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Journal articles on the topic 'Structural phase'

Author: Grafiati

Published: 5 June 2025

Last updated: 24 June 2025

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1

Aftandiliants, Ye G. "Modelling of structure forming in structural steels." Naukovij žurnal «Tehnìka ta energetika» 11, no. 4 (2020): 13–22. http://dx.doi.org/10.31548/machenergy2020.04.013.

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The study showed that the influence of alloying elements on the secondary structure formation of the steels containing from 0.19 to 0.37 wt. % carbon; 0.82-1.82 silicon; 0.63-3.03 manganese; 1.01-3.09 chromium; 0.005-0.031 nitrogen; up to 0.25 wt.% vanadium and austenite grain size is determined by their change in the content of vanadium nitride phase in austenite, its alloying and overheating above tac3, and the dispersion of ferrite-pearlite, martensitic and bainitic structures is determined by austenite grain size and thermal kinetic parameters of phase transformations. Analytical dependencies are defined that describe the experimental data with a probability of 95% and an error of 10% to 18%. An analysis results of studying the structure formation of structural steel during tempering after quenching show that the dispersion and uniformity of the distribution of carbide and nitride phases in ferrite is controlled at complete austenite homogenization by diffusion mobility and the solubility limit of carbon and nitrogen in ferrite, and secondary phase quantity in case of the secondary phase presence in austenite more than 0.04 wt. %. Equations was obtained which, with a probability of 95% and an error of 0.7 to 2.6%, describe the real process.

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2

Knight, Kevin S., William G. Marshall, C. Michael B. Henderson, and Andrew A. Chamberlain. "Equation of state and a high-pressure structural phase transition in the gillespite-structured phase Ba0.5Sr0.5CuSi4O10." European Journal of Mineralogy 25, no. 6 (2014): 909–17. http://dx.doi.org/10.1127/0935-1221/2013/0025-2333.

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3

Aftandiliants, Ye G. "Modelling of phase transformations in structural steels." Naukovij žurnal «Tehnìka ta energetika» 11, no. 2 (2020): 15–20. http://dx.doi.org/10.31548/machenergy2020.02.015.

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4

A. Cowley, R., and S. M. Shapiro. "Structural Phase Transitions." Journal of the Physical Society of Japan 75, no. 11 (2006): 111001. http://dx.doi.org/10.1143/jpsj.75.111001.

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5

Kubicki, Maciej. "Structural Aspects of Phase Transitions." Solid State Phenomena 112 (May 2006): 1–20. http://dx.doi.org/10.4028/www.scientific.net/ssp.112.1.

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There are two kinds of structural transformations in the crystalline solid state: solid state reactions, in which the product chemically different from the starting material can be isolated, and polymorphic transitions, when the phases have different organization of identical molecules in the crystal structures. As a consequence, the starting and the final phases of a solid state reaction differ in the melt and vapor, while different polymorphic modifications are identical in melt or gas phase. Some examples of the different phase transitions in the solid state are described in detail: the π-molecular complexes, the hydrogen-bond transformations and the reversible single crystal - twin transition.

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6

Yurov, V. M., S. A. Guchenko, V. Ch Laurinas, and O. N. Zavatskaya. "Structural phase transition in surface layer of metals." Bulletin of the Karaganda University. "Physics" Series 93, no. 1 (2019): 50–60. http://dx.doi.org/10.31489/2019ph1/50-60.

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7

KAR, MANORANJAN, N. RAMA KRISHNAN, INDRAJIT TALUKDAR, and K. ACHARYYA. "STRUCTURAL TRANSITION OF NANOCRYSTALLINE TiO2." International Journal of Nanoscience 10, no. 01n02 (2011): 59–63. http://dx.doi.org/10.1142/s0219581x11007648.

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Nanocrystalline TiO 2 sample was prepared by high-energy ball mill method. A known quantity of anatase phase- TiO 2 was milled for 83 h in air. The samples were collected at intervals of 5 h of milling. The XRD patterns were recorded for all the samples. The crystal structure changed from anatase phase for bulk material to rutile-rich phase for nanocrystalline material. Nanocrystalline TiO 2, which is a mixture of anatase, rutile, and srilankite phase, was prepared by milling for 60 h. The XRD pattern of unmilled anatase phase of TiO 2 could be refined with I41/amd space group. The crystallite size of the TiO 2 was found to decrease with milling time upto 50 h and then the size of rutile phase increases while the sizes of anatase and srilankite phases remain constant upto 60 h of milling. After 60 h, the sizes of all the phases remain constant. The average crystallite size for rutile phase is found to be 12 nm after 60 h of milling.

