Artículos de revistas sobre el tema "(x)BiScO3-(1-x)PbTiO3"

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1

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.

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2

Chen, 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.

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(1-x)BiScO3-xPbTiO3 (BSPT) based ferroelectric ceramics were prepared by conventional solid state process. X-ray diffraction analysis revealed that the morphotropic phase boundary (MPB) separating the rhombohedral and tetragonal phases for the BSPT system exited near x=0.62. It was found that the stability of perovskite structure of the BSPT system was improved with the increase of PbTiO3 content. For the 0.36BiScO3-0.64Pb1-ySryTiO3 (BSPST) system, because of higher amount of ionic bonding, the stability of perovskite structure for BSPT compounds containing strontium is larger than that of non-strontium compound.
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3

Alekseev, 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.

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4

Sun, 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.

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In this study, (1–x)Bi0.5Na0.5TiO3– xBiScO3 (BNT–xBS) ceramics were synthesized via conventional solidstate reaction sintering. The effects of the BiScO3 content on the surface microstructure, energy storage, strain, and dielectric properties of BNT–xBS ceramics were systemically investigated. Results indicated that the phase structure of BNT–xBS ceramics transformed from the rhombohedral phase into the pseudo-cubic phase. As the increasing BiScO3 content, the average grain size decreased. BiScO3 destroyed the long-range ordered ferroelectric phase, enhancing relaxor behavior. Energy storage density initially increased and then decreased, reaching a maximum of 0.17 J/cm3 at x = 0.1. In addition, the maximum energy storage efficiency was 59% at x = 0.2. The BiScO3 content significantly affected the electrical properties of BNT– xBS ceramics.
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5

Kowalski, 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.

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6

Porokhonskyy, 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.

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7

Tai, 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.

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8

Kowalski, 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.

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9

Yang, 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.

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10

Zhao, 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.

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11

Winotai, Pongtip, Nitinai Udomkan y Siwaporn Meejoo. "Piezoelectric properties of Fe2O3-doped (1−x)BiScO3–xPbTiO3 ceramics". Sensors and Actuators A: Physical 122, n.º 2 (agosto de 2005): 257–63. http://dx.doi.org/10.1016/j.sna.2005.06.008.

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12

Zhang, Shaopeng, Xiaohui Wang y Longtu Li. "Raman Spectra and Phase Transition in (1−x)BiScO3−xPbTiO3Nanopowders". Ferroelectrics 450, n.º 1 (enero de 2013): 28–34. http://dx.doi.org/10.1080/00150193.2013.838463.

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13

Zhao, Wei, Xiaohui Wang, Longtu Li y Zhilun Gui. "Synthesis of nanosized (1 − x)BiScO3 − xPbTiO3 ferroelectric ceramic powders". Journal of Electroceramics 21, n.º 1-4 (20 de agosto de 2007): 625–28. http://dx.doi.org/10.1007/s10832-007-9248-6.

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14

Eitel, R. E., S. J. Zhang, T. R. Shrout, C. A. Randall y I. Levin. "Phase Diagram of the Perovskite System (1−x)BiScO3-xPbTiO3". Journal of Applied Physics 96, n.º 5 (septiembre de 2004): 2828–31. http://dx.doi.org/10.1063/1.1777810.

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15

Duan, Runrun, Michael S. Haluska y Robert F. Speyer. "Multiple dielectric anomalies in xBiLaO3–(1 − x)PbTiO3 piezoelectrics". Journal of Materials Research 23, n.º 2 (febrero de 2008): 565–69. http://dx.doi.org/10.1557/jmr.2008.0074.

