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Journal articles on the topic 'Ferroelastic'

Author: Grafiati

Published: 4 June 2021

Last updated: 27 January 2023

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1

Skaliukh, Alexander. "Modeling of a hysteretic deformation response in polycrystalline ferroelastics." EPJ Web of Conferences 221 (2019): 01045. http://dx.doi.org/10.1051/epjconf/201922101045.

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You In the absence of an electric field a mathematical model describing the ferroelastic response of complete ferroelectrics ferroelastics on action of mechanical stresses is proposed. The modeling is based on the concept of a “ferroelastic” element, similar to the theory of plasticity where used the Saint-Venant element of “dry friction”. The constitutive relations for elastic and residual strains are constructed. The dependence of elastic compliance on the main values of the tensor of residual strains is established. For residual strains, the constitutive relations are obtained in differentials. The obtained constitutive equations can be used in finite element analysis of irreversible processes of deformation of polycrystalline ferroelastics. A number of numerical experiments were performed, which showed good agreement with the experimental data.

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2

Ding, Xinkai, and Gaoyang Gou. "Two-dimensional ferroelasticity and ferroelastic strain controllable anisotropic transport properties in CuTe monolayer." Nanoscale 13, no. 45 (2021): 19012–22. http://dx.doi.org/10.1039/d1nr03689k.

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Based on the transverse thermoelectric effect and the domain-wall motion assisted ferroelastic switching, ferroelastic strain controllable transport properties can be achieved in two-dimensional ferroelastic CuTe monolayers.

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3

Salje, Ekhard K. H. "Ferroelastic Materials." Annual Review of Materials Research 42, no. 1 (August 4, 2012): 265–83. http://dx.doi.org/10.1146/annurev-matsci-070511-155022.

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4

Muramatsu, Mayu, Tatsuya Kawada, and K. Terada. "A Simulation of Ferroelastic Phase Formation by Using Phase Field Model." Key Engineering Materials 725 (December 2016): 208–13. http://dx.doi.org/10.4028/www.scientific.net/kem.725.208.

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In order to incorporate the mechanical behavior of ferroelastic phase into the stress analysis of solid oxide fuel cell in consideration of elastic, creep, thermal and reduction strains, we propose a mathematical model to predict the formation of ferroelastic phases in crystal grains of La0.6Sr0.4Co0.2Fe0.8O3-δ. The phase field model equipped with the elastic energy is introduced to realize the morphology formation of ferroelastic phases in a crystal grain. By the use of the developed mathematical model, some numerical examples are performed to reproduce the deformation-induced nucleation and growth of ferroelastic phases of La0.6Sr0.4Co0.2Fe0.8O3-δ.

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5

Рогинский, Е. М., А. С. Крылов, and Ю. Ф. Марков. "Эффекты фазового перехода, индуцированные давлением, в модельных сегнетоэластиках Hg-=SUB=-2-=/SUB=-Br-=SUB=-2-=/SUB=-." Письма в журнал технической физики 44, no. 17 (2018): 3. http://dx.doi.org/10.21883/pjtf.2018.17.46564.17346.

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AbstractRaman spectra of model improper ferroelastics (Hg_2Br_2 crystals) have been analyzed in a wide range of hydrostatic pressures. The baric dependences of the phonon frequencies are obtained. The revealing and anomalous behavior of the soft mode, which is genetically related to the acoustic phonon (ТА_1) at the Brillouin zone boundary (point X ) of the tetragonal phase, are most interesting. The buildup of the second acoustic phonon (ТА_2) from the same point has also been found in the ferroelastic-phase spectra, and its baric behavior has been investigated. The splitting of doubly degenerate phonons of the E _g symmetry has been revealed at fairly high pressures and explained.