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8

Hou, Zhi Yao, Xiao Di Wang, Jun Wang, and Bin Zhu. "Structural Studies on Ceria-Carbonate Composite Electrolytes." Key Engineering Materials 368-372 (February 2008): 278–81. http://dx.doi.org/10.4028/www.scientific.net/kem.368-372.278.

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This paper studied structures of ceria-carbonate two-phase composites, with an emphasis on the interfacial structures and interactions between the two constituent phases of ceria and carbonate. The phase structure was analyzed by DSC, XRD and SEM. The IR measurements were carried out to identify the bonding situations and interfaces. Some new absorptions and wavenumber shifts of the bands appeared in IR spectra. There are strong indications of the interfacial phenomena exist in the two-phase composites through comparison between the two-phase composite with each individual constituent phases. The results opened a new interesting subject on the two-phase composite structures with significant importance for applications in advanced low temperature (300-600°C) SOFC.

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9

Weakley, T. J. R., E. R. Ylvisaker, R. J. Yager, et al. "Phase transitions in K2Cr2O7 and structural redeterminations of phase II." Acta Crystallographica Section B Structural Science 60, no. 6 (2004): 705–15. http://dx.doi.org/10.1107/s010876810402333x.

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Crystals of phase II K2Cr2O7, potassium dichromate, space group P\overline 1, grown from aqueous solution undergo a first-order transition to phase I, space group reportedly P21/n, at a phase-transition temperature, T PT, of 544 (2) K on first heating; the corresponding transition on cooling is at 502 (2) K. The endotherm on subsequent heatings occurs reproducibly at T PT = 531 (2) K. Mass loss between ca 531 and 544 K, identified as included water, is rapid and continues more slowly to higher temperatures for a total loss of ca 0.20%. The higher T PT on first heating is associated with the increasing pressure of superheated water occupying inclusion defects. The latent diagonal glide plane in phase II allows the structure of phase I to be inferred. The triclinic structure at 296 K has been independently redetermined. Normal probability analysis shows high consistency between the resulting and previous atomic coordinates, but with uncertainties reduced by a factor of ca 2. The earlier uncertainties are systematically underestimated by a comparable factor. The structure of phase IIb, space group A2/a on transposing axes, was determined at ca 300 K by Krivovichev et al. [Acta Cryst. (2000), C56, 629–630]. The first-order transition between phases I and II arises from the ca 60° relative rotation of terminal O atoms in each tetrahedron as the n glide plane is gained or lost. A transition between phases IIb and I, also of first order, is likely but not between phases II and IIb. An intermediate phase may exist between phases IIb and I.

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10

Tkachuk, O., Ya Matychak, I. Pohrelyuk, and V. Fedirko. "Diffusion of Nitrogen and Phase—Structural Transformations in Titanium." METALLOFIZIKA I NOVEISHIE TEKHNOLOGII 36, no. 8 (2016): 1079–89. http://dx.doi.org/10.15407/mfint.36.08.1079.

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11

Carpenter, Michael A., and Ekhard K. H. Salje. "Elastic anomalies in minerals due to structural phase transitions." European Journal of Mineralogy 10, no. 4 (1998): 693–812. http://dx.doi.org/10.1127/ejm/10/4/0693.

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12

Knight, Kevin S., and C. Michael B. Henderson. "Structural basis for the anomalous low-temperature thermal expansion behaviour of the gillespite-structured phase Ba0.5Sr0.5CuSi4O10." European Journal of Mineralogy 19, no. 2 (2007): 189–200. http://dx.doi.org/10.1127/0935-1221/2007/0019-1711.

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13

Zhao, Yusheng, Fuming Chu, Robert B. Von Dreele, and Qing Zhu. "Structural phase transitions of HfV2 at low temperatures." Acta Crystallographica Section B Structural Science 56, no. 4 (2000): 601–6. http://dx.doi.org/10.1107/s0108768100003633.