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Compositions of xBiLaO3–(1 − x) PbTiO3 over the range 0 ≤ x ≤ 0.225 were calcined and sintered. The dielectric constant with temperature and differential scanning calorimetry measurements were in excellent agreement with respect to Curie-like tetragonal to cubic transformations starting at 495 °C for pure PbTiO3, shifting to lower temperatures with increasing x. For compositions of x ≥ 0.05, a second higher-temperature (∼600 °C) endotherm, and matching dielectric anomaly, were consistently observed, for which there were no structural changes indicated by hot-stage x-ray diffraction. This transformation was speculated to be based on a thermally induced desegregation of B-site cations.
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16

Yao, Zhonghua, Hanxing Liu, Yang Liu, Zhaohui Wu, Minghe Cao y Hua Hao. "High-temperature relaxor cobalt-doped (1−x)BiScO3-xPbTiO3 piezoelectric ceramics". Applied Physics Letters 92, n.º 14 (7 de abril de 2008): 142905. http://dx.doi.org/10.1063/1.2904615.

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17

Topolov, V. Yu. "Heterophase states and a bridging phase in (1-x)BiScO3−xPbTiO3". Crystal Research and Technology 47, n.º 10 (30 de julio de 2012): 1054–63. http://dx.doi.org/10.1002/crat.201200243.

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18

Pham-Thi, Mai, Henri Hemery y Hichem Dammak. "X ray investigation of high oriented (1−x)PbMg1/3Nb2/3O3–(x)PbTiO3 ceramics". Journal of the European Ceramic Society 25, n.º 12 (enero de 2005): 2433–35. http://dx.doi.org/10.1016/j.jeurceramsoc.2005.03.077.

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19

Skidmore, Thomas A., Timothy P. Comyn y Steven J. Milne. "Dielectric and Piezoelectric Properties in the System: (1−x)[(Na0.5K0.5NbO3)0.93-(LiTaO3)0.07]-x[BiScO3]". Journal of the American Ceramic Society 93, n.º 3 (marzo de 2010): 624–26. http://dx.doi.org/10.1111/j.1551-2916.2009.03470.x.

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20

Singh, K., N. S. Negi, R. K. Kotnala y M. Singh. "Dielectric and magnetic properties of (BiFeO3)1−x(PbTiO3)x ferromagnetoelectric system". Solid State Communications 148, n.º 1-2 (octubre de 2008): 18–21. http://dx.doi.org/10.1016/j.ssc.2008.07.022.

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21

Singh, Ajay, Vishal Singh y K. K. Bamzai. "Structural and magnetic studies on (x)PbTiO3 – (1 − x)SrFe12O19 composite multiferroics". Materials Chemistry and Physics 155 (abril de 2015): 92–98. http://dx.doi.org/10.1016/j.matchemphys.2015.02.004.

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22

Yang, Xiaoming, Chao He, Ying Liu, Xiuzhi Li, Zujian Wang, Shujuan Han, Shilie Pan y Xifa Long. "Structural and Electrical Characteristics of (1−x )Pb(Lu1/2 Nb1/2 )O3 -x PbTiO3 Ceramics with Low PbTiO3". Journal of the American Ceramic Society 99, n.º 10 (16 de junio de 2016): 3325–29. http://dx.doi.org/10.1111/jace.14321.

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23

Бехтин, М. А., А. А. Буш y А. Г. Сегалла. "Получение и электрофизические свойства керамики (1–x)BiScO3⇒xPbTiO3с добавками MnO2и Ni2O3". Неорганические материалы 50, n.º 1 (2014): 104–10. http://dx.doi.org/10.7868/s0002337x14010023.

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24

Zhuang, Jian, Jinming Lu, Alexei A. Bokov, Nan Zhang, Jie Zhang, Hua Wu, Wei Ren y Zuo-Guang Ye. "Magnetic properties of multiferroic (1-x)PbTiO3-xDyFeO3 system". Ferroelectrics 534, n.º 1 (3 de octubre de 2018): 206–11. http://dx.doi.org/10.1080/00150193.2018.1473689.

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25

Zou, Ting Ting, Xiao Hui Wang y Long Tu Li. "Preparation and Characterization of (1-x)BiScO3-xPbTiO3 Ceramics by Two-Step Sintering". Key Engineering Materials 368-372 (febrero de 2008): 8–10. http://dx.doi.org/10.4028/www.scientific.net/kem.368-372.8.

