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Journal articles on the topic 'Antiphase domains'

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Published: 4 June 2021

Last updated: 11 February 2022

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1

van Roermund, H. L. M., and J. M. Lardeaux. "Modification of antiphase domain sizes in omphacite by dislocation glide and creep mechanisms and its petrological consequences." Mineralogical Magazine 55, no. 380 (1991): 397–407. http://dx.doi.org/10.1180/minmag.1991.055.380.09.

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AbstractA T.E.M. study of omphacites from the western Italian Alps (Sesia Lanzo Zone and Monviso eclogites) has revealed a bimodal size distribution of antiphase domains: (a) 250–350 Å, (b) ≥ 2500 Å. In addition observed dislocation substructures and ‘large-scale’ antiphase domains are intimately interconnected.A model is presented that can explain modification of the antiphase domain sizes by the interplay of cooling/growth and dislocation glide and/or creep mechanisms. Subsequent coarsening of the modified antiphase domains is inferred to be the result of surface free-energy processes. The model clearly illustrates that only the ‘relatively undeformed’ areas containing the small-scale antiphase domains can be used for thermometric methods.

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2

ICHIMIYA, AYAHIKO, and YUSUKE OHNO. "STRUCTURAL ANALYSIS OF IMPERFECT CRYSTAL SURFACES BY REFLECTION HIGH-ENERGY ELECTRON DIFFRACTION: ANTIPHASE DOMAINS OF A ${\rm Si}(111)(\sqrt 3 \times\sqrt 3)$-Ag SURFACE." Surface Review and Letters 04, no. 05 (1997): 985–90. http://dx.doi.org/10.1142/s0218625x97001164.

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For dynamical calculations of reflection high-energy electron diffraction (RHEED) for imperfect crystal surfaces, a general formula of Fourier coefficients of crystal potential with domain structures is developed. Using the formula, RHEED intensity rocking curves are calculated for a [Formula: see text]-Ag surface with antiphase domains. We discuss effects of antiphase domains of surfaces in structure determinations by RHEED.

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3

Reiche, J. "Antiphase domains in Langmuir-Blodgett films." Thin Solid Films 284-285 (September 1996): 453–55. http://dx.doi.org/10.1016/s0040-6090(95)08364-2.

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4

KOIZUMI, Y., T. FUJITA, and Y. MINAMINO. "Anomalous growth of antiphase domains in Ti3Al." Scripta Materialia 60, no. 3 (2009): 144–47. http://dx.doi.org/10.1016/j.scriptamat.2008.09.017.

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5

Koizumi, Yuichiro, and Yoritoshi Minamino. "Anomalous Growth of Antiphase Domains in Ti3Al." Materia Japan 48, no. 12 (2009): 594. http://dx.doi.org/10.2320/materia.48.594.

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6

Feng, C. R., D. J. Michel, and C. R. Crow. "Antiphase domains and {011} twins in TiAl." Philosophical Magazine Letters 61, no. 3 (1990): 95–100. http://dx.doi.org/10.1080/09500839008206486.

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7

Nordquist, P. E. R., M. L. Gipe, G. Kelner, P. H. Klein та R. J. Gorman. "Antiphase domains and etching of β-SiC". Materials Letters 9, № 1 (1989): 17–20. http://dx.doi.org/10.1016/0167-577x(89)90123-7.

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8

Lu, Ping, Jiadong Zhou, Xinling Liu, et al. "Characterization of phase-transition-induced micro-domain structures in vanadium dioxide." Journal of Applied Crystallography 47, no. 2 (2014): 732–38. http://dx.doi.org/10.1107/s1600576714002854.

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The displacive structural phase transition of vanadium dioxide (VO2) from the high-temperature tetragonal rutile (R) phase to the low-temperature monoclinic M1 or M2 phase may induce the formation of a variety of domain structures. Here, all possible types of phase-transition-induced domain structures of the M1 and M2 phases have been theoretically formulated by using a general space group method. The predicted domain structures of the M1 phase, including mirror or rotation twins and antiphase domains, have been confirmed by transmission electron microscopy observation of VO2powders and films, while the antiphase domains have never been involved in previous studies. The changes undergone by domain structures during a thermal or electron-beam-induced phase transition have been investigated. These results may suggest the potential influence of domain structures on the nucleation and progress of phase transitions, which unambiguously affect the hysteresis behavior of the first-order transition of VO2.