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6

Zhao, Meng-Meng, Lin Zhou, Ping-Ping Shi, Xuan Zheng, Xiao-Gang Chen, Ji-Xing Gao, Fu-Juan Geng, Qiong Ye, and Da-Wei Fu. "Halogen substitution effects on optical and electrical properties in 3D molecular perovskites." Chemical Communications 54, no. 94 (2018): 13275–78. http://dx.doi.org/10.1039/c8cc07052k.

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7

Xu, Xilong, Yandong Ma, Baibiao Huang, and Ying Dai. "Two-dimensional ferroelastic semiconductors in single-layer indium oxygen halide InOY (Y = Cl/Br)." Physical Chemistry Chemical Physics 21, no. 14 (2019): 7440–46. http://dx.doi.org/10.1039/c9cp00011a.

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8

Alikin, Denis, Anton Turygin, Andrei Ushakov, Mikhail Kosobokov, Yurij Alikin, Qingyuan Hu, Xin Liu, Zhuo Xu, Xiaoyong Wei, and Vladimir Shur. "Competition between Ferroelectric and Ferroelastic Domain Wall Dynamics during Local Switching in Rhombohedral PMN-PT Single Crystals." Nanomaterials 12, no. 21 (November 6, 2022): 3912. http://dx.doi.org/10.3390/nano12213912.

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The possibility to control the charge, type, and density of domain walls allows properties of ferroelectric materials to be selectively enhanced or reduced. In ferroelectric–ferroelastic materials, two types of domain walls are possible: pure ferroelectric and ferroelastic–ferroelectric. In this paper, we demonstrated a strategy to control the selective ferroelectric or ferroelastic domain wall formation in the (111) single-domain rhombohedral PMN-PT single crystals at the nanoscale by varying the relative humidity level in a scanning probe microscopy chamber. The solution of the corresponding coupled electro-mechanical boundary problem allows explaining observed competition between ferroelastic and ferroelectric domain growth. The reduction in the ferroelastic domain density during local switching at elevated humidity has been attributed to changes in the electric field spatial distribution and screening effectiveness. The established mechanism is important because it reveals a kinetic nature of the final domain patterns in multiaxial materials and thus provides a general pathway to create desirable domain structure in ferroelectric materials for applications in piezoelectric and optical devices.

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9

Meng, Xin, Zhi-Bo Liu, Ke Xu, Lei He, Yu-Zhen Wang, Ping-Ping Shi, and Qiong Ye. "Metal regulated organic–inorganic hybrid ferroelastic materials: [(CH₃)₃CN(CH₃)₂CH₂F]₂[MBr₄] (M = Cd and Zn)." Inorganic Chemistry Frontiers 9, no. 8 (2022): 1603–8. http://dx.doi.org/10.1039/d1qi01533h.

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Two organic–inorganic hybrid compounds [(CH3)3CN(CH3)2CH2F]2[MBr4] (M = Cd and Zn) undergo ferroelastic phase transitions. The substitution of metal center Cd with Zn of inorganic anions regulate the ferroelastic phase transitions.

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10

Wadhawan, V. K. "Ferroelastic Phase Transitions." Materials Science Forum 3 (January 1985): 91–109. http://dx.doi.org/10.4028/www.scientific.net/msf.3.91.

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11

Saint-Grégoire, P. "Ferroelastic Incommensurate Phases." Key Engineering Materials 101-102 (March 1995): 237–84. http://dx.doi.org/10.4028/www.scientific.net/kem.101-102.237.

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12

D'yakov, Vladimir A., Vladimir I. Pryalkin, and Alexeil Aleksandrovski. "New ferroelastic: LiNaCO3." Ferroelectrics Letters Section 19, no. 5-6 (September 1995): 163–69. http://dx.doi.org/10.1080/07315179508204718.

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13

Dec, J. "Paraelastic—ferroelastic interfaces." Phase Transitions 45, no. 1 (November 1993): 35–58. http://dx.doi.org/10.1080/01411599308203517.

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14

Jiménez, R., A. Castro, and B. Jiménez. "Evidence of ferroelastic–ferroelastic phase transition in BiMoxW1−xO6 compounds." Applied Physics Letters 83, no. 16 (October 20, 2003): 3350–52. http://dx.doi.org/10.1063/1.1613801.