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High-performance fine-grain (1-x)BiScO3-xPbTiO3 ceramics were prepared by two-step sintering method. Influences of sintering temperature, holding time, and composition on the microstructure and properties were discussed. The BSPT ceramics obtained via two-step sintering reaches density higher than 95% at a low temperature of 800°C without any sintering aid, and the grain size of the ceramics is also effectively controlled. Excellent piezoelectric properties between the composition of x=0.63 and x=0.64 reveals a probable MPB in this range, suggesting a potential approach to pursue high performance BSPT ceramics.
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26

Singh, K., Ashish Gautam, K. Sen, R. K. Kotnala, Mahesh Kumar, P. Gautam y M. Singh. "Room temperature long range ferromagnetic ordering in (BiFeO3)1−x (PbTiO3)x nanocrystallites". Journal of Applied Physics 109, n.º 12 (15 de junio de 2011): 123911. http://dx.doi.org/10.1063/1.3592281.

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27

Ansell, Troy Y., David P. Cann, Eva Sapper y Jürgen Rödel. "Thermal Depolarization in the High-Temperature Ternary Piezoelectric System x PbTiO3 -y BiScO3 -z Bi(Ni1/2 Ti1/2 )O3". Journal of the American Ceramic Society 98, n.º 2 (13 de octubre de 2014): 455–63. http://dx.doi.org/10.1111/jace.13268.

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28

Bilalodin, Bilalodin. "PENUMBUHAN DAN KARAKTERISASI LAPISAN TIPIS PbTiO3 YANG DISIAPKAN DENGAN TEKNIK SPIN COATING". Molekul 3, n.º 1 (1 de mayo de 2008): 48. http://dx.doi.org/10.20884/1.jm.2008.3.1.47.

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The growth of PbTiO3 ferroelectric thin films have successfully done. Thin films were made from bulk (powder) PbTiO3 dissolved in methanol solution. The condensation was mixed during 1 hour to get homogeneous condensation. Thin films were grown above corning substrates by spin coating method. Optimation was done by various of annealing temperature. The physical properties of thin films were characterized by Energi Dispersive X-Ray Spectroscopy (EDS), X-Ray Diffraction (XRD), Scanning and Electron Microscopy (SEM). EDS measurement showed that the stoichiometry composition ratio of Pb/Ti is 1/1.26 at annealing temperature 600oC and 1/1.29 at annealing temperature 700oC. The result of XRD pattern showed that crystal structure of PbTiO3 thin films are tetragonal. The calculated lattice parameters ontained from Chohen Method are a=b= 3.873 Å dan c= 4.130Å. The result of SEM PbTiO3 thin film showed that thin film has globular grain size.
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29

Eitel, Richard E., Thomas R. Shrout y Clive A. Randall. "Tailoring Properties and Performance of (1-x)BiScO3–xPbTiO3Based Piezoceramics by Lanthanum Substitution". Japanese Journal of Applied Physics 43, n.º 12 (9 de diciembre de 2004): 8146–50. http://dx.doi.org/10.1143/jjap.43.8146.

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30

Chen, Si, Xianlin Dong, Chaoliang Mao y Fei Cao. "Thermal Stability of (1?x)BiScO3?xPbTiO3Piezoelectric Ceramics for High-Temperature Sensor Applications". Journal of the American Ceramic Society 89, n.º 10 (octubre de 2006): 3270–72. http://dx.doi.org/10.1111/j.1551-2916.2006.01201.x.

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31

Zou, Tingting, Xiaohui Wang, Han Wang, Caifu Zhong, Longtu Li y I.-Wei Chen. "Bulk dense fine-grain (1−x)BiScO3–xPbTiO3 ceramics with high piezoelectric coefficient". Applied Physics Letters 93, n.º 19 (10 de noviembre de 2008): 192913. http://dx.doi.org/10.1063/1.2995861.

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32

Li, X. Z., Q. Wei, Z. J. Wang y X. F. Long. "Relaxor behaviour of (1−x)Ba(Sc1/2Nb1/2)O3−x PbTiO3 solid solution". Materials Research Innovations 14, n.º 2 (abril de 2010): 110–12. http://dx.doi.org/10.1179/143307510x12599329343763.

