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Journal articles on the topic 'Electric field induced phase transition'

Author: Grafiati
Published: 7 July 2024
Last updated: 31 July 2025

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1

Lelidis, I., and G. Durand. "Electric-field-induced isotropic-nematic phase transition." Physical Review E 48, no. 5 (1993): 3822–24. http://dx.doi.org/10.1103/physreve.48.3822.

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2

Hinterstein, Manuel, Michael Knapp, Markus Hölzel, et al. "Field-induced phase transition in Bi1/2Na1/2TiO3-based lead-free piezoelectric ceramics." Journal of Applied Crystallography 43, no. 6 (2010): 1314–21. http://dx.doi.org/10.1107/s0021889810038264.

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The origin of the electric field-induced strain in the polycrystalline ceramic 0.92Bi1/2Na1/2TiO3–0.06BaTiO3–0.02K1/2Na1/2NbO3was investigated usingin situhigh-resolution X-ray and neutron diffraction techniques. The initially existing tetragonal phase with pseudocubic lattice undergoes a reversible phase transition to a significantly distorted rhombohedral phase under electric field, accompanied by a change in the oxygen octahedral tilting froma0a0c+toa−a−a−and in the tilting angle. The polarization values for the tetragonal and rhombohedral phases were calculated based on the structural info
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3

Камзина, Л. С. "Индуцированный фазовый переход в монокристаллических твердых растворах PbMg-=SUB=-1/3-=/SUB=-Nb-=SUB=-2/3-=/SUB=-O-=SUB=-3-=/SUB=--29PbTiO-=SUB=-3-=/SUB=- и PbZn-=SUB=-1/3-=/SUB=-Nb-=SUB=-2/3-=/SUB=-O-=SUB=-3-=/SUB=--9PbTiO-=SUB=-3-=/SUB=-: сходство и различие". Физика твердого тела 63, № 11 (2021): 1880. http://dx.doi.org/10.21883/ftt.2021.11.51591.152.

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The kinetics of the induced phase transition in single-crystal relaxor solid solutions PbMg1 / 3Nb2 / 3O3-29PbTiO3 and PbZn1 / 3Nb2 / 3O3-9PbTiO3 is studied when an electric field is applied along the [001] direction. At temperatures below the temperature of the morphotropic phase transition, the changes in the dielectric constant and optical transmission in electric fields are studied. It is shown that the decrease in optical transmission with time is associated only with a change in the sizes of nanoregions during the phase transition. It was found that the induced phase transition proceeds
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4

Kamzina L.S. "Induced phase transition in monocrystalline solids solutions PbMg-=SUB=-1/3-=/SUB=-Nb-=SUB=-2/3-=/SUB=-O-=SUB=-3-=/SUB=--29PbTiO-=SUB=-3-=/SUB=- and PbZn-=SUB=-1/3-=/SUB=-Nb-=SUB=-2/3-=/SUB=-O-=SUB=-3-=/SUB=--9PbTiO-=SUB=-3-=/SUB=-: similarity and difference." Physics of the Solid State 63, no. 13 (2022): 1743. http://dx.doi.org/10.21883/pss.2022.13.52315.152.

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The kinetics of the induced phase transition in single-crystal relaxor solid solutions PbMg1/3Nb2/3O3-29PbTiO3 and PbZn1/3Nb2/3O3-9PbTiO3 is studied when an electric field is applied along the [001] direction. At temperatures below the temperature of the morphotropic phase transition, the changes in the dielectric constant and optical transmission in electric fields are studied. It is shown that the decrease in optical transmission with time is associated only with a change in the sizes of nanoregions during the phase transition. It was found that the induced phase transition proceeds differen
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5

Zhang, Yu, Weiping Gong, Zhen Li, et al. "Two Consecutive Negative Electrocaloric Peaks in <001>-Oriented PMN-30PT Single Crystals." Crystals 14, no. 5 (2024): 458. http://dx.doi.org/10.3390/cryst14050458.