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15

Ren, Xiaobing, Yu Wang, Kazuhiro Otsuka, Pol Lloveras, Teresa Castán, Marcel Porta, Antoni Planes, and Avadh Saxena. "Ferroelastic Nanostructures and Nanoscale Transitions: Ferroics with Point Defects." MRS Bulletin 34, no. 11 (November 2009): 838–46. http://dx.doi.org/10.1557/mrs2009.234.

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AbstractFor decades, a kind of nanoscale microstructure, known as the premartensitic “tweed structure” or “mottled structure,” has been widely observed in various martensitic or ferroelastic materials prior to their martensitic transformation, but its origin has remained obscure. Recently, a similar nanoscale microstructure also has been reported in highly doped ferroelastic systems, but it does not change into martensite; instead, it undergoes a nanoscale freezing transition—“strain glass” transition—and is frozen into a nanodomained strain glass state. This article provides a concise review of the recent experimental and modeling/simulation effort that is leading to a unified understanding of both premartensitic tweed and strain glass. The discussion shows that the premartensitic tweed or strain glass is characterized by nano-sized quasistatic ferroelastic domains caused by the existence of random point defects or dopants in ferroelastic systems. The mechanisms behind the point-defect-induced nanostructures and glass phenomena will be reviewed, and their significance in ferroic functional materials will be discussed.

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16

Arnauda, Barbara, Ali Akbari-Fakhrabadi, Nina Orlovskaya, Viviana Meruane, and Wakako Araki. "Room Temperature Ferroelastic Creep Behavior of Porous (La0.6Sr0.4)0.95Co0.2Fe0.8O3-δ." Processes 8, no. 11 (October 24, 2020): 1346. http://dx.doi.org/10.3390/pr8111346.

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The time-dependent deformation of porous (La0.6Sr0.4)0.95Co0.2Fe0.8O3-δ (LSCF) under constant uniaxial compressive stress at room temperature has been studied. Both axial and lateral stress–strain deformation curves clearly show the non-linear ferroelastic behavior of LSCF perovskite during compression. The ferroelastic characteristics of deformation curves such as coercive stress and apparent loading moduli decrease when the porosity of the samples increases. Ferroelastic creep deformations at applied stresses of 25 and 50 MPa demonstrate that stress and porosity are influencing factors on creep deformation, which increases with increasing stress and porosity. A negative creep or axial expansion and lateral contraction were observed in the sample with 35% porosity under 50-MPa constant compression stress.

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17

FIL, V. D., G. A. ZVYAGINA, S. V. ZHERLITSYN, I. M. VITEBSKY, V. L. SOBOLEV, S. N. BARILO, and D. I. ZHIGUNOV. "ACOUSTIC PROPERTIES OF Nd2CuO4 AT LOW TEMPERATURES." Modern Physics Letters B 05, no. 20 (August 30, 1991): 1367–75. http://dx.doi.org/10.1142/s0217984991001672.

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Acoustic properties anomalies near the points of phase transition in the magnetic subsystem of Nd 2 CuO 4 have been studied. A spontaneous ferroelastic phase transition at T = 5 K and magnetic field induced ferroelastic phase transition (PT) associated with continuous spin reorientations at T < 0.5 K have been found. The exchange nature of magnetoelastic coupling is suggested.

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18

Voloshinovskii, A., S. Myagkota, and R. Levitskii. "Luminescence of Ferroelastic CsPbCl3Nanocrystals." Ferroelectrics 317, no. 1 (July 2005): 119–23. http://dx.doi.org/10.1080/00150190590963570.

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19

Vlokh, R. O., and V. Y. Slivka. "Enantiomorphism of ferroelastic domains." Ferroelectrics 98, no. 1 (October 1989): 167–69. http://dx.doi.org/10.1080/00150198908217580.

