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Статті в журналах з теми "Amorphous structure"

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Автор: Grafiati

Опубліковано: 30 травня 2022

Оновлено: 31 травня 2022

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1

Weibin Qiu, Weibin Qiu, and Jiaxian Wang Jiaxian Wang. "Low-loss amorphous Si waveguides with gradient refractive index cladding structure." Chinese Optics Letters 10, no. 4 (2012): 041601–41602. http://dx.doi.org/10.3788/col201210.041601.

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2

Niu, Yihan, Dan Zhao, Bo Zhu, Shunbo Wang, Zhaoxin Wang, and Hongwei Zhao. "Molecular dynamics investigations of the size effects on mechanical properties and deformation mechanism of amorphous and monocrystalline composite AlFeNiCrCu high-entropy alloy nanowires." Nanotechnology 33, no. 10 (December 15, 2021): 105705. http://dx.doi.org/10.1088/1361-6528/ac2e79.

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Анотація:

Abstract The atomic models of amorphous and monocrystalline composite AlFeNiCrCu high-entropy alloy nanowires were established via the molecular dynamics method. The effects of amorphous structure thickness on mechanical properties and deformation mechanism were investigated by applying tensile and compressive loads to the nanowires. As the thickness of amorphous structures increases, the tensile yield strength decreases, and the asymmetry between tension and compression decreases. The tensile deformation mechanism transforms from the coupling interactions between stacking faults in crystal structures and uniform deformation of amorphous structures to the individual actions of uniform deformation of amorphous structures. During the tensile process, the nanowires necking appears at amorphous structures, and the thinner amorphous structures, the more prone to necking. The compressive deformation mechanism is the synergistic effects of twins and SFs in crystal structures and uniform deformation of amorphous structures, which is irrelevant to amorphous structure thickness. Remarkably, amorphous structures transform into crystal structures in the amorphous and monocrystalline composite nanowires during the compressive process.

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3

Roche, Olivier, Frederick Freundlich, Frank Shipper, and Charles C. Manz. "Mondragon’s amorphous network structure." Organizational Dynamics 47, no. 3 (July 2018): 155–64. http://dx.doi.org/10.1016/j.orgdyn.2018.01.001.

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4

Weber, Th, J. C. Muijsers, and J. W. Niemantsverdriet. "Structure of Amorphous MoS3." Journal of Physical Chemistry 99, no. 22 (June 1995): 9194–200. http://dx.doi.org/10.1021/j100022a037.

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5

Lamparter, P., and R. Kniep. "Structure of amorphous Al2O3." Physica B: Condensed Matter 234-236 (June 1997): 405–6. http://dx.doi.org/10.1016/s0921-4526(96)01044-7.

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6

Nakamura, N., H. Tarui, T. Matsuyama, K. Watanabe, S. Noguchi, S. Tsuda, S. Nakano, Y. Kuwano, and S. Ohara. "Amorphous superlattice structure devices." IEEE Transactions on Electron Devices 35, no. 12 (1988): 2448. http://dx.doi.org/10.1109/16.8876.

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7

Kobashi, Yukitaka, and Shiro Kodera. "Structure of Amorphous Selenium." Japanese Journal of Applied Physics 37, Part 1, No. 5A (May 15, 1998): 2590–92. http://dx.doi.org/10.1143/jjap.37.2590.

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8

Kobayashi, Masayoshi. "Structure of amorphous boron." Journal of Materials Science 23, no. 12 (December 1988): 4392–98. http://dx.doi.org/10.1007/bf00551937.

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9

Oda, Naoto, Aya Tominaga, Hiroshi Sekiguchi, Ryoko Nakano, and Shigeru Yao. "Development of an Internal Structure by Amorphous Polymer in the Melt State." Nihon Reoroji Gakkaishi 45, no. 2 (2017): 101–5. http://dx.doi.org/10.1678/rheology.45.101.