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We report a high-resolution synchrotron X-ray powder diffraction study on HfV2, hafnium divanadium, at low temperatures. In this work we show, for the first time, a complete sequence of structural phase transitions of HfV2 from cubic (Fd3m) to tetragonal (I41/amd) to orthorhombic (Imma) in succession as temperature decreases. Peak splitting and extra diffraction peaks owing to lattice distortion can be clearly distinguished for the low-symmetry phases. The atomic positions and lattice parameters were obtained by Rietveld refinement. The bond lengths and angles of the HfV2 crystal structure at the low-symmetry phases were correctly determined from the structure refinement. The face-centered cubic (Fd3m) unit cell (Z = 24) transforms to a body-centered tetragonal (I41/amd) phase with a 45° rotation relative to the cubic cell and with a reduced number of atoms (Z = 12) in the unit cell at a temperature of T = 112 K. The orthorhombic phase occurs at T = 102 K and it keeps the body-centered symmetry (Imma) and Z = 12 in the unit cell. The refinement results indicate that there may be a small amount of untransformed cubic phase left over in the lower symmetry phases. The abnormal thermal contraction of both tetragonal phase and orthorhombic phase marks the significance of structural change in HfV2.

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14

SUN, XIAO-XIAO, ZHI-RU REN, and DAO-GUANG WANG. "STRUCTURAL TRANSITIONS OF BiI3 UNDER PRESSURE." Modern Physics Letters B 26, no. 32 (2012): 1250217. http://dx.doi.org/10.1142/s021798491250217x.

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High pressure studies of BiI 3 at 0 K are performed using first-principles pseudopotential calculations within the framework of density functional theory. The calculations indicate that BiI 3 undergoes a structural transition from rhombohedral R-3 phase to monoclinic P2 1/c phase at 7 GPa which is accompanied by a 5.8% volume collapse. In addition, we find that P2 1/c phase prevails about 60 GPa range and transforms to cubic Fm-3m phase at 68 GPa, and finally takes the orthorhombic Pnma phase at high pressures up to 133 GPa. The structural and electronic properties of four competitive structures are also calculated. The analysis of density of states reveals that BiI 3 has semiconductor-metal transition at about 61 GPa, which also demonstrates the metallic nature of both Fm-3m and Pnma phases.

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15

Tomioka, Naotaka, Kiyoshi Fujino, Eiji Ito, Tomoo Katsura, Thomas Sharp, and Takumi Kato. "Microstructures and structural phase transition in (Mg,Fe)SiO3 majorite." European Journal of Mineralogy 14, no. 1 (2002): 7–14. http://dx.doi.org/10.1127/0935-1221/2002/0014-0007.

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16

Khare, Varsha, N. P. Lalla, R. S. Tiwari, and O. N. Srivastava. "On the new structural phases in Al65Cu20Cr15 quasicrystalline alloy." Journal of Materials Research 10, no. 8 (1995): 1905–12. http://dx.doi.org/10.1557/jmr.1995.1905.

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The quasicrystalline (qc) alloy Al65Cu20Cr15, unlike its Ru- and Fe-bearing counterparts like Al65Cu20Ru15 and Al65Cu20Fe15, is a metastable phase. This qc alloy has been shown to possess several structural variants and curious structural characteristics. We have investigated the qc alloy Al65Cu20Cr15 with special reference to the possible occurrence of new structural variants. TEM exploration of the as-quenched qc alloy has indeed revealed the existence of several new phases. These are (i) body-centered cubic (bcc) (a = 12.60 Å, disordered) and simple cubic (s.c.) (a = 12.60 Å, ordered), which are the 1/1 approximants of the primitive icosahedral phase (i phase); (ii) a twice order-induced modulated cubic phase (bcc, a = 25.20 Å) which has been shown to correspond to 1/1 approximant of the ordered i phase [i.e., face-centered icosahedral (FCI)]; and (iii) real crystalline bcc (a = 8.90 Å) and face-centered cubic (fcc) (a = 17.98 Å) phases possessing a specific orientation relationship with the icosahedral matrix phase. Tentative structural models showing the interrelationships between the bcc/fcc phases have been outlined.

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17

Kiełbus, Andrzej, and Tomasz Rzychoń. "Structural Stability of Mg–6Al–2Sr Magnesium Alloy." Solid State Phenomena 176 (June 2011): 75–82. http://dx.doi.org/10.4028/www.scientific.net/ssp.176.75.