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20

Matsuo, Yasumitsu, Junko Hatori, Katsumi Irokawa, Masaru Komukae, Toshio Osaka, and Yasuharu Makita. "Ferroelastic Phase Transition inTl2SeO4." Journal of the Physical Society of Japan 65, no. 12 (December 15, 1996): 3931–34. http://dx.doi.org/10.1143/jpsj.65.3931.

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21

Bravic, G., R. Von der Mühll, and J. Ravez. "Ferroelastic phase of Pb5Al3F19." Acta Crystallographica Section A Foundations of Crystallography 56, s1 (August 25, 2000): s386. http://dx.doi.org/10.1107/s0108767300028075.

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22

Seki, Tomohiro, Chi Feng, Kentaro Kashiyama, Shunichi Sakamoto, Yuichi Takasaki, Toshiyuki Sasaki, Satoshi Takamizawa, and Hajime Ito. "Photoluminescent Ferroelastic Molecular Crystals." Angewandte Chemie 132, no. 23 (March 24, 2020): 8924–28. http://dx.doi.org/10.1002/ange.201914610.

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23

Seki, Tomohiro, Chi Feng, Kentaro Kashiyama, Shunichi Sakamoto, Yuichi Takasaki, Toshiyuki Sasaki, Satoshi Takamizawa, and Hajime Ito. "Photoluminescent Ferroelastic Molecular Crystals." Angewandte Chemie International Edition 59, no. 23 (March 24, 2020): 8839–43. http://dx.doi.org/10.1002/anie.201914610.

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24

Qu, Xue Xuan, Hua Xia, and Xin-Kui Zhang. "Ferroelastic Domains in PrLaP5O14." Physica Status Solidi (a) 126, no. 1 (July 16, 1991): 125–28. http://dx.doi.org/10.1002/pssa.2211260113.

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25

Janovec, V., L. Richterov Aacute;, and D. B. Litvin. "Non-ferroelastic twin laws and distinction of domains in non-ferroelastic phases." Ferroelectrics 140, no. 1 (February 1993): 95–100. http://dx.doi.org/10.1080/00150199308008269.

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26

Ribet, M., S. Léon, F. Lefaucheux, and M. C. Robert. "Study of ferroelastic domains in HTMA crystals at the ferroelectric–ferroelastic transition." Journal of Applied Crystallography 23, no. 4 (August 1, 1990): 277–81. http://dx.doi.org/10.1107/s0021889890002709.

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27

Gorfman, Semën, David Spirito, Guanjie Zhang, Carsten Detlefs, and Nan Zhang. "Identification of a coherent twin relationship from high-resolution reciprocal-space maps." Acta Crystallographica Section A Foundations and Advances 78, no. 3 (April 28, 2022): 158–71. http://dx.doi.org/10.1107/s2053273322002534.

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Twinning is a common crystallographic phenomenon which is related to the formation and coexistence of several orientation variants of the same crystal structure. It may occur during symmetry-lowering phase transitions or during the crystal growth itself. Once formed, twin domains play an important role in defining physical properties: for example, they underpin the giant piezoelectric effect in ferroelectrics, superelasticity in ferroelastics and the shape-memory effect in martensitic alloys. Regrettably, there is still a lack of experimental methods for the characterization of twin domain patterns. Here, a theoretical framework and algorithm are presented for the recognition of ferroelastic domains, as well as the identification of the coherent twin relationship using high-resolution reciprocal-space mapping of X-ray diffraction intensity around split Bragg peaks. Specifically, the geometrical theory of twinned ferroelastic crystals [Fousek & Janovec (1969). J. Appl. Phys. 40, 135–142] is adapted for the analysis of the X-ray diffraction patterns. The necessary equations are derived and an algorithm is outlined for the calculation of the separation between the Bragg peaks, diffracted from possible coherent twin domains, connected to one another via a mismatch-free interface. It is demonstrated that such separation is always perpendicular to the planar interface between mechanically matched domains. For illustration purposes, the analysis is presented of the separation between the peaks diffracted from tetragonal and rhombohedral domains in the high-resolution reciprocal-space maps of BaTiO3 and PbZr1−x Ti x O3 crystals. The demonstrated method can be used to analyse the response of multi-domain patterns to external perturbations such as electric field, change of temperature or pressure.