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10

Ryaguzov, A. P. "STUDY OF THE STRUCTURE OF AMORPHOUS CARBON FILMS MODIFIED WITH SILICON OXIDE." Eurasian Physical Technical Journal 16, no. 1 (June 14, 2019): 6–11. http://dx.doi.org/10.31489/2019no1/6-11.

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11

Long, N. J., and H. J. Trodahl. "Structure of amorphous carbon in amorphous C/Ge multilayers." Journal of Applied Physics 67, no. 4 (February 15, 1990): 1753–56. http://dx.doi.org/10.1063/1.345599.

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12

Dubinets, Aleksandr, Evgeny Pustovalov, Evgeny B. Modin, Aleksandr N. Fedorets, Vladimir Tkachev, and Vladimir Plotnikov. "Modeling of Structures Nanocrystalline and Amorphous Alloys." Solid State Phenomena 245 (October 2015): 60–66. http://dx.doi.org/10.4028/www.scientific.net/ssp.245.60.

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Анотація:

In this paper discusses and demonstrates the possibility of modeling materials with amorphous and nanocrystalline structure using random close packing of atoms and nanoclusters models. Concordance structure of the real models alloys was evaluated by the radial distribution function obtained as a result of calculations, and in its modeled structures estimation. Modeling structure of the amorphous matrix and the spatial distribution of nanoclusters in two-component amorphous alloys with composition Fe80B20carried out by Ishikawa method. For modeling structure multicomponent amorphous metal alloys we developed correlation-spectral model of the amorphous matrix and nanoclusters. At modeling passing electron wave through the sample used a layered approach, and for the "visualization" imaging we modeled optical schemes of high-resolution electron microscopes.

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13

SHIROTA, Yasuhiko. "Amorphous Structure and Relaxation in Glassy Polymers. Amorphous Molecular Mateials: Structures and Morphological Changes." Kobunshi 47, no. 5 (1998): 309–12. http://dx.doi.org/10.1295/kobunshi.47.309.

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14

Fukunaga, Toshiharu. "Partial structure of amorphous metal." Bulletin of the Japan Institute of Metals 26, no. 6 (1987): 481–89. http://dx.doi.org/10.2320/materia1962.26.481.

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15

Hirotsu, Yoshihiko. "Local structure of amorphous alloys." Bulletin of the Japan Institute of Metals 27, no. 9 (1988): 714–19. http://dx.doi.org/10.2320/materia1962.27.714.

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16

Wu Zhen-Wei, Li Mao-Zhi, Xu Li-Mei, and Wang Wei-Hua. "Inherited structure of amorphous matter." Acta Physica Sinica 66, no. 17 (2017): 176405. http://dx.doi.org/10.7498/aps.66.176405.

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17

Hausleitner, Ch, and J. Hafner. "Structure of amorphous FeZr alloys." Journal of Non-Crystalline Solids 144 (January 1992): 175–86. http://dx.doi.org/10.1016/s0022-3093(05)80398-9.

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18

TANIO, Norihisa. "Amorphous Structure and Optical Properties." Kobunshi 55, no. 9 (2006): 734–37. http://dx.doi.org/10.1295/kobunshi.55.734.

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19

Nuding, Ma, P. Lamparter, S. Steeb, and R. Bellissent. "Structure of hydrogenated amorphous Ni56Dy44." Journal of Alloys and Compounds 253-254 (May 1997): 118–20. http://dx.doi.org/10.1016/s0925-8388(96)02911-8.

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20

Abrosimova, Galina E. "Structure evolution of amorphous alloys." Uspekhi Fizicheskih Nauk 181, no. 12 (2011): 1265. http://dx.doi.org/10.3367/ufnr.0181.201112b.1265.

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21

Eichinger, Bruce E., Erich Wimmer, and Jannie Pretorius. "The structure of amorphous sulfur." Macromolecular Symposia 171, no. 1 (June 2001): 45–56. http://dx.doi.org/10.1002/1521-3900(200106)171:1<45::aid-masy45>3.0.co;2-n.