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9

Li, Zhen, Ralph Skomski, Steven Michalski, Lanping Yue, and Roger D. Kirby. "Magnetic antiphase domains in Co/Ru/Co trilayers." Journal of Applied Physics 107, no. 9 (2010): 09D303. http://dx.doi.org/10.1063/1.3367966.

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10

Rzepski, Jacqueline Devaud, Annick Quivy, Yvonne Calvayrac, Marianne Corner-Quiquandon, and Denis Gratias. "Antiphase domains in icosahedral Al‐Cu‐Fe alloy." Philosophical Magazine B 60, no. 6 (1989): 855–69. http://dx.doi.org/10.1080/13642818908209747.

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11

Liliental-Weber, Zuzanna, Michael A. O'Keefe, and Jack Washburn. "Lattice imaging of antiphase boundaries in GaAs grown on Si." Proceedings, annual meeting, Electron Microscopy Society of America 46 (1988): 598–99. http://dx.doi.org/10.1017/s0424820100105059.

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The growth of GaAs on Si has been recognized as a highly desirable technology goal for a number of years. However, the large lattice misfit between GaAs and Si and the problem of growing a polar crystal on a nonpolar substrate can result in a high density of lattice defects, including antiphase disorder. At an antiphase boundary (APB) the Ga-As bonds are replaced by As-As and Ga-Ga bonds. It is expected that APBs can be highly charged, and they might collect charged impurities unless alternating As-As and Ga-Ga bonds are so close that they can neutralize each other. APBs can result from the coalescence of GaAs domains independently nucleated on the Si substrate. This can occur due to a single step or an odd number of (a/4) Si surface steps, or when the coalescing domains have grown so that one domain starts with a Ga layer and the other domain starts with an As layer.

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12

Woodward, P., R.-D. Hoffmann, and A. W. Sleight. "Order-disorder in A2M3+M5+O6 perovskites." Journal of Materials Research 9, no. 8 (1994): 2118–27. http://dx.doi.org/10.1557/jmr.1994.2118.

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Using x-ray and neutron diffraction data, the degree of order of the octahedral site cations has been determined for the perovskites Sr2AlNbO6 and Sr2AlTaO6, which have been prepared by several different methods and annealed at temperatures up to 1690 °C. The degree of order generally increases with increasing synthesis temperature. The amount of cation ordering is, therefore, primarily controlled by kinetic processes and not by thermodynamic equilibrium considerations. Increased order obtained with increased heating time confirms this general kinetic limitation on the degree of order. However, annealing Sr2AlNbO6 in the highest temperature region resulted in some decrease in order, presumably due to thermodynamic considerations. The cubic edge of both compounds decreases significantly with increasing order. Ordered domains are separated by antiphase boundaries which occur in high concentrations. The cubic cell edge within the ordered domains is significantly smaller than the overall cell edge when the concentration of antiphase boundaries is high. The antiphase boundaries cause significant lattice strain which generally decreases as the concentration of antiphase boundaries decreases. Results on other A2M3+M5+O6 systems are briefly presented.

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13

Lei, Shenhui, Huiqing Fan, Jiawen Fang, Xiaohu Ren, Longtao Ma, and Hailin Tian. "Unusual devisable high-performance perovskite materials obtained by engineering in twins, domains, and antiphase boundaries." Inorganic Chemistry Frontiers 5, no. 3 (2018): 568–76. http://dx.doi.org/10.1039/c7qi00711f.

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14

Itoh, Kazuyuki, and Atsukimi Nishikori. "Diffraction intensity from a crystal composed of antiphase domains." Ferroelectrics 234, no. 1 (1999): 39–46. http://dx.doi.org/10.1080/00150199908225280.

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15

Varschavsky, Ari, та Eduardo Donoso. "Antiphase boundary energies of α-CuAl ordered domains". Materials Science and Engineering: A 104 (жовтень 1988): 141–47. http://dx.doi.org/10.1016/0025-5416(88)90415-6.