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The Mg–6Al–2Sr magnesium alloy containing 6.15 at.% of aluminium, 2.1 at.% of strontium and 0.42 at.% of manganese was investigated at sand casting state performed at 700°C and after annealing treatment at 180°C, 250°C and 350°C during 500÷5000h with cooling in air. In the as-cast conditions the Mg–6Al–2Sr alloy consisted of α-Mg grains with intermetallic phases: (Al,Mg)4Sr, Al8Mn5 and Al3Mg13Sr. Annealing at 180°C resulted in the precipitation of the Mg17Al12 phase in the aluminium enriched area and the beginning of decomposition of the Al3Mg13Sr phase. Annealing at 250°C causes further decomposition of the Al3Mg13Sr phase while no precipitates of the Mg17Al12 phase could be observed. After exposure at 350°C the total decomposition of the Al3Mg13Sr phase into a mixture of the Al4Sr and α-Mg phases has been observed

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18

Jakubas, R., G. Bator, M. Foulon, J. Lefebvre, and J. Matuszewski. "Structural Phase Transitions in (n-C3H7NH3)2SbBr5." Zeitschrift für Naturforschung A 48, no. 3 (1993): 529–34. http://dx.doi.org/10.1515/zna-1993-0314.

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Abstract Dielectric, DSC, thermal expansion and preliminary X-ray diffraction studies on (n-C3H7NH3)- SbBr5 are reported. It was found that this crystal undergoes a complex sequence of phase transitions. On cooling: phase I → phase II at 188.7 K (continuous), II → III at 165 K (1st order, ΔS = 26.8 J/mol K), III → IV at 137 K (1st order, 1.6 J/mol K). On heating: IV → III at 154 K, III → II’ at 168 K, II’ → II at 177 K (1st order, 2.8 J/mol K), II → I at 189 K. All 1st order phase transitions are likely due to the motion of the n-C3H7NH3+cations. The dielectric dispersion studies between 100 Hz-1 MHz within the phases I and II indicate a fast reorientational motion of dipoles with τ < 10−7 S.

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19

Massarotti, V., M. Bini, and D. Capsoni. "Structural and Defect Study of LiMn2O4 Formation." Zeitschrift für Naturforschung A 51, no. 4 (1996): 267–76. http://dx.doi.org/10.1515/zna-1996-0406.

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Abstract The LiMn2O4 formation from MnO and Li2CO3 mixtures with lithium cationic fraction 0.31 <̲ x <̲ 0.40 was studied by structural profile refinement from X-ray data, thermal (TGA and DSC) measurements and scanning electron microscopy (SEM) observations. Quantitative phase analysis, structural and microstructural parameters and composition of the coexisting phases were obtained. Different behaviours were observed in the composition ranges 0.33 <̲ x <̲ 0.35 and x >̲ 0.37. In the former range only the stoichiometric spinel phase was obtained, in the latter, in addition to the Li2MnO3 compound, two spinel phases could be considered: I) LiMn2O4 stoichiometric spinel; II) Li1 + yMn2-yO4 (0.11 <̲ y <̲ 0.23), a non-stoichiometric phase whose small particle size resulted practically independent of the initial composition and annealing temperature. Such a conclusion was supported also by SEM observations. The relative abundance of phase II increased with increasing lithium content and with decreasing temperature.

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20

Jahn, I. R., H. Ritter, K. Schwab, and K. Knorr. "Structural phase sequence and modulated phases of (C3H7NH3)2CuBr4." Ferroelectrics 205, no. 1 (1998): 119–32. http://dx.doi.org/10.1080/00150199808228392.

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21

Vega, D., G. Polla, A. G. Leyva, et al. "Structural Phase Diagram of Ca1−xYxMnO3: Characterization of Phases." Journal of Solid State Chemistry 156, no. 2 (2001): 458–63. http://dx.doi.org/10.1006/jssc.2000.9023.

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22

Karpinsky, Dmitry V., Maxim V. Silibin, Siarhei I. Latushka, et al. "Structural and Magnetic Phase Transitions in BiFe1 − xMnxO3 Solid Solution Driven by Temperature." Nanomaterials 12, no. 9 (2022): 1565. http://dx.doi.org/10.3390/nano12091565.