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22

Inam, F., James P. Lewis, and D. A. Drabold. "Hidden structure in amorphous solids." physica status solidi (a) 207, no. 3 (February 4, 2010): 599–604. http://dx.doi.org/10.1002/pssa.200982877.

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23

Weber, TH, J. C. Muijsers, and J. W. Niemantsverdriet. "The Structure of Amorphous MoS3." Bulletin des Sociétés Chimiques Belges 104, no. 4-5 (September 1, 2010): 299. http://dx.doi.org/10.1002/bscb.19951040417.

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24

Kobayashi, Masayoshi, Iwami Higashi, and Michio Takami. "Fundamental Structure of Amorphous Boron." Journal of Solid State Chemistry 133, no. 1 (October 1997): 211–14. http://dx.doi.org/10.1006/jssc.1997.7430.

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25

Suzuki, Kenji. "Dynamic Structure of Amorphous Solids." Radiation Effects and Defects in Solids 148, no. 1-4 (August 1999): 85–86. http://dx.doi.org/10.1080/10420159908229086.

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26

Elliott, S. R., J. C. Dore, and E. Marseglia. "THE STRUCTURE OF AMORPHOUS PHOSPHORUS." Le Journal de Physique Colloques 46, no. C8 (December 1985): C8–349—C8–353. http://dx.doi.org/10.1051/jphyscol:1985852.

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27

Uda, Tsuyoshi. "Atomic structure of amorphous silicon." Solid State Communications 64, no. 5 (November 1987): 837–41. http://dx.doi.org/10.1016/0038-1098(87)90712-5.

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28

O'Reilly, E. P., J. Robertson, and D. Beeman. "Electronic structure of amorphous carbon." Journal of Non-Crystalline Solids 77-78 (December 1985): 83–86. http://dx.doi.org/10.1016/0022-3093(85)90616-7.

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29

Truss, J. K. "The structure of amorphous sets." Annals of Pure and Applied Logic 73, no. 2 (June 1995): 191–233. http://dx.doi.org/10.1016/0168-0072(94)00024-w.

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30

Liebing, L., and F. Künstler. "Lamellate structure of amorphous silicon." Solar Energy Materials 14, no. 2 (October 1986): 79–94. http://dx.doi.org/10.1016/0165-1633(86)90067-5.

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31

Agarwal, S. C. "Electronic structure of amorphous semiconductors." Bulletin of Materials Science 18, no. 6 (October 1995): 669–78. http://dx.doi.org/10.1007/bf02744803.

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32

Drchal, V., and J. Málek. "Electronic structure of amorphous GeS." Solid State Communications 73, no. 2 (January 1990): 163–66. http://dx.doi.org/10.1016/0038-1098(90)91039-j.

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33

Holzman, Louis M., Yeon-Wook Kim, and Thomas F. Kelly. "Structure of pure metallic and semiconductor glasses." Proceedings, annual meeting, Electron Microscopy Society of America 48, no. 4 (August 1990): 142–43. http://dx.doi.org/10.1017/s0424820100173844.

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Анотація:

There has been a great deal of interest in amorphous materials as the advance of technology has enabled a greater variety of alloys and elements to be quenched into the amorphous state and as new uses for amorphous materials have been developed. Because the analysis of the structure of amorphous alloys is quite complicated, it is highly desirable to have specimens available of pure elements in the amorphous state in order to more easily study amorphous structure and for comparison with theory. However, very few pure elements have been quenched into the amorphous state and most of those that have been are only stable at temperatures close to absolute zero. This has limited the methods available for the study of their structure. We have produced room-temperature-stable amorphous samples of pure elements (V,Nb,Ta,Mo,W,Fe,Co,Ni,Si,Ge) from the melt using electrohydrodynamic (EHD) atomization. Diffraction patterns of these samples were obtained using a Vacuum Generators HB501 STEM and these patterns were analyzed to obtain the radial distribution function for the pure element specimens.