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The versatile electrocaloric (EC) behaviors of the (1-x)Pb(Mg1/3Nb2/3)O3-xPT (PMN-100xPT) single crystal are closely related to the multiple phase transitions under the multiple fields of electric field and temperature. In this work, the EC effect of &lt;001&gt;-oriented PMN-30PT single crystals with chemical composition at morphotropic phase boundary has been studied during the phase transformation process from the ferroelectric rhombohedral (R) phase to the tetragonal (T) phase. Two consecutive negative EC peaks have been achieved for the first time. Based on the projection of the EC effect
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6

Hirotsu, Shunsuke. "Electric-Field-Induced Phase Transition in Polymer Gels." Japanese Journal of Applied Physics 24, S2 (1985): 396. http://dx.doi.org/10.7567/jjaps.24s2.396.

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7

Tao, R. "Electric-field-induced phase transition in electrorheological fluids." Physical Review E 47, no. 1 (1993): 423–26. http://dx.doi.org/10.1103/physreve.47.423.

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8

Li, Zhen Rong, Jun Jie Qian, Guo Qiang Zhang, Zeng Zhe Xi, Zhuo Xu, and Xi Yao. "Dielectric Properties and Phase Transition of [110]-Oriented 0.68PMN-0.32PT Single Crystals Induced by Temperature and DC Electric Field." Key Engineering Materials 336-338 (April 2007): 42–45. http://dx.doi.org/10.4028/www.scientific.net/kem.336-338.42.

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The dielectric response of [110]-oriented 0.68PMN-0.32PT single crystal under dc electric field has been investigated. The characteristics of phase transition under temperature and dc electric field are provided. When electric field is above 2.3kV/cm, abnormal phase transition is induced by temperature and electric field, which corresponds to the phase transition from rhombohedral to orthorhombic ferroelectric phase. With increasing dc electric field, the stable temperature region of orthorhombic phase is expanded. The electric field-temperature (E-T) phase diagram of [110]-oriented 0.68PMN-0.
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9

Shabbir, Ghulam. "Aging Behavior and Electric Field Induced Instabilities in Lead Magnesium Niobate - Titanate Relaxor Ferroelectric Single Crystal." Key Engineering Materials 778 (September 2018): 212–16. http://dx.doi.org/10.4028/www.scientific.net/kem.778.212.

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The aging characteristics and influence of electric field poling on the phase transitions in (1-x)Pb (Mg1/3Nb2/3)O3-xPbTiO3 (PMN-xPT) [110]-oriented single crystal were examined through temperature dependent complex capacitance study. In addition to two phase transition anomalies exhibited by the crystal in the virgin state, other phase transition instabilities were observed in the complex capacitance of the crystal under the external applied electric field. The aging behavior deviated from the linear logarithmic law and followed the stretched exponential expression typical for relaxor ferroel
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10

Kawasugi, Yoshitaka, Hikaru Masuda, Jiang Pu та ін. "Electric Double Layer Doping of Charge-Ordered Insulators α-(BEDT-TTF)2I3 and α-(BETS)2I3". Crystals 11, № 7 (2021): 791. http://dx.doi.org/10.3390/cryst11070791.

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Field-effect transistors based on strongly correlated insulators are an excellent platform for studying the electronic phase transition and simultaneously developing phase transition transistors. Molecular conductors are suitable for phase transition transistors owing to the high tunability of the electronic states. Molecular Mott transistors show field-induced phase transitions including superconducting transitions. However, their application to charge-ordered insulators is limited. In this study, we fabricated electric double layer transistors based on quarter-filled charge-ordered insulator
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11

Moriwake, Hiroki, Ayako Konishi, Takafumi Ogawa, Craig A. J. Fisher, Akihide Kuwabara, and Desheng Fu. "The electric field induced ferroelectric phase transition of AgNbO3." Journal of Applied Physics 119, no. 6 (2016): 064102. http://dx.doi.org/10.1063/1.4941319.

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12

Mukherjee, Prabir K., and Muklesur Rahman. "Electric-field induced isotropic to smectic-C phase transition." Journal of Molecular Liquids 196 (August 2014): 204–7. http://dx.doi.org/10.1016/j.molliq.2014.03.034.

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13

Li, Changhui, Xiangqun Zhang, Zhaohua Cheng, and Young Sun. "Electric field induced phase transition in charge-ordered LuFe2O4." Applied Physics Letters 93, no. 15 (2008): 152103. http://dx.doi.org/10.1063/1.3001591.