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28

Harrison, R. J., S. A. T. Redfern, and U. Bismayer. "Seismic-frequency attenuation at first-order phase transitions: dynamical mechanical analysis of pure and Ca-doped lead orthophosphate." Mineralogical Magazine 68, no. 6 (December 2004): 839–52. http://dx.doi.org/10.1180/0026461046860226.

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AbstractThe low-frequency mechanical properties of pure and Ca-doped lead orthophosphate, (Pb1–xCax)3(PO4)2, have been studied using simultaneous dynamical mechanical analysis, X-ray diffraction (XRD), and optical video microscopy in the vicinity of the first-order ferroelastic phase transition. Both samples show mechanical softening at T > Tc, which is attributed to the presence of dynamic short-range order and microdomains. Stress-induced nucleation of the low-temperature ferroelastic phase within the hightemperature paraelastic phase was observed directly via optical microscopy at T ≈ Tc. Phase coexistence is associated with rapid mechanical softening and a peak in attenuation, P1, that varies systematically with heating rate and measuring frequency. A second peak, P2, occurs ≈3–5°C below Tc, accompanied by a rapid drop in the rate of mechanical softening. This is attributed to the change in mode of anelastic response from the displacement of the paraelastic/ferroelastic phase interface to the displacement of domain walls within the ferroelastic phase. Both the advancement/retraction of needles (W walls) and wall translation/rotation (W′ walls) modes of anelastic response were identified by optical microscopy and XRD. A third peak, P3, occurring ≈ 15°C below Tc, is attributed to the freezing-out of local flip disorder within the coarse ferroelastic domains. A fourth peak, P4, occurs at a temperature determined by the amplitude of the dynamic force. This peak is attributed to the crossover between the saturation (high temperature) and the superelastic(low temperature) regimes. Both samples display large superelastic softening due to domain wall sliding in the ferroelastic phase. Softening factors of 20 and 5 are observed in the pure and doped samples, respectively, suggesting that there is a significant increase in the intrinsic elastic constants (and hence the restoring force on a displaced domain wall) with increasing Ca content. No evidence for domain freezing was observed down to −150°C in either sample, although a pronounced peak in attenuation, P5, at T ≈ −100°C is tentatively attributed to the interaction between domain walls and lattice defects.Both samples show similar high values of attenuation within the domain-wall sliding regime. It is concluded that the magnitude of attenuation for ferroelastic materials in this regime is determined by the intrinsic energy dissipation caused by the wall-phonon interaction, and not by the presence of lattice defects. This will have a large impact on attempts to predict the effect of domain walls on seismic properties of mantle minerals at high temperature and pressure.

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29

Song, Hongzhang, Yongxiang Li, Kunyu Zhao, Huarong Zeng, Guorong Li, and Qingrui Yin. "The scanning electron acoustic microscopy investigation on ferroic materials under local stress." Journal of Materials Research 24, no. 7 (July 2009): 2173–78. http://dx.doi.org/10.1557/jmr.2009.0269.

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In this paper, the responses in the microregion of three ferroic-type materials, such as ferroelectric single crystals (PMN-PT and BaTiO3), ferromagnetic alloy (Fe81Ga19), and ferroelastic alloy (Ni53Mn24Ga23), to local stress induced by Vickers indentations were studied using scanning electron-acoustic microscopy (SEAM), a powerful technique for nondestructive investigation of the microstructure of materials. The responses of ferroelectric domains, magnetic domains, and ferroelastic domains to local stress were successfully observed. These responses possess three major features including the plastic deformation underneath the indenter, the extension of microcracks induced by indentation, and the formation of new lamellar domains within the matrix domain structure. In addition, by using the unique ability of SEAM to image layer by layer, the distributions of residual stress at different depths were obtained. The generation mechanisms of the electron acoustic signals of ferroelectric domains, magnetic domains, and ferroelastic domains are discussed.