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34

Hirotsu, Yoshihiko, Kazunori Anazawa, and Sigemaro Nagakura. "Structure of sputter-deposited amorphous Pd-Si alloy studied by High Resolution Electron Microscopy." Proceedings, annual meeting, Electron Microscopy Society of America 48, no. 4 (August 1990): 126–27. http://dx.doi.org/10.1017/s0424820100173765.

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Recent structural studies of amorphous alloys by precise X-ray and neutron diffraction, Mossbauer spectroscopy and NMR have shown an atomic ordering developing beyond the first neighbor atomic distance, which is called a medium range ordering (MRO) of atoms in amorphous alloys. Lattice fringe images extending in a range of 1 to 2 nm have been observed in amorphous alloys by high resolution electron microscopy(HREM), indicating a possible formation of the MRO structures. In our HREM study of amorphous Pd77.5Cu6Si16.5 alloy ribbons, MRO domains with α-Pd-like structure were observed under the most appropriate underfocus condition. For more detailed understanding of MRO structure, it is necessary to calculate HREM images for possible MRO models and compare them with observed ones. In this study, we calculated HREM images for an amorphous Pd80Si20 with (1) a dense random packing(DRP) structure, (2) a FCC MRO structure( a FCC cluster embedded in the DRP structure) and (3) an icosahedral MRO structure( an icosahedral cluster embedded in the DRP structure).

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35

O’Keefe, Michael A., and Margaret L. Sattler. "HRTEM simulation of amorphous materials." Proceedings, annual meeting, Electron Microscopy Society of America 48, no. 4 (August 1990): 112–13. http://dx.doi.org/10.1017/s0424820100173698.

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Image simulation has become one of the preferred techniques for analysis of high-resolution transmission electron micrographs, in both bright-field and dark-field modes. This is especially true of microscope images used in stuctural studies, both for perfect crystal structures, and for defects within periodic structures. In using image simulation for structural analysis, comparison is made point-by-point (pixel by pixel) between the experimental image and one simulated under identical imaging conditions for a model structure. Comparison with a matching simulated image enables features in the experimental image to be identified as belonging to structural features in the specimen, such as groups of atoms, or individual atoms. In the case of amorphous structures, however, no such one-to-one correspondence between simulations and experimental high-resolution images can be expected. It is thus much more difficult to determine whether the model from which one is simulating images really does describe the appropriate amorphous structure. Amorphous structures are characterized not in terms of atom positions within a well-defined unit cell, but interms of a “radial distribution function” (RDF), a function that gives the average number of atoms lying at any given distance from an average atom. The RDF is thus a non-periodic Patterson function, and a single RDF can arise from many different arrangements of atoms, provided only that atomic positions within the structure have the “right” statistical distribution.

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36

Nor, R. M., S. N. M. Halim, Mohamad Fariz Mohamad Taib, and M. Kamil Abd-Rahman. "First Principles Investigation on the Structural, Electronic and Optical Properties of Amorphous Silica Glass." Solid State Phenomena 268 (October 2017): 92–96. http://dx.doi.org/10.4028/www.scientific.net/ssp.268.92.

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The structural, electronic, and optical properties of an amorphous SiO2 (a-SiO2) model is investigated by using first-principles calculation. Most research works used beta-cristobalite glass structure as a reference to amorphous silica structure. However, only the electronic properties were been presented without any link towards the optical properties. Here, we demonstrate simultaneous electronic and optical properties, which closely matched to a-SiO2 properties by generating small sample of amorphous quartz glass. Using the Rietveld refinement, amorphous silica structure was generated and optimized using density functional theory in CASTEP computer code. A thorough analysis of the amorphous quartz structure obtained from different thermal treatment was carried out. The structure of amorphous silica was validated with previous theoretical and experimental works. It is shown that small sample of amorphous silica have similar structural, electronic and optical properties with a larger sample. The calculated optical and electronic properties from the a-SiO2 glass match closely to previous theoretical and experimental data from others. The a-SiO2 band gap of 5.853 eV is found to be smaller than the experimental value of ~9 eV. This is due to the underestimation and assumption made in DFT. However, the band gap value is in good agreement with the other theoretical works. Apart from the absorption edge at around 6.5 eV, the refractive index is 1.5 at 0eV. Therefore, this atomic structure can served as a reference model for future research works on amorphous structures.