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14

Giacomelli, Fernando C., Nádya P. da Silveira, Frédéric Nallet, Petr Černoch, Miloš Steinhart, and Petr Štěpánek. "Cubic to Hexagonal Phase Transition Induced by Electric Field." Macromolecules 43, no. 9 (2010): 4261–67. http://dx.doi.org/10.1021/ma1000817.

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15

Helal, Md Al, and Seiji Kojima. "Effect of electric field on elastic properties of BaTiO3 single crystals: a micro-Brillouin scattering study." Japanese Journal of Applied Physics 61, SG (2022): SG1016. http://dx.doi.org/10.35848/1347-4065/ac4c6f.

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The analysis of local polar clusters formed by random fields in ferroelectrics is of technical and fundamental importance in understanding piezoelectricity. The temperature and electric field dependences of elastic properties and the ferroelectric phase transition have been investigated in (100)-oriented BaTiO3 single crystals by micro-Brillouin scattering. In the field cooling process, LA phonons are scattered by polar clusters. As a result, the LA phonon frequency increases as compared with that of the zero-field cooling process. Under the application of an external electric field along the
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16

Moshnyaga, Vasily, and Konrad Samwer. "Polaronic Emergent Phases in Manganite-based Heterostructures." Crystals 9, no. 10 (2019): 489. http://dx.doi.org/10.3390/cryst9100489.

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Transition metal functional oxides, e.g., perovskite manganites, with strong electron, spin and lattice correlations, are well-known for different phase transitions and field-induced colossal effects at the phase transition. Recently, the interfaces between dissimilar perovskites were shown to be a promising concept for the search of emerging phases with novel functionalities. We demonstrate that the properties of manganite films are effectively controlled by low dimensional emerging phases at intrinsic and extrinsic interfaces and appeared as a result of symmetry breaking. The examples includ
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17

He, Hui-Kai, Yong-Bo Jiang, Jun Yu, et al. "Ultrafast and stable phase transition realized in MoTe2-based memristive devices." Materials Horizons 9, no. 3 (2022): 1036–44. http://dx.doi.org/10.1039/d1mh01772a.

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An electric-field induced phase transition between semiconducting 2H and metallic 1T′ phases in a MoTe2 device is demonstrated for the first time. The phase transition exhibits faster switching compared with phase-change random-access memory (PCRAM), and shows more controllable switching than conventional memristive devices.
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18

Wang, Peng-Fei, Qianqian Hu, Tan Zheng, Yu Liu, Xiaofeng Xu, and Jia-Lin Sun. "Optically Monitored Electric-Field-Induced Phase Transition in Vanadium Dioxide Crystal Film." Crystals 10, no. 9 (2020): 764. http://dx.doi.org/10.3390/cryst10090764.

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Vanadium dioxide (VO2), due to its electrically induced metal-to-insulator transition with dramatic changes in electrical and optical properties, is considered to be a powerful material for electro-optical devices. However, there are still some controversies about phase transition mechanism under voltage. Here, based on optical characterizations on VO2 crystal nanofilm during the whole process of phase transition, temporal evolution and spatial distribution of changes in electricity, optic and temperature are investigated simultaneously, to explore the mechanism. The variations of Raman spectr
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19

Ando, Ryosuke, Ryo Watanuki, Kazuhiro Kudo, Hyuma Masu та Masatoshi Sakai. "Phase Transition Field Effect Transistor Observed in an α-(BEDT-TTF)2I3 Single Crystal". Solids 4, № 3 (2023): 201–12. http://dx.doi.org/10.3390/solids4030013.

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The metal–insulator transition induced by the gate electric field in the charge order phase of the α-(BEDT-TTF)2I3 single-crystal field-effect transistor (FET) structure was clearly observed near the phase transition temperature. An abrupt increase in the electrical conductance induced by the applied gate electric field was evident, which corresponds to the partial dissolution of the charge order phase triggered by the gate electric field. The estimated nominal dissolved charge order region (i.e., the gate-induced metallic region) was overestimated in 130–150 K, suggesting additional effects s
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20

Gorbatenko, V. V., B. N. Prasolov, S. A. Gorbatenko, and N. V. Datsenko. "Harmonic Analysis of the Polarization Reversal of the Rb2ZnCl4 Crystal in the Incommensurate Phase." Кристаллография 68, no. 5 (2023): 734–37. http://dx.doi.org/10.31857/s0023476123600453.