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16

Gumennyk, K., L. Stefanovich, and E. Feldman. "Kinetics of coupled ordering and segregation in antiphase domains." physica status solidi (b) 246, no. 1 (2009): 56–61. http://dx.doi.org/10.1002/pssb.200844277.

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17

Feng, C. R., D. J. Michel, and C. R. Crowe. "A Transmission Electron Microscope study of APB in TiAl." Proceedings, annual meeting, Electron Microscopy Society of America 47 (August 6, 1989): 326–27. http://dx.doi.org/10.1017/s0424820100153609.

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Antiphase domains are usually observed in materials with an ordered superlattice structure and the domain boundaries are termed antiphase boundaries (APB). For the Ll0 structure of TiAl, no micrographs have been presented to confirm the existence of an APB. The primary reason for this is the high APB energy which is associated with the separation of the superdislocations. However, APB also could be formed thermally. The purpose of this paper is to report the observation of a thermally formed APB in TiAl and to describe the character of this APB.The TEM foils were prepared from a 7.5v% TiB2 particle reinforced Ti-45at% Al alloy, initially produced by Martin Marietta Laboratories through XD™ processing followed by casting. Thin sections were sliced from the block alloy and 3mm discs were cut from the thin sections.

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18

Ping Wang, Yan, Antoine Letoublon, Tra Nguyen Thanh, et al. "Quantitative evaluation of microtwins and antiphase defects in GaP/Si nanolayers for a III–V photonics platform on silicon using a laboratory X-ray diffraction setup." Journal of Applied Crystallography 48, no. 3 (2015): 702–10. http://dx.doi.org/10.1107/s1600576715009954.

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This study is carried out in the context of III–V semiconductor monolithic integration on silicon for optoelectronic device applications. X-ray diffraction is combined with atomic force microscopy and scanning transmission electron microscopy for structural characterization of GaP nanolayers grown on Si. GaP has been chosen as the interfacial layer, owing to its low lattice mismatch with Si. But, microtwins and antiphase boundaries are still difficult to avoid in this system. Absolute quantification of the microtwin volume fraction is used for optimization of the growth procedure in order to eliminate these defects. Lateral correlation lengths associated with mean antiphase boundary distances are then evaluated. Finally, optimized growth conditions lead to the annihilation of antiphase domains within the first 10 nm.

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19

Mezzadri, F., D. Delmonte, F. Orlandi, et al. "Structural and magnetic characterization of the double perovskite Pb2FeMoO6." Journal of Materials Chemistry C 4, no. 7 (2016): 1533–42. http://dx.doi.org/10.1039/c5tc03529e.

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20

Tseng, Bae‐Heng, Song‐Bin Lin, Gin‐Lern Gu, and Wei Chen. "Elimination of orientation domains and antiphase domains in the epitaxial films with chalcopyrite structure." Journal of Applied Physics 79, no. 3 (1996): 1391–96. http://dx.doi.org/10.1063/1.361038.

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21

Fung, K. K., R. L. Withers, Y. F. Yan, and Z. X. Zhao. "Direct observation of antiphase domains in Bi2Sr2CaCu2O8by transmission electron microscopy." Journal of Physics: Condensed Matter 1, no. 1 (1989): 317–22. http://dx.doi.org/10.1088/0953-8984/1/1/028.

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22

M�ller, Wolfgang Friedrich, Yusof Vojdan-Shemshadi, and Horst Pentinghaus. "Transmission electron microscopic study of antiphase domains in CaAl2Ge2O8-Feldspar." Physics and Chemistry of Minerals 14, no. 3 (1987): 235–37. http://dx.doi.org/10.1007/bf00307987.

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23

Hajjari, E., M. Divandari, S. H. Razavi, T. Homma, and S. Kamado. "Intermetallic compounds and antiphase domains in Al/Mg compound casting." Intermetallics 23 (April 2012): 182–86. http://dx.doi.org/10.1016/j.intermet.2011.12.001.