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30

Ovsyuk, Nikolay N., and Sergei V. Goryainov. "Role of internal pressure in a ferroelastic phase transition." European Journal of Mineralogy 17, no. 2 (April 29, 2005): 215–22. http://dx.doi.org/10.1127/0935-1221/2005/0017-0215.

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31

Rok, M., G. Bator, B. Zarychta, B. Dziuk, J. Repeć, W. Medycki, M. Zamponi, G. Usevičius, M. Šimėnas, and J. Banys. "Isostructural phase transition, quasielastic neutron scattering and magnetic resonance studies of a bistable dielectric ion-pair crystal [(CH3)2NH2]2KCr(CN)6." Dalton Transactions 48, no. 13 (2019): 4190–202. http://dx.doi.org/10.1039/c8dt05082a.

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32

McGuinn, M. D., and S. A. T. Redfern. "Ferroelastic phase transition in SrAl2Si2O8 feldspar at elevated pressure." Mineralogical Magazine 58, no. 390 (March 1994): 21–26. http://dx.doi.org/10.1180/minmag.1994.058.390.02.

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AbstractSynthetic end-member strontium feldspar (SrAl2Si2O8) has been studied in a diamond-anvil cell at elevated pressures up to 10.3 GPa using energy-dispersive X-ray powder diffraction. Cell parameters have been refined between ambient pressure and 6 GPa. SrAl2Si2O8 undergoes a ferroelastic phase transition from the ambient pressure monoclinic space group I2/c to the high-pressure triclinic space group I at 3.2 ± 0.4 GPa. The transition appears to be first-order and the ferroelastic and co-elastic components of the spontaneous strain tensor have been calculated.

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33

Zhang, Ting, Yandong Ma, Lin Yu, Baibiao Huang, and Ying Dai. "Direction-control of anisotropic electronic behaviors via ferroelasticity in two-dimensional α-MPI (M = Zr, Hf)." Materials Horizons 6, no. 9 (2019): 1930–37. http://dx.doi.org/10.1039/c9mh00633h.

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34

Ma, An-ning, Sheng-shi Li, Shu-feng Zhang, Chang-wen Zhang, Wei-xiao Ji, Ping Li, and Pei-ji Wang. "Discovery of a ferroelastic topological insulator in a two-dimensional tetragonal lattice." Physical Chemistry Chemical Physics 21, no. 9 (2019): 5165–69. http://dx.doi.org/10.1039/c9cp00272c.

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35

Meng, Qian-Ru, Wei-Jian Xu, Wang-Hua Hu, Hui Ye, Xiao-Xian Chen, Wei Yuan, Wei-Xiong Zhang, and Xiao-Ming Chen. "An unprecedented hexagonal double perovskite organic–inorganic hybrid ferroelastic material: (piperidinium)2[KBiCl6]." Chemical Communications 57, no. 51 (2021): 6292–95. http://dx.doi.org/10.1039/d1cc02085d.

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36

Hu, Minglang, Shaowen Xu, Chao Liu, Guodong Zhao, Jiahui Yu, and Wei Ren. "First-principles prediction of a room-temperature ferromagnetic and ferroelastic 2D multiferroic MnNX (X = F, Cl, Br, and I)." Nanoscale 12, no. 47 (2020): 24237–43. http://dx.doi.org/10.1039/d0nr06268e.

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37

Lan, Qingwen, and Changpeng Chen. "Two-dimensional ferroelasticity and negative Poisson's ratios in monolayer YbX (X = S, Se, Te)." Physical Chemistry Chemical Physics 24, no. 4 (2022): 2203–8. http://dx.doi.org/10.1039/d1cp05080j.