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37

Магомедов, М. Н. "Уравнение состояния и поверхностные свойства аморфного железа". Журнал технической физики 90, № 10 (2020): 1731. http://dx.doi.org/10.21883/jtf.2020.10.49806.62-20.

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It is shown that on the nonlinear dependence of the first coordination number (kn) versus the packing coefficient (kp) of the structure of a mono-component substance, three special points corresponding to the amorphous structure can be distinguished. Based on the pairwise interatomic potential of Mie–Lennard-Jones, the state equation and properties of iron for both these three amorphous structures and the crystal state are calculated. It is shown that at kp = 0.45556 and kn = 6.2793 the minimum chemical potential is reached, i.e. this point is corresponding a thermodynamically stable amorphous structure into the liquid phase. An energetically equivalent point with the same kn value, but with kp = 0.6237, is a thermodynamically unstable amorphous structure corresponding to the solid phase. It is shown that the specific surface energy of an amorphous solid metal is greater than that of an amorphous liquid phase, but less than that of a metal in the crystalline state. This should lead to the fact that the surface of the crystal metal should tend to amorphize.

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38

Ni, Bing Ying, and Zhan Kui Zhao. "Evolution and Performance of Porous Structure on the Surface of Fe₇₆Si_7.2B_9.6P_7.2 Amorphous Ribbon." Materials Science Forum 898 (June 2017): 653–56. http://dx.doi.org/10.4028/www.scientific.net/msf.898.653.

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Анотація:

Porous structures with enhanced specific surface area exhibit higher catalytic activity than the bulk counterpart. In this work, the porous structures with tunable pore size are synthesized through chemical dealloying of the Fe76Si7.2B9.6P7.2 amorphous alloys in corrosion solution. Meanwhile, under the effect of ultrasound-assistance, the distribution of porous and composition are uniform on the amorphous alloys. X-ray diffraction demonstrated that the amorphous structure has not been corrupted or tampered in the dealloyed samples. It was also found that the porous alloy shows superior catalytic activity in degrading phenol-containing wastewater, the degradation rate significantly increases as compared to the un-dealloyed Fe76Si7.2B9.6P7.2 amorphous alloys. Finally, the formation mechanism of porous structure is discussed.

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39

Shelyakov, Alexander, Nikolay Sitnikov, Irina Zaletova, Natalia Tabachkova, and Nikolay Andreev. "Effect of External Impacts on the Structure and Martensitic Transformation of Rapidly Quenched TiNiCu Alloys." Metals 11, no. 10 (September 26, 2021): 1528. http://dx.doi.org/10.3390/met11101528.

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TiNi-TiCu quasibinary system alloys with a high Cu content produced by rapid quenching from liquid state in the form of thin amorphous ribbons exhibit pronounced shape memory effect after crystallization and are promising materials for miniaturized and fast operating devices. There is currently no complete clarity of the mechanisms of structure formation during crystallization from the amorphous state that determine the structure-sensitive properties of these alloys. This work deals with the effect of the initial amorphous state structure and crystallization method of the alloys on their structure and phase transformations. To this end the alloy containing 30 at.% Cu was subjected to thermal and mechanical impact in the amorphous state and crystallized using isothermal or electropulse treatment. We show that after all types of treatment in the amorphous state the structure of the alloy remains almost completely amorphous but the characteristic temperatures and enthalpy of crystallization become slightly lower. Isothermal crystallization of alloy specimens produces a submicrocrystalline structure with an average grain size in the 0.4–1.0 μm range whereas electropulse crystallization generates a bimorphic structure consisting of large 4–6 μm grains and 2–3 μm high columnar crystals in the vicinity of the surface. The grains have nanosized plate-like and subgrain structures. The largest grains are observed in thermally activated samples, meanwhile, mechanical impact in the amorphous state leads to the formation of equiaxed finer grains with a less defective subgrain structure and to the shift of the temperature range of the martensitic transformation toward lower temperatures.