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The polarization reversal of Rb2ZnCl4 crystals in the incommensurate phase near a ferroelectric phase transition (PT) under the action of harmonic electric field has been studied using harmonic analysis. During polarization reversal of a test sample under the action of harmonic electric field, a PT induced by the electric field from the incommensurate phase to the ferroelectric phase and a PT from the field-induced ferroelectric phase back to the incommensurate phase occur. The study of the active and reactive contributions to the amplitudes of current density harmonics made it possible to det
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21

Li, Xiaojin, Quanxin Yang, Xin Zhang, Shan He, Hongliang Liu, and Pengfei Wu. "Low DC Electric-Field-Induced Phase Transition in KTa0.59Nb0.41O3 Crystal." Crystal Growth & Design 20, no. 2 (2019): 1248–53. http://dx.doi.org/10.1021/acs.cgd.9b01509.

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22

Thürk, Marcel, and Dietmar Porschke. "Phase transition of dimyristoylphosphatidylglycerol bilayers induced by electric field pulses." Biochimica et Biophysica Acta (BBA) - Biomembranes 1067, no. 2 (1991): 153–58. http://dx.doi.org/10.1016/0005-2736(91)90037-9.

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23

Li, Xian, Tian Qiu, Jiahao Zhang, et al. "Terahertz field–induced ferroelectricity in quantum paraelectric SrTiO3." Science 364, no. 6445 (2019): 1079–82. http://dx.doi.org/10.1126/science.aaw4913.

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“Hidden phases” are metastable collective states of matter that are typically not accessible on equilibrium phase diagrams. These phases can host exotic properties in otherwise conventional materials and hence may enable novel functionality and applications, but their discovery and access are still in early stages. Using intense terahertz electric field excitation, we found that an ultrafast phase transition into a hidden ferroelectric phase can be dynamically induced in quantum paraelectric strontium titanate (SrTiO3). The induced lowering in crystal symmetry yields substantial changes in the
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24

ZHOU, L. W., J. F. YE, R. B. TAO, et al. "PRELIMINARY OPTICAL STUDY ON ER FLUIDS." International Journal of Modern Physics B 08, no. 20n21 (1994): 2921–33. http://dx.doi.org/10.1142/s0217979294001214.

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Linear and nonlinear optical study on electrorheological (ER) fluids is reported. The ER fluids under the investigation were glass beads, zeolite and ferroelectrics. The linear optical response of some ER fluids showed sharp changes near critical electric fields. An enhancement of electric field induced second harmonic generations (EFISH) was observed as the function of E2, where E is the external electric field. The said enhancement is considered to be corresponding to a modulation of the material's refractive index associated with the electric field induced polarization of the delocalized el
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25

Lü, Xiao-Long, and Hang Xie. "Topological edge states and transport properties in zigzag stanene nanoribbons with magnetism." New Journal of Physics 24, no. 3 (2022): 033010. http://dx.doi.org/10.1088/1367-2630/ac4009.

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Abstract In this work, we investigate the topological phase transitions and corresponding transport properties in zigzag stanene nanoribbon with different magnetism. The results show that the off-resonant circularly polarized (ORCP) light may induce anisotropic chiral edge state with a magnetic phase transition from antiferromagnetic state to nonmagnetic state. In combination with the ORCP light and electric field, the 100% spin-polarized edge state can be induced with some magnetic orders. The finite-size effect is also an important factor for the magnetic phase transitions, which in turn ind
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26

GAO, J., E. J. GUO, S. Y. WANG, Z. P. WU, and H. J. BU. "TUNABLE PHASE TRANSITION AND PHOTO-INDUCED RESISTANCE IN La0.8Ca0.2MnO3/FERROELECTRIC HETEROSTRUCTURES." Modern Physics Letters B 27, no. 22 (2013): 1350162. http://dx.doi.org/10.1142/s0217984913501625.