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24

Hu, Yan-Ling, Eric Rind, and James S. Speck. "Antiphase boundaries and rotation domains in In2O3(001) films grown on yttria-stabilized zirconia (001)." Journal of Applied Crystallography 47, no. 1 (2014): 443–48. http://dx.doi.org/10.1107/s1600576713033864.

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In2O3is important because it has been widely used as a transparent contact material and an active gas sensor material. To understand and utilize its intrinsic physics as a semiconductor, it is necessary to have In2O3with a high material quality. In this article, single-crystalline (001)-oriented In2O3thin films were grown on yttria-stabilized zirconia (001) substrate, and a group theory analysis and transmission electron microscopy (TEM) experiments were conducted to investigate the defects within the In2O3film. Owing to the reduced symmetry of the bixbyite structure (space group Ia{\overline 3}) in comparison with the fluorite template (space group Fm {\overline 3}m), the formation of antiphase domains and 90° rotation domains in the In2O3thin films is anticipated. This prediction is confirmed experimentally by TEM and high-angle annular dark-field scanning transmission electron microscopy images. The size of the enclosed domains ranges from 50 to 300 nm, and the major domain boundaries are along the (110), (1{\overline 1}0), (010) and (100) planes. The rotation domains are related by a fourfold rotation operation along the 〈001〉 directions, which will cause the permutation of the axes of the bixbyite structure.

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25

Fukuda, Koichiro. "Intracrystalline Microstructure of Synthetic Merwinite." Journal of Materials Research 15, no. 7 (2000): 1570–75. http://dx.doi.org/10.1557/jmr.2000.0225.

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Crystals of merwinite were prepared at 1550 °C from chemical reagents, and their intracrystalline microstructures were examined by the combined use of x-ray diffraction and optical microscopy. The crystals were composed of pseudomerohedral twins. The adjacent twin domains were related by the pseudosymmetry two-fold axis parallel to ⟨011⟩with the composition surface {811} The overall twin structure was constructed by introducing the pseudo-symmetry three-fold axis normal to (100), which must originally be a symmetry element of the former high-symmetry phase. The transition from the primitive trigonal (point group 3m) to the primitive monoclinic (space group P21/a) was accompanied by the combination of reducing the order of the point group and the change in the size of the unit cell. The order of the point group was reduced from 12 to 4, resulting in three twin domains with six different interfaces. This accounted for the experimentally observed microstructure consisting of repeated lamella twins in several orientations. Because the unit lattice translation would be lost during the transition, the formation of antiphase domains was expected. The lost translation vectors were 1/2[011], 1/2[100], and 1/2[111] resulting in four antiphase domains. As a result, the total number of domains possible in the transition was 3 × 4 = 12.

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26

Kulkarni, U. D., S. Hata, T. Nakano, M. Mitsuhara, K. Ikeda та H. Nakashima. "Monte Carlo simulation of antiphase boundaries and growth of antiphase domains in Al5Ti3phase in Al-rich γ-TiAl intermetallics". Philosophical Magazine 91, № 22 (2011): 3068–78. http://dx.doi.org/10.1080/14786435.2011.563761.

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27

Moore, KT, DR Veblen, and JM Howe. "Experimental Evidence of Ca Segregation to Antiphase Boundaries in Pigeonite." Microscopy and Microanalysis 7, S2 (2001): 254–55. http://dx.doi.org/10.1017/s1431927600027343.

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For over 30 years geologists have been trying to better understand antiphase domains (APD) and boundaries (APB) in pigeonite in hopes of using them as markers for the thermal history of the rocks in which they are found. The ability to know the cooling history of igneous rocks is of great interest to geologists and pigeonite has received special attention on this matter because it has exsolution (precipitation) and antiphase domains (APD), both of which can be used as possible thermal markers. APDs in pigeonite arise because of the C2/c → P21/c transformation that occurs upon cooling. When multiple APDs nucleate, grow, and impinge upon one another, they are either in registry or have a translational discrepancy of ½(a+b). The size of the APDs can be used as a qualitative marker of cooling rates, since slowly cooled pigeonites favor large APDs and rapidly cooled pigeonites favor small APDs.