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40

Hobbs, Linn W., Xianglong Yuan, L. C. Qin, Vinay Pulim, and Alexander Coventry. "The Nanostructures of Amorphous Silicas." Microscopy and Microanalysis 8, no. 1 (February 2002): 29–34. http://dx.doi.org/10.1017/s1431927602010061.

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Анотація:

Topologically modeled amorphized silica structures have been refined using a molecular dynamics simulation technique. Several metastable structures with substantially different medium-range connectivities, as characterized by primitive ring statistics, were obtained. Whereas the total correlation function is insensitive to these differences, the first sharp diffraction peak derived from energy-filtered electron diffraction shows a promising correlation to medium-range structure.

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41

Prikhodko, O., M. Maltekbasov, N. Almasov, S. Maximova, V. Ushanov, S. Dyusembayev, and S. Kozyukhin. "Structure and electronic properties of amorphous As40Se30S30 films prepared by ion-plasma sputtering method." Physical Sciences and Technology 2, no. 1 (2015): 24–29. http://dx.doi.org/10.26577/2409-6121-2015-2-1-24-29.

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42

Zong, R. L., S. P. Wen, F. Lv, F. Zeng, Y. Gao, and F. Pan. "Amorphous-CuTa/amorphous-CoZrNb multilayers: Structure, mechanical properties and thermal stability." Surface and Coatings Technology 202, no. 17 (May 2008): 4242–47. http://dx.doi.org/10.1016/j.surfcoat.2008.03.017.

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43

Hsieh, H. Y., B. H. Toby, T. Egami, Y. He, S. J. Poon, and G. J. Shiflet. "Atomic structure of amorphous Al90FexCe10−x." Journal of Materials Research 5, no. 12 (December 1990): 2807–12. http://dx.doi.org/10.1557/jmr.1990.2807.

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Анотація:

The atomic structure of liquid-quenched amorphous Al90FexCe10−x(x= 5,7) was studied by pulsed neutron and x-ray scattering. The atomic pair-density function determined by pulsed neutron diffraction indicates that a significant portion of Al–Fe distances is anomalously short, while some part of the Al–Al distances is anomalously long. Both neutron and x-ray scattering showed the presence of a prepeak in the structure factor. These results suggest that a strong interaction between A1 and Fe modifies the structure of this glass, leading to chemical and topological short-range ordering.

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44

Hung, P. K., D. K. Belashchenko, V. M. Chieu, N. T. Duong, Vo Van Hoang, and T. B. Van. "Local Structure of Amorphous Canonical Systems." Journal of Metastable and Nanocrystalline Materials 2-6 (July 1999): 393–98. http://dx.doi.org/10.4028/www.scientific.net/jmnm.2-6.393.

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45

Hung, P. K., D. K. Belashchenko, V. M. Chieu, N. T. Duong, Vo Van Hoang, and T. B. Van. "Local Structure of Amorphous Canonical Systems." Materials Science Forum 312-314 (July 1999): 393–98. http://dx.doi.org/10.4028/www.scientific.net/msf.312-314.393.

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46

Hachiya, Kan. "Electronic structure of amorphous germanium sulphides." Journal of Non-Crystalline Solids 312-314 (October 2002): 566–69. http://dx.doi.org/10.1016/s0022-3093(02)01781-7.

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