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Heterostructures of La 0.8 Ca 0.2 MnO 3 (LCMO)/ferroelectric were formed by growing a layer of perovskite manganite LCMO on the ferroelectric 0.67 Pb ( Mg 1/3 Nb 2/3) O 3-0.33 PbTiO 3 (PMN-PT) single crystals. Well tunable structural, magnetic, and transport properties were achieved by applying electric fields on the formed heterostructures. By varying electric fields biased on the PMN-PT, the metal–insulator transition and resistance could be modulated continuously and reversely. Field modulation of photo-induced resistance (PR) was also observed. In situ X-ray diffraction indicates that the
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27

Nan, Tianxiang, Yeonbae Lee, Shihao Zhuang, et al. "Electric-field control of spin dynamics during magnetic phase transitions." Science Advances 6, no. 40 (2020): eabd2613. http://dx.doi.org/10.1126/sciadv.abd2613.

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Controlling magnetization dynamics is imperative for developing ultrafast spintronics and tunable microwave devices. However, the previous research has demonstrated limited electric-field modulation of the effective magnetic damping, a parameter that governs the magnetization dynamics. Here, we propose an approach to manipulate the damping by using the large damping enhancement induced by the two-magnon scattering and a nonlocal spin relaxation process in which spin currents are resonantly transported from antiferromagnetic domains to ferromagnetic matrix in a mixed-phased metallic alloy FeRh.
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28

Камзина, Л. С., Л. А. Кулакова та H. Luo. "Временные зависимости диэлектрических и акустических свойств в монокристаллах PbFe-=SUB=-0.5-=/SUB=-Nb-=SUB=-0.5-=/SUB=-O-=SUB=-3-=/SUB=- и PbFe-=SUB=-0.5-=/SUB=-Nb-=SUB=-0.5-=/SUB=-O-=SUB=-3-=/SUB=---7PbTiO-=SUB=-3-=/SUB=-". Физика твердого тела 61, № 4 (2019): 703. http://dx.doi.org/10.21883/ftt.2019.04.47416.308.

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AbstractThe time changes of permittivity, damping and velocity of sound are studied for PbFe_0.5Nb_0.5O_3 and PbFe_0.5Nb_0.5O_3–7PbTiO_3 single crystals in the electric fields of 0 &lt; E &lt; 6 kV/cm. The room-temperature local symmetry of these compounds is shown to be rather more monoclinic than rhombohedral, which is typical of other similar systems. No abrupt sound attenuation anomalies are observed upon the phase transition into the ferroelectric phase in the electric field. The effects seem to be far from the crystal symmetry changes and are attributed to the gradual transition of near-
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29

Meyer, Claire, Christophe Blanc, Geoffrey R. Luckhurst, Patrick Davidson, and Ivan Dozov. "Biaxiality-driven twist-bend to splay-bend nematic phase transition induced by an electric field." Science Advances 6, no. 36 (2020): eabb8212. http://dx.doi.org/10.1126/sciadv.abb8212.

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Although the existence of the twist-bend (NTB) and splay-bend (NSB) nematic phases was predicted long ago, only the former has as yet been observed experimentally, whereas the latter remains elusive. This is especially disappointing because the NSB nematic is promising for applications in electro-optic devices. By applying an electric field to a planar cell filled with the compound CB7CB, we have found an NTB-NSB phase transition using birefringence measurements. This field-induced transition to the biaxial NSB occurred, although the field was applied along the symmetry axis of the macroscopic
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30

Duan, Xiaodong, and Weili Luo. "EVIDENCE OF SECOND ORDER PHASE TRANSITION OF FERROFLUID IN EXTERNAL ELECTRIC FIELD." International Journal of Modern Physics B 15, no. 06n07 (2001): 837–41. http://dx.doi.org/10.1142/s0217979201005349.

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When a DC electric field is applied perpendicular to a thin film of ferrofluid constrained between two conducting plates, the ferrofluid separates into phases that are concentrated and dilute in magnetic particles for field strength above a critical value. The phase separation stems from the competition between the electrostatic energy and entropy of the induced dipoles. The entropy around the critical value of the phase separation is continues in our experiment indicating the transition is second order.
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31

JIANG, DONGDONG, YUJUN FENG, JINMEI DU, and YAN GU. "EFFECTS OF SHOCK PRESSURE AND SELF-GENERATED ELECTRIC FIELD ON SHOCK-INDUCED FERROELECTRIC TO ANTIFERROELECTRIC PHASE TRANSITION IN LEAD ZIRCONATE STANNATE TITANATE FERROELECTRIC CERAMICS." Journal of Advanced Dielectrics 02, no. 04 (2012): 1250026. http://dx.doi.org/10.1142/s2010135x12500269.