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33

Surowiak, Z., M. F. Kupriyanov, A. E. Panich y R. Skulski. "The properties of the non-stoichiometric ceramics (1−x)PbMg1/3Nb2/3O3–(x)PbTiO3". Journal of the European Ceramic Society 21, n.º 15 (enero de 2001): 2783–86. http://dx.doi.org/10.1016/s0955-2219(01)00363-6.

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34

Rai, Radheshyam, Abinhav Sinha, Seema Sharmac y N. K. P. Sinha. "Investigation of structural and electrical properties of (1−x) Bi0.5Mg0.5TiO3–(x) PbTiO3 ceramic system". Journal of Alloys and Compounds 486, n.º 1-2 (noviembre de 2009): 273–77. http://dx.doi.org/10.1016/j.jallcom.2009.06.124.

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35

Martín-Arias, L., A. Castro y M. Algueró. "Ferroelectric phases and relaxor states in the novel lead-free (1 − x) Bi1/2K1/2TiO3 − x BiScO3 system (0 ≤ x ≤ 0.3)". Journal of Materials Science 47, n.º 8 (7 de enero de 2012): 3729–40. http://dx.doi.org/10.1007/s10853-011-6222-0.

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36

Ivanov, Oleg, Elena Danshina, Yulia Tuchina y Viacheslav Sirota. "Diffuse Phase Transition and Ferroelectric Properties of Ceramic Solid Solutions in New SrTiO3-BiScO3 System". Advances in Science and Technology 67 (octubre de 2010): 59–63. http://dx.doi.org/10.4028/www.scientific.net/ast.67.59.

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Ceramic solid solutions of (1-x)SrTiO3-(x)BiScO3 system with x=0, 0.05, 0.1, 0.2, 0.3, 0.4 and 0.5 have been for the first time synthesized via solid-state processing techniques. Both of end compounds in this system are not ferroelectric materials. X-ray diffraction analysis revealed that at room temperature the samples under study at x=0.2, 0.3, 0.4 and 0.5 consist of mixture of center-symmetric cubic Pm3m phase and polar tetragonal P4mm phase. Anomalous behaviour of dielectric permittivity and dielectric losses for these samples is found to be specific one for ferroelectrics with diffuse phase transitions. Furthermore, examination of the polarization hysteresis behavior revealed weakly nonlinear hysteresis loops in the ferroelectric phase.
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37

Tu, Chi-Shun, C. L. Tsai, V. Hugo Schmidt, Haosu Luo y Zhiwen Yin. "Dielectric, hypersonic, and domain anomalies of (PbMg1/3Nb2/3O3)1−x(PbTiO3)x single crystals". Journal of Applied Physics 89, n.º 12 (15 de junio de 2001): 7908–16. http://dx.doi.org/10.1063/1.1370998.

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38

Zhang, R., S. Peng, D. Xiao, Y. Wang, B. Yang, J. Zhu, P. Yu y W. Zhang. "Preparation and Characterization of (1 —x) Pb(Mg1/3Nb2/3) O3 —x PbTiO3 Electrocaloric Ceramics". Crystal Research and Technology 33, n.º 5 (1998): 827–32. http://dx.doi.org/10.1002/(sici)1521-4079(1998)33:5<827::aid-crat827>3.0.co;2-h.

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39

Kwon, Do-Kyun, Clive A. Randall, Thomas R. Shrout y Michael T. Lanagan. "Dielectric Properties and Relaxation in (1−x)BiScO3-xBa(Mg1/3Nb2/3)O3Solid Solutions". Journal of the American Ceramic Society 87, n.º 6 (junio de 2004): 1088–92. http://dx.doi.org/10.1111/j.1551-2916.2004.01088.x.

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40

Jiang, Yihang, Baoquan Qin, Yi Zhao, Yuzhi Jiang, Wei Shi, Qishou Li, Dingquan Xiao y Jianguo Zhu. "Phase Transition, Piezoelectric Properties, and Thermal Stability of (1−x−y)BiScO3-yBiGaO3-xPbTiO3Ceramics". Journal of the American Ceramic Society 91, n.º 9 (septiembre de 2008): 2943–46. http://dx.doi.org/10.1111/j.1551-2916.2008.02580.x.