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The crystal structure and magnetic state of the (1 − x)BiFeO3-(x)BiMnO3 solid solution has been analyzed by X-ray diffraction using lab-based and synchrotron radiation facilities, magnetization measurements, differential thermal analysis, and differential scanning calorimetry. Dopant concentration increases lead to the room-temperature structural transitions from the polar-active rhombohedral phase to the antipolar orthorhombic phase, and then to the monoclinic phase accompanied by the formation of two-phase regions consisting of the adjacent structural phases in the concentration ranges 0.25 < x1 < 0.30 and 0.50 ≤ x2 < 0.65, respectively. The accompanied changes in the magnetic structure refer to the magnetic transitions from the modulated antiferromagnetic structure to the non-colinear antiferromagnetic structure, and then to the orbitally ordered ferromagnetic structure. The compounds with a two-phase structural state at room temperature are characterized by irreversible temperature-driven structural transitions, which favor the stabilization of high-temperature structural phases. The magnetic structure of the compounds also exhibits an irreversible temperature-induced transition, resulting in an increase of the contribution from the magnetic phase associated with the high-temperature structural phase. The relationship between the structural parameters and the magnetic state of the compounds with a metastable structure is studied and discussed depending on the chemical composition and heating prehistory.

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23

Lavigne, Rob, Jean-Paul Noben, Kirsten Hertveldt та ін. "The structural proteome of Pseudomonas aeruginosa bacteriophage ϕKMV". Microbiology 152, № 2 (2006): 529–34. http://dx.doi.org/10.1099/mic.0.28431-0.

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The structural proteome of ϕKMV, a lytic bacteriophage infecting Pseudomonas aeruginosa, was analysed using two approaches. In one approach, structural proteins of the phage were fractionated by SDS-PAGE for identification by liquid chromatography-mass spectrometry (LC-MS). In a second approach, a whole-phage shotgun analysis (WSA) was applied. WSA uses trypsin digestion of whole phage particles, followed by reversed-phase HPLC and gas-phase fractionation of the complex peptide mixture prior to MS. The results yield a comprehensive view of structure-related proteins in ϕKMV and suggest subtle structural differences from phage T7.

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24

Aleksandrov, K. S., L. S. Emelyanova, S. V. Misyul, et al. "Structural Phase Transition in Rb2CdCl4." Japanese Journal of Applied Physics 24, S2 (1985): 399. http://dx.doi.org/10.7567/jjaps.24s2.399.

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25

ITOH, Kazuyuki. "Structural phase transitions of ferroelectrics." Nihon Kessho Gakkaishi 28, no. 4 (1986): 247–60. http://dx.doi.org/10.5940/jcrsj.28.247.

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26

Angel, R. J. "High-Pressure Structural Phase Transitions." Reviews in Mineralogy and Geochemistry 39, no. 1 (2000): 85–104. http://dx.doi.org/10.2138/rmg.2000.39.04.

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27

Mikhailova, D., D. Trots, H. Ehrenberg, and H. Fuess. "Structural phase transitions in Sr2ScReO6." Acta Crystallographica Section A Foundations of Crystallography 63, a1 (2007): s184. http://dx.doi.org/10.1107/s0108767307095840.

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28

Nakayama, Noriaki, Takanobu Itoyama, Keiko Fujiwara, Akihiko Nakatsuka, Masahiko Isobe, and Yutaka Ueda. "Structural Phase Transition of Li2MnSiO4." Transactions of the Materials Research Society of Japan 37, no. 3 (2012): 475–78. http://dx.doi.org/10.14723/tmrsj.37.475.

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29

Beige, H., M. Diestelhorst, R. Forster, J. Albers, and J. Petersson. "Chaos Near Structural Phase Transition." Zeitschrift für Naturforschung A 45, no. 8 (1990): 958–64. http://dx.doi.org/10.1515/zna-1990-0804.

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Abstract An experimental model of a Duffing oscillator is presented. It consists of a linear inductance, a resistance and a ferroelectric nonlinear capacitance. A computer controlled measuring system recorded quantitatively the phase portrait of this series-resonance circuit. The comparison of experimentally observed phase portraits with those calculated by a computer allows to check different assumptions about the nature of the nonlinear properties

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30

Froyen, Sverre, Su-Huai Wei, and Alex Zunger. "Epitaxy-induced structural phase transformations." Physical Review B 38, no. 14 (1988): 10124–27. http://dx.doi.org/10.1103/physrevb.38.10124.

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31

Kabirov, Yu V., B. S. Kul’buzhev, and M. F. Kupriyanov. "Structural phase transitions in CdTiO3." Physics of the Solid State 43, no. 10 (2001): 1968–71. http://dx.doi.org/10.1134/1.1410640.

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32

Beige, H., M. Diestelhorst, R. Forster, J. Albers, and H. E. Müser. "Chaos near structural phase transition." Ferroelectrics 104, no. 1 (1990): 355–60. http://dx.doi.org/10.1080/00150199008223839.