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Kinetics of the ferroelectric (FE) to antiferroelectric (AFE) phase transformation under shock wave compression is critical to design the shock-activated power supply and can be characterized in terms of both a transition rate and a limiting degree of transition. By measuring the depoling currents under the short-circuit and high-impedance conditions, we investigated the influence of shock pressure and self-generated electric field on the phase transition kinetics of tin-modified lead zirconate titanate ceramics (Pb0.99Nb0.02[(Zr0.90Sn0.10)0.96Ti0.04]0.98O3) in the pressure range from 0.23 to
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32

Artemenko, S. N. "Modification of charge density wave fluctuations by charge perturbations." Journal de Physique IV 12, no. 9 (2002): 77–78. http://dx.doi.org/10.1051/jp4:20020359.

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Spectral density of fluctuations of the CDW phase are calculated taking into account electric field induced by phase fluctuations. The approach based upon the fluctuation-dissipation theorem (FDT) combined with equations of linear response of the CDW conductor is used. Fluctuating electric field is found to suppress fluctuations of the phase, while fluctuations of the electric potential are sizeable. This suggests that transition from the CDW to the normal state (which is usually observed well below the mean-field transition temperature) may he provoked by fluctuations of the chemical potentia
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33

Камзина, Л. С., та G. Li. "Влияние концентрации La на кинетику индуцированного фазового перехода в прозрачной керамике PbMg-=SUB=-1/3-=/SUB=-Nb-=SUB=-2/3-=/SUB=-O-=SUB=-3-=/SUB=--25PbTiO-=SUB=-3-=/SUB=-". Физика твердого тела 62, № 4 (2020): 584. http://dx.doi.org/10.21883/ftt.2020.04.49124.644.

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The effect of La concentration on the kinetic nature of the induced phase transition in PbMg1/3Nb2/3O3–25PbTiO3 ferroceramics was studied. At temperatures below the Vogel-Fulcher temperature, the time-dependent changes in the dielectric constant and optical transmission in electric fields are studied 0 &lt;E &lt;6 kV / cm. It was found that in an electric field in La-containing transparent ceramics, a sharp decrease in the dielectric constant and optical transmission occurs over time, indicating an induced phase transition and an increase in the fraction of the ferroelectric phase. It has been
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34

Lyu, Jing, Zicong Marvin Wong, Haicheng Sun, Shuo-Wang Yang, and Guo Qin Xu. "Electric Field-Induced Phase Transition of Nanowires on Germanium(001) Surfaces." Journal of Physical Chemistry Letters 13, no. 4 (2022): 1063–68. http://dx.doi.org/10.1021/acs.jpclett.1c04020.

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35

Kamzina, L. S., and N. N. Krainik. "Electric-field-induced phase transition in single-crystal lead zinc niobate." Physics of the Solid State 40, no. 3 (1998): 485–88. http://dx.doi.org/10.1134/1.1130315.

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36

Gorev, M. V., V. S. Bondarev, and K. S. Aleksandrov. "Heat capacity of PMN near an electric-field-induced phase transition." JETP Letters 85, no. 6 (2007): 283–85. http://dx.doi.org/10.1134/s0021364007060045.

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37

Gordon, A., B. E. Vugmeister, S. Dorfman, and H. Rabitz. "Depolarization excitation as an electric field-induced first-order phase transition." Physica B: Condensed Matter 292, no. 3-4 (2000): 257–63. http://dx.doi.org/10.1016/s0921-4526(00)00476-2.

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38

Zhang, Mao-Hua, Lovro Fulanović, Sonja Egert, et al. "Electric-field-induced antiferroelectric to ferroelectric phase transition in polycrystalline NaNbO3." Acta Materialia 200 (November 2020): 127–35. http://dx.doi.org/10.1016/j.actamat.2020.09.002.