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28

Prakash, U., R. A. Buckley, and H. Jones. "Formation of B2 antiphase domains in rapidly solidified Fe-Al alloys." Philosophical Magazine A 64, no. 4 (1991): 797–805. http://dx.doi.org/10.1080/01418619108213949.

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29

Zheng, S. J., and X. L. Ma. "Asymmetrical twin boundaries and highly dense antiphase domains in BaNb0.3Ti0.7O3thin films." Philosophical Magazine 87, no. 28 (2007): 4421–31. http://dx.doi.org/10.1080/14786430701541138.

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30

Kobayashi, Keisuke, Tsukasa Koyama, Hideki Kamo, et al. "Doping Effect on Interlocked Ferroelectric and Structural Antiphase Domains in YMnO3." Japanese Journal of Applied Physics 51, no. 9S1 (2012): 09LE09. http://dx.doi.org/10.7567/jjap.51.09le09.

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31

Takeno, S., S. Nakamura, K. Abe, and S. Komatsu. "A novel mosaic-like structure in SrTiO3 thin films on a Pt(001) surface revealed by transmission electron microscopy." Journal of Materials Research 11, no. 11 (1996): 2777–84. http://dx.doi.org/10.1557/jmr.1996.0351.

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A novel mosaic-like structure in SrTiO3 thin films was discovered and characterized by means of transmission electron microscopy (TEM). The films were deposited on a (001) oriented Pt surface. The orientation relationship between SrTiO3 film and Pt substrate was determined, and four types of growth modes were revealed. These four growth modes formed four types of domains, respectively, and these domains and Pt formed peculiarly ordered interfacial structures, i.e., near coincidence site lattices. Antiphase boundaries between two adjacent domains were also observed by high-resolution imaging.

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32

Kimura, M., J. B. Cohen, S. Chandavarkar, and K. Liang. "Short-range ordering of Cu3Au above Tc in the topmost 80 A of a (001) face." Journal of Materials Research 12, no. 1 (1997): 75–82. http://dx.doi.org/10.1557/jmr.1997.0013.

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The short-range order in the near surface region of the Cu3Au(001) face was investigated above the critical temperature by glancing-incidence x-ray diffraction, measuring the diffuse intensity throughout a two-dimensional region of reciprocal space. This intensity was analyzed quantitatively to obtain the two-dimensional Cowley–Warren short-range-order parameters and atomic displacements. Monte-Carlo simulation based on these values has revealed that the atomic configurations in the surface consist of ordered domains and clusters in a disordered matrix. There is a large number of {10} antiphase domain boundaries (APDB).

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33

Hall, Ernest L., та Ami E. Berkowitz. "Microstructural defects in γ-Fe2O3 particles". Journal of Materials Research 1, № 6 (1986): 836–44. http://dx.doi.org/10.1557/jmr.1986.0836.

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The microstructure of three different types of γ-Fe2O3 particles were examined using transmission electron microscopy. These included pure γ-Fe2O3, γ-Fe2O3 that had been surface modified using Co, and γ-Fe2O3 that had been doped with Co. The major internal microstructural defects found in the particles in all of the samples were pores and antiphase boundaries. Some particles also had a very high density of dislocations and low-angle boundaries. In general, the particles could be described as single crystals with symmetric cross section. The structure is based on a tetragonal unit cell, and each particle is divided into antiphase domains in which the c axis is oriented at 90°with respect to adjoining domains. The particles often exhibited very irregular shapes. No effect of Co modification was seen on the internal or surface structure of the particles. The Co-doped particles were found to be smaller in size and contained a lower density of internal defects. The effect of the microstructural defects and morphological irregularities in these particles on magnetic behavior is discussed.

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34

Kobayashi, K., H. Kamo, K. Kurushima, et al. "Real-space imaging of ferroelectric and structural antiphase domains in hexagonal YMnO3." Journal of the Korean Physical Society 62, no. 7 (2013): 1077–81. http://dx.doi.org/10.3938/jkps.62.1077.

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35

Wan, Li, Yawei Li, Xiangjian Meng, et al. "Observation of antiphase domains in BiFeO3 thin films by X-ray diffraction." Physica B: Condensed Matter 391, no. 1 (2007): 124–29. http://dx.doi.org/10.1016/j.physb.2006.09.007.