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38

Feng, Xukun, Xikui Ma, Lei Sun, Jian Liu, and Mingwen Zhao. "Tunable ferroelectricity and antiferromagnetism via ferroelastic switching in an FeOOH monolayer." Journal of Materials Chemistry C 8, no. 40 (2020): 13982–89. http://dx.doi.org/10.1039/d0tc04400h.

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39

Salje, Ekhard, and Xiangdong Ding. "Ferroelastic Domain Boundary-Based Multiferroicity." Crystals 6, no. 12 (December 9, 2016): 163. http://dx.doi.org/10.3390/cryst6120163.

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40

Kukushkin, S. A. "Switching Kinetics of Ferroelastic Ferroelectrics." Physics of the Solid State 44, no. 12 (December 2002): 2298. http://dx.doi.org/10.1134/1.1529928.

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41

Mielcarek, S., B. Mroz, A. Trzaskowska, Z. Tylcynski, and T. Andrews. "Surface Phonons in Ferroelastic Crystals." Ferroelectrics 267, no. 1 (January 2002): 391–96. http://dx.doi.org/10.1080/00150190210995.

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42

Redfern, S. A. T. "Ferroelastic phase transition in CaTiO3perovskite." Acta Crystallographica Section A Foundations of Crystallography 52, a1 (August 8, 1996): C436. http://dx.doi.org/10.1107/s0108767396082086.

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43

Dudnik, E. F., and S. V. Akimov. "Optical Activity in Ferroelastic Crystals." Ferroelectrics 397, no. 1 (June 21, 2010): 54–64. http://dx.doi.org/10.1080/00150193.2010.484718.

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44

Sastry, P. U. M., and A. Sequeira. "Structural transformations in ferroelastic TINO3." Philosophical Magazine B 75, no. 5 (May 1997): 659–67. http://dx.doi.org/10.1080/13642819708202347.

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45

Lookman, T., S. R. Shenoy, K. O. Rasmussen, A. Saxena, and A. R. Bishop. "On dynamics of ferroelastic transitions." Journal de Physique IV (Proceedings) 112 (October 2003): 195–99. http://dx.doi.org/10.1051/jp4:2003864.

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46

Melnikova, S. V., L. A. Shabanova, A. I. Zaitsev, S. A. Parshikov, O. A. Ageev, and K. S. Aleksandrov. "Ferroelastic phase transition in Cs3Bi2I9crystal." Ferroelectrics Letters Section 20, no. 5-6 (March 1996): 163–67. http://dx.doi.org/10.1080/07315179608204735.

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47

Flerov, I. N., A. F. Bovina, V. N. Voronov, M. V. Gorev, S. V. Misjul, S. V. Melnikova, and L. A. Shabanova. "Ferroelastic phase transitions in elpasolites." Ferroelectrics 64, no. 1 (June 1985): 25–27. http://dx.doi.org/10.1080/00150198508018688.

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48

Zhou, Guo-Xiang, Xue Bai, Ya-jiao Wei, and Mei-Ling Guo. "Ferroelastic phase transition of LiCsSO4crystal." Ferroelectrics 502, no. 1 (September 25, 2016): 221–30. http://dx.doi.org/10.1080/00150193.2016.1236236.

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Matuso, Atsushi, Katsumi Irokawa, Masaru Komukae, Toshio Osaka, and Yasuharu Makita. "Structural Study of Ferroelastic TlH2PO4." Journal of the Physical Society of Japan 63, no. 4 (April 15, 1994): 1626–27. http://dx.doi.org/10.1143/jpsj.63.1626.

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Kim, C. H., J. W. Jang, S. Y. Cho, I. T. Kim, and K. S. Hong. "Ferroelastic twins in LaAlO3 polycrystals." Physica B: Condensed Matter 262, no. 3-4 (April 1999): 438–43. http://dx.doi.org/10.1016/s0921-4526(98)00848-5.

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