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39

Wang, Jin Fei, Tong Qing Yang, K. Wei, G. Li, and Yong Xiang Li. "Influence of Zr/Sn Ratio Electric Properties of PLZST Ceramic." Key Engineering Materials 547 (April 2013): 101–5. http://dx.doi.org/10.4028/www.scientific.net/kem.547.101.

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(Pb0.97La0.02)(Zr0.92-xSnxTi0.08)O3 (PLZST) ferroelectric ceramics with x=0.40, 0.25, 0.15, respectively, were investigated. It was found that these ceramics with different Zr:Sn ratios were perovskite structure. With increasing of Zr:Sn ratio, the phase-transition electric-field of antiferroelectric to ferroelectric phase increased. when x&gt;0.15,All the samples have double hysteresis loops with antiferroelectric phase characteristics. Yet, when the electric field was removed at lower temperature of -5oC and -20oC, for x=0.25 and 0.40, the electric field induced FE phase can remain metastabl
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40

Ivanov, V. Yu, A. M. Kuz’menko, A. Yu Tikhanovskii, and A. A. Mukhin. "Magnetic, Dielectric, and Magnetoelectric Phenomena Accompanying Low-Temperature Magnetic Transitions in GdFeO3." JETP Letters 121, no. 2 (2025): 95–102. https://doi.org/10.1134/s0021364024604354.

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A number of new features in the magnetic, magnetoelectric, and magnetodielectric properties of the GdFeO3 orthoferrite at phase transitions induced by a magnetic field H || a, b, c at low temperatures have been detected. A threefold increase in the permittivity in the form of peaks during spin-flip transitions in the Gd subsystem, which is accompanied by the suppression of the spontaneous electric polarization, as well as dielectric anomalies at a spin-reorientation (spin-flop) transition induced by the magnetic field H || a in the Gd and Fe subsystems in both ferroelectric $$(T &lt; T_{{\text
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41

Sun, Xiaohui, Houbing Huang, Hasnain Mehdi Jafri, Junsheng Wang, Yongqiang Wen, and Zhi-Min Dang. "Wide Electrocaloric Temperature Range Induced by Ferroelectric to Antiferroelectric Phase Transition." Applied Sciences 9, no. 8 (2019): 1672. http://dx.doi.org/10.3390/app9081672.

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The ferroelectric (FE) to antiferroelectric (AFE) phase transition tuning the temperature range of electrocaloric (EC) effects was investigated using phenomenological Landau–Devonshire theory. Contrary to ferroelectric to paraelectric (PE) phase transitions for electrocaloric effects, the ferroelectric to antiferroelectric phase transition was adopted to obtain large entropy changes under an applied electric field in a Sm-doping BiFeO3 system. In addition, the doping composition and hydrostatic pressure was observed to tune the ferroelectricantiferroelectric–paraelectric phase transition tempe
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42

Behera, Sushant Kumar, and Pritam Deb. "Controlling the bandgap in graphene/h-BN heterostructures to realize electron mobility for high performing FETs." RSC Advances 7, no. 50 (2017): 31393–400. http://dx.doi.org/10.1039/c7ra06069f.

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43

Wang, Jian, Yun Liu, Andrew Studer, Lasse Norén, and Ray Withers. "Effect of Electric Field and Temperature on Average Structure and Domain Wall Motion in 0.93Bi0.5Na0.5TiO3-0.07BaTiO3Ceramic." Advances in Condensed Matter Physics 2013 (2013): 1–4. http://dx.doi.org/10.1155/2013/830971.

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In situneutron powder diffraction patterns and dielectric spectra of 0.93Bi0.5Na0.5TiO3-0.07BaTiO3ceramic were investigated under different electrical fields and temperatures. An electric-field-induced phase transition from metrically cubic to metrically tetragonal, associated with strong domain wall motion, occurs. Such induced phase and domain wall motion are unchanged until the high-temperature phase transition occurs from metrically tetragonal to metrically cubic. All these changes are irrelevant to the observed depolarization temperature (75°C). The depolarization behaviour is thus sugges
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44

Porsch, F., and H. Stegemeyer. "Electric Field Induced Phase Transitions in Liquid-Crystalline Blue Phases." Liquid Crystals 2, no. 3 (1987): 395–99. http://dx.doi.org/10.1080/02678298708086684.