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36

Kobayashi, Keisuke, Tsukasa Koyama, Hideki Kamo, et al. "Doping Effect on Interlocked Ferroelectric and Structural Antiphase Domains in YMnO$_{3}$." Japanese Journal of Applied Physics 51 (September 20, 2012): 09LE09. http://dx.doi.org/10.1143/jjap.51.09le09.

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37

Datta, R., S. Kanuri, S. V. Karthik, D. Mazumdar, J. X. Ma, and A. Gupta. "Formation of antiphase domains in NiFe2O4 thin films deposited on different substrates." Applied Physics Letters 97, no. 7 (2010): 071907. http://dx.doi.org/10.1063/1.3481365.

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38

Ueda, O., T. Soga, T. Jimbo, and M. Umeno. "Direct evidence for self‐annihilation of antiphase domains in GaAs/Si heterostructures." Applied Physics Letters 55, no. 5 (1989): 445–47. http://dx.doi.org/10.1063/1.101870.

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39

Gusak, Andriy, Rafal Abdank-Kozubski, and Dmytro Tyshchenko. "Grain Growth in Open Systems." Diffusion Foundations 5 (July 2015): 229–44. http://dx.doi.org/10.4028/www.scientific.net/df.5.229.

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Grain growth in open systems is analyzed for the cases of flux-driven ripening during soldering, flux-driven lateral growth during deposition of thin films, flux-driven lateral growth during reactive growth of intermediate phase, flux-driven lateral growth of antiphase domains in FCC-phase A3B and BCC-phase AB during the diffusion growth of ordered phase layer.

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40

Huang, Y., and J. M. Cowley. "The long-period structure on ordering alloy surfaces." Proceedings, annual meeting, Electron Microscopy Society of America 52 (1994): 816–17. http://dx.doi.org/10.1017/s042482010017181x.

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The long-period structure (LPS) has long been known to exist in bulk ordering alloys such as CuAu and Cu3Au. in the structure the ordered lattice shifts back and forth by a vector every M unit cells and forms a super cell 2M unit cells long. The planes where the lattice shifts are usually called antiphase boundaries (APBs) and the LPS can be regarded as periodically arranged antiphase domains. This superstructure can be detected by the splitting (∝1/M) of some superlattice spots in the diffraction panern. One may ask whether the LPS also occurs on the surface; if so, what is its effect onthe diffraction pattern. The answer to them is important to explain some unknown features observed in the RHEED experiment. They also have significance for the surface transition theories.Ideal termination of a LPS Cu3Au crystal gives a surface first-layer atomic arrangement shown in fig.1a. In this arrangement the basic vectors a and b of the surface hexagonal ordered structure are two bulk {110} vectors. Every M unit cells in a direction the lattice shifts by(1/2)b. This forms the 2-D super unit cell with a size of 2Ma×b. The relatively shifted areas are actually 2-D antiphase domains. The boundaries between them are the periodically arranged linear APBs. All these features indicate that the ideal Cu3Au(111) surface is indeed a 2-D LPS. Fig.1b and 1c show the 2-D reciprocal lattice calculated from the above surface arrangement.

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41

Lee, Kap Ho, Yeung Jo Lee, and Kenji Hiraga. "Precipitation behavior in the early stage of aging in an Al–Li°Cu–Mg–Zr–Ag (Weldalite 049) alloy." Journal of Materials Research 14, no. 2 (1999): 384–89. http://dx.doi.org/10.1557/jmr.1999.0056.

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The precipitation behavior of various phases during the aging process of an Ag–Li°Cu–Mg–Zr–Ag (Weldalite 049) alloy was investigated by high-resolution electron microscopy and in situ hot-stage microscopy. Two kinds of domains with L12-type ordered structures, which are considered to be δ′ and β′ phases, are observed with different domain sizes in the alloy quenched from 530 °C. In the early stage of aging at 190 °C, the δ′ phase is precipitated as surrounding the β' phase, and the δ′ domains appear with in-phase and antiphase relationships to the β′ lattices. In situ observations at 190 °C clearly show that the T1 phase precipitates predominantly on dislocations at subgrain boundaries and then is homogeneously formed in the matrix with increasing aging time. The nucleation of the S′ phase is associated with clustering of Cu and Mg in the matrix, and the S0 domains are grown with {210} habit planes.