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41

Tao, Hong y JiaGang Wu. "Composition dependence of phase structure and electrical properties of (1−y)Bi1−x Nd x FeO3−y BiScO3 ceramics". Science China Technological Sciences 59, n.º 7 (2 de junio de 2016): 1029–35. http://dx.doi.org/10.1007/s11431-016-6051-0.

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42

Shi, Wei, Ying Pei, Jianshuai Wei, Qiang Chen, Dingquan Xiao y Jianguo Zhu. "Dielectric and Piezoelectric Properties of (1-x)(0.36BiScO3-0.64 PbTiO3)-xBiYbO3Ceramics". Ferroelectrics 409, n.º 1 (noviembre de 2010): 3–7. http://dx.doi.org/10.1080/00150193.2010.485836.

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43

Peng, Xin, Huajun Kang, Laijun Liu, Changzheng Hu, Liang Fang, Jun Chen y Xianran Xing. "Multiferroic properties and enhanced magnetoelectric coupling in (1 − x)PbTiO3 − xNdFeO3". Solid State Sciences 15 (enero de 2013): 91–94. http://dx.doi.org/10.1016/j.solidstatesciences.2012.09.007.

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44

Zhukov, S. G., V. V. Chernyshov y S. B. Vakhrushev. "Structural peculiarities of (PbMg1/3Nb2/3O3)1-x-(PbTiO3)xsolid solutions". Ferroelectrics 235, n.º 1 (diciembre de 1999): 143–49. http://dx.doi.org/10.1080/00150199908214874.

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45

Hu, Penghao, Jun Chen, Xueyi Sun, Jinxia Deng, Xi Chen, Ranbo Yu, Lijie Qiao y Xianran Xing. "Zero thermal expansion in (1−x)PbTiO3–xBi(Mg,Ti)1/2O3 piezoceramics". Journal of Materials Chemistry 19, n.º 11 (2009): 1648. http://dx.doi.org/10.1039/b816822a.

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46

Tawfik, A., D. M. Hemeda, M. Z. Said y M. M. Yousef. "Structural Properties of the Ferroelectric Nanocomposite (1-x) BaTiO3–(x) PbTiO3 Prepared by Tartrate Acid Method". Physical Science International Journal 20, n.º 1 (17 de noviembre de 2018): 1–17. http://dx.doi.org/10.9734/psij/2018/44797.

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47

Ranjith, R. y S. B. Krupanidhi. "Antiferroelectriclike polarization behavior in compositionally varying (1−x) Pb(Mg1∕3Nb2∕3)O3–(x) PbTiO3 multilayers". Applied Physics Letters 91, n.º 8 (20 de agosto de 2007): 082907. http://dx.doi.org/10.1063/1.2775044.

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48

Zhang, Xinyang, Thomas J. Kennedy, Eugene V. Colla, M. B. Weissman y D. D. Viehland. "Non-equilibrium strain relaxation noise in the relaxor ferroelectric (PbMg1/3Nb2/3O3)1-x(PbTiO3)x". Journal of Applied Physics 124, n.º 23 (21 de diciembre de 2018): 234102. http://dx.doi.org/10.1063/1.5049816.

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Randall, C. A., R. Eitel, B. Jones, T. R. Shrout, D. I. Woodward y I. M. Reaney. "Investigation of a high Tc piezoelectric system: (1−x)Bi(Mg1/2Ti1/2)O3–(x)PbTiO3". Journal of Applied Physics 95, n.º 7 (abril de 2004): 3633–39. http://dx.doi.org/10.1063/1.1625089.

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Zou, Tingting, Xiaohui Wang, Wei Zhao y Longtu Li. "Preparation and Properties of Fine-Grain (1−x)BiScO3−xPbTiO3 Ceramics by Two-Step Sintering". Journal of the American Ceramic Society 91, n.º 1 (17 de diciembre de 2007): 121–26. http://dx.doi.org/10.1111/j.1551-2916.2007.01903.x.

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