMEDC, 2011. http://dx.doi.org/10.1115/msec2011-50263.
Texto completoJiang, Yihang, Baoquan Qin, Yi Chen, Wei Huang, Yi Zhao, Zhuo Xu, Dingquan Xiao y Jianguo Zhu. "Preparation and Characterization of yBiGaO3-(1-x-y)BiScO3-xPbTiO3 Piezoelectric Ceramics". En 2007 Sixteenth IEEE International Symposium on the Applications of Ferroelectrics. IEEE, 2007. http://dx.doi.org/10.1109/isaf.2007.4393341.
Texto completoStevenson, T., T. P. Comyn, A. J. Bell y R. Cywinski. "Multiferroic (ferroelectro-magnetic) properties of bismuth ferrite lead titanate x(BiFeO3)-1-x(PbTiO3)". En 2007 Sixteenth IEEE International Symposium on the Applications of Ferroelectrics. IEEE, 2007. http://dx.doi.org/10.1109/isaf.2007.4393285.
Texto completoBingrong Yuan, Shengwen Yu, Wufeng Yang, Xiaowen Zhou y Jinrong Cheng. "Composition dependence of xBiFeO3-(1-x)PbTiO3 films prepared by sol-gel technique". En 2009 18th IEEE International Symposium on the Applications of Ferroelectrics (ISAF). IEEE, 2009. http://dx.doi.org/10.1109/isaf.2009.5307556.
Texto completoVenkata, S. Avula, J. Heidler, J. Dreiser, J. Vijayakumar, L. Howald, F. Nolting y C. Piamonteze. "Magnetoelectric coupling between ultra-thin Fe films and Pb (Mg1/3Nb2/3) O3] (1−x)-[PbTiO3] x, x=0.32 (001) (PMN-PT) using x-ray magnetic circular dichroism". En 2017 IEEE International Magnetics Conference (INTERMAG). IEEE, 2017. http://dx.doi.org/10.1109/intmag.2017.8008023.
Texto completoQishou Li, Wei Shi, Yuzhi Jiang, Ying Pei, Qiang Chen, Xi Yue, Dingquan Xiao y Jianguo Zhu. "Effect of Y-doping on the piezoelectric properties of (1-x)BiScO3-xPbTiO3 high-temperature piezoelectric ceramics". En 2009 18th IEEE International Symposium on the Applications of Ferroelectrics (ISAF). IEEE, 2009. http://dx.doi.org/10.1109/isaf.2009.5307539.
Texto completoTurner, Stuart L., Tim P. Comyn y Andrew J. Bell. "Comparison of Surface and Bulk Crystal Structure in the xBiFeO3-(1-x)PbTiO3 Solid Solution System". En 2006 IEEE International Symposium on the Applications of Ferroelectrics. IEEE, 2006. http://dx.doi.org/10.1109/isaf.2006.4387852.
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