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42

MIRANDA, MONTSERRAT A., and JAVIER BURGUETE. "SPATIOTEMPORAL PHASE SYNCHRONIZATION IN A LARGE ARRAY OF CONVECTIVE OSCILLATORS." International Journal of Bifurcation and Chaos 20, no. 03 (2010): 835–47. http://dx.doi.org/10.1142/s0218127410026125.

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In a quasi-1D thermal convective system consisting of a large array of nonlinearly coupled oscillators, clustering is the way to achieve a regime of mostly antiphase synchronized oscillators. This regime is characterized by a spatiotemporal doubling of traveling modes. As the dynamics is explored beyond a spatiotemporal chaos regime (STC) with weak coupling, new interacting modes emerge through a supercritical bifurcation. In this new regime, the system exhibits coherent subsystems of antiphase synchronized oscillators, which are stationary clusters following a spatiotemporal beating phenomena (ZZ regime). This regime is the result of a stronger coupling. We show from a phase mismatch model applied to each oscillator, that these phase coherent domains undergo a global phase instability, meanwhile the interactions between oscillators become nonlocal. For each value of the control parameter we find out the time-varying topology (link matrix) from the contact interactions between oscillators. The new characteristic spatiotemporal scales are extracted from the antiphase correlations at the time intervals defined by the link matrix. The interpretation of these experimental results contributes to widen the understanding of other complex systems exhibiting similar phase chaotic dynamics in 2D and 3D.

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43

Bolshakov, Alexey D., Vladimir V. Fedorov, Olga Yu Koval, et al. "Effective Suppression of Antiphase Domains in GaP(N)/GaP Heterostructures on Si(001)." Crystal Growth & Design 19, no. 8 (2019): 4510–20. http://dx.doi.org/10.1021/acs.cgd.9b00266.

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Stefanovich, L. I., and É. P. Fel’dman. "Kinetics of formation and growth of antiphase domains during second-order phase transitions." Journal of Experimental and Theoretical Physics 86, no. 1 (1998): 128–33. http://dx.doi.org/10.1134/1.558477.

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Chou, T. C., and K. N. Tu. "Secondary grain growth and formation of antiphase domains in ordered Cu3Au thin films." Journal of Applied Physics 64, no. 5 (1988): 2375–79. http://dx.doi.org/10.1063/1.341669.

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Farin, P., M. Marquardt, W. Martyanov, et al. "Three-dimensional structure of antiphase domains in GaP on Si(0 0 1)." Journal of Physics: Condensed Matter 31, no. 14 (2019): 144001. http://dx.doi.org/10.1088/1361-648x/aafcfb.

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Berenguer, Felisa, Richard Bean, Catriona McCallion, et al. "Coherent X-ray diffraction imaging of antiphase domains and biological tissues with ptychography." Acta Crystallographica Section A Foundations of Crystallography 65, a1 (2009): s66—s67. http://dx.doi.org/10.1107/s0108767309098705.

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Wang, Yunzhi, and Armen Khachaturyan. "Effect of antiphase domains on shape and spatial arrangement of coherent ordered intermetallics." Scripta Metallurgica et Materialia 31, no. 10 (1994): 1425–30. http://dx.doi.org/10.1016/0956-716x(94)90130-9.

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Vronka, Marek, Ladislav Straka, Marc De Graef, and Oleg Heczko. "Antiphase boundaries, magnetic domains, and magnetic vortices in Ni–Mn–Ga single crystals." Acta Materialia 184 (February 2020): 179–86. http://dx.doi.org/10.1016/j.actamat.2019.11.043.

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Li, Yuan, G. Salviati, M. M. G. Bongers, L. Lazzarini, L. Nasi, and L. J. Giling. "On the formation of antiphase domains in the system of GaAs on Ge." Journal of Crystal Growth 163, no. 3 (1996): 195–202. http://dx.doi.org/10.1016/0022-0248(95)00958-2.

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