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33

Bechstedt, F., and K. Hübner. "Structural phase transition in SiOx." Journal of Non-Crystalline Solids 93, no. 1 (1987): 125–41. http://dx.doi.org/10.1016/s0022-3093(87)80033-9.

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34

Friese, Karen, and Yasushi Kanke. "Structural phase transitions in BaV6O11." Journal of Solid State Chemistry 179, no. 11 (2006): 3277–85. http://dx.doi.org/10.1016/j.jssc.2006.04.059.

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35

Ishizawa, Nobuo, Kenji Tateishi, Saki Kondo, and Tsuyoshi Suwa. "Structural Phase Transition of Gd3RuO7." Inorganic Chemistry 47, no. 2 (2008): 558–66. http://dx.doi.org/10.1021/ic701732d.

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36

Saines, Paul J., Brendan J. Kennedy, and Ronald I. Smith. "Structural phase transitions in BaPrO3." Materials Research Bulletin 44, no. 4 (2009): 874–79. http://dx.doi.org/10.1016/j.materresbull.2008.09.013.

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37

Vrtis, M. L., J. D. Jorgensen, and D. G. Hinks. "Structural phase transition in CeCu6." Physica B+C 136, no. 1-3 (1986): 489–92. http://dx.doi.org/10.1016/s0378-4363(86)80125-5.

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38

Koyama, Y., Y. Wakabayashi, and Y. Inoue. "Structural phase transitions in La1.885Sr0.115CuO4." Physica C: Superconductivity 235-240 (December 1994): 833–34. http://dx.doi.org/10.1016/0921-4534(94)91641-1.

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39

White, William B. "Defects and structural phase transitions." Materials Research Bulletin 25, no. 2 (1990): 265. http://dx.doi.org/10.1016/0025-5408(90)90054-6.

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40

Dorner, B. "Structural excitations and phase transformation." Physica B: Condensed Matter 180-181 (June 1992): 265–70. http://dx.doi.org/10.1016/0921-4526(92)90729-c.

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41

Yeung, W. "Magnetically induced structural phase transitions." Physica B+C 149, no. 1-3 (1988): 185–93. http://dx.doi.org/10.1016/0378-4363(88)90240-9.

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42

Kashida, S., and K. Yamamoto. "Structural phase transition in KHCO3." Journal of Solid State Chemistry 86, no. 2 (1990): 180–87. http://dx.doi.org/10.1016/0022-4596(90)90133-i.

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43

Wandner, Derk, Pascal Link, Oliver Heyer, et al. "Structural Phase Transitions in EuC2." Inorganic Chemistry 49, no. 1 (2010): 312–18. http://dx.doi.org/10.1021/ic901979v.

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44

Blochwitz, Stefan, Ronny Habel, Martin Diestelhorst, and Horst Beige. "Chaos at structural phase transitions." Ferroelectrics 183, no. 1 (1996): 95–104. http://dx.doi.org/10.1080/00150199608224095.

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45

Thompson, A. L., A. E. Goeta, C. C. Wilson, et al. "Structural phase transitions in CsInF4." Acta Crystallographica Section A Foundations of Crystallography 58, s1 (2002): c341. http://dx.doi.org/10.1107/s0108767302098604.

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46

Ishibashi, Yoshihiro, and Vladimir Dvo\(\check{\text{r}}\)ák. "Structural Phase Transitions in CH3NH3HgCl3." Journal of the Physical Society of Japan 58, no. 12 (1989): 4493–95. http://dx.doi.org/10.1143/jpsj.58.4493.

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47

Green, M. A., M. Kurmoo, P. Day, and K. Kikuchi. "Structural phase transformations in C70." Journal of the Chemical Society, Chemical Communications, no. 22 (1992): 1676. http://dx.doi.org/10.1039/c39920001676.

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48

Beige, H., M. Diestelhorst, R. Forster, J. Albers, and J. Petersson. "Chaos near Structural Phase Transition." Acta Physica Polonica A 81, no. 3 (1992): 413–18. http://dx.doi.org/10.12693/aphyspola.81.413.

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Singh, S., K. Aneesh, and R. K. Singh. "Structural phase transition in NdAs." Journal of Physics: Conference Series 215 (March 1, 2010): 012112. http://dx.doi.org/10.1088/1742-6596/215/1/012112.

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Christensen, N. E. "Structural phase stability ofB2andB32intermetallic compounds." Physical Review B 32, no. 1 (1985): 207–28. http://dx.doi.org/10.1103/physrevb.32.207.

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