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45

Wexler, Adam D., Elmar C. Fuchs, Jakob Woisetschläger, and Giuseppe Vitiello. "Electrically induced liquid–liquid phase transition in water at room temperature." Physical Chemistry Chemical Physics 21, no. 34 (2019): 18541–50. http://dx.doi.org/10.1039/c9cp03192h.

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46

Tang, H., Y. J. Feng, Z. Xu, C. H. Zhang, and J. Q. Gao. "Effect of Nb doping on microstructure and electric properties of lead zirconate stannum titanate antiferroelectric ceramics." Journal of Materials Research 24, no. 5 (2009): 1642–45. http://dx.doi.org/10.1557/jmr.2009.0202.

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The aim of this work is to study the effect of Nb element doping on the microstructure and electrical properties of lead zirconate stannum titanate (PZST) ceramic and to improve phase transition properties of PZST. Nb-doped Pb(Zr,Sn,Ti)O3 ceramic samples were prepared by the conventional mixed oxide method. Phase transitions induced by temperature, pressure, and electric field were measured with electric dielectric permittivity, hydrostatic pressure, and hysteresis. The microstructure of the samples was observed by electron scanning microscope to discuss the effect of Nb doping on PZST ceramic
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47

Kamzina L. S. "Peculiarities of the induced phase transition in single-crystal solid solutions Na-=SUB=-1/2-=/SUB=-Bi-=SUB=-1/2-=/SUB=-TiO-=SUB=-3-=/SUB=--5 %BaTiO-=SUB=-3-=/SUB=-." Physics of the Solid State 64, no. 6 (2022): 654. http://dx.doi.org/10.21883/pss.2022.06.53828.288.

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The dielectric and optical properties, as well as the time dependences of the permittivity in an electric field applied along the [001] direction, are studied in Na1/2Bi1/2TiO3-5 %BaTiO3 single crystals lying near the morphotropic phase boundary. It is shown that, even in the absence of an electric field, dielectric and optical hysteresis associated with the coexistence of tetragonal and rhombohedral phases is observed in a wide temperature range, and the relative volume fractions of the two phases largely depend on temperature. It was found that at temperatures below the temperature of the mo
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48

Gobelko, I. E., A. V. Rozhkov, and D. N. Dresvyankin. "Perekhod metall-dielektrik i drugie elektronnye svoystva dvukhsloynogo AV-grafena na ferromagnitnoy podlozhke." Письма в Журнал экспериментальной и теоретической физики 118, no. 9-10 (11) (2023): 689–96. http://dx.doi.org/10.31857/s1234567823210103.

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Using a simple theoretical model, AB-stacked bilayer graphene deposited on a ferromagnetic insulating substrate is studied. In addition to the exchange Zeeman field induced by the substrate, the model allows one to take into account the effective external electric field perpendicular to the graphene sample plane (such field arises due to the contact with the substrate and can also be induced by applying a gate voltage). It has been demonstrated that AB-stacked graphene in zero electric field is in a metallic state. As the field increases, a transition to the insulating phase occurs. The spectr
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49

Gobelko, I. E., A. V. Rozhkov, and D. N. Dresvyankin. "Metal–Insulator Transition and Other Electronic Properties of AB-Stacked Bilayer Graphene Deposited on a Ferromagnetic Substrate." JETP Letters 118, no. 9 (2023): 676–83. http://dx.doi.org/10.1134/s0021364023603068.

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Using a simple theoretical model, AB-stacked bilayer graphene deposited on a ferromagnetic insulating substrate is studied. In addition to the exchange Zeeman field induced by the substrate, the model allows one to take into account the effective external electric field perpendicular to the graphene sample plane (such field arises due to the contact with the substrate and can also be induced by applying a gate voltage). It has been demonstrated that AB-stacked graphene in zero electric field is in a metallic state. As the field increases, a transition to the insulating phase occurs. The spectr
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50

Bai, Gang, Xueshi Qin, Qiyun Xie, and Cunfa Gao. "Electric-field-induced phase transition and electrocaloric effect in PZT near morphotropic phase boundary." Physica B: Condensed Matter 560 (May 2019): 208–14. http://dx.doi.org/10.1016/j.physb.2019.02.030.

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