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1

Wood, R. M. "Defects and Defect Processes in Nonmetallic Solids." Physics Bulletin 37, no. 12 (1986): 503. http://dx.doi.org/10.1088/0031-9112/37/12/037.

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2

Olemskoi, O. I., and I. O. Shuda. "Radiation Defects in Solids." Uspehi Fiziki Metallov 10, no. 1 (2009): 1–25. http://dx.doi.org/10.15407/ufm.10.01.001.

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3

Apostol, M. "On Defects in Solids." Journal of Physical Chemistry 100, no. 35 (1996): 14835–36. http://dx.doi.org/10.1021/jp960820r.

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4

Mao, Sheng, and Prashant K. Purohit. "Defects in flexoelectric solids." Journal of the Mechanics and Physics of Solids 84 (November 2015): 95–115. http://dx.doi.org/10.1016/j.jmps.2015.07.013.

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5

Kornyushin, Yuri. "Inhomogeneously distributed defects in solids." Materials Chemistry and Physics 67, no. 1-3 (2001): 6–11. http://dx.doi.org/10.1016/s0254-0584(00)00412-0.

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6

Serre, Christian. "Defects visualized in porous solids." Nature 493, no. 7432 (2013): 313–14. http://dx.doi.org/10.1038/493313a.

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7

Martin, David C., Patricia M. Wilson, Jun Liao, and Marie-Christine G. Jones. "Chain-End Defects in Extended-Chain Polymer Solids." MRS Bulletin 20, no. 9 (1995): 47–51. http://dx.doi.org/10.1557/s088376940003493x.

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Understanding the influence of local variations in symmetry (“defects”) on the macroscopic properties of polymers in the condensed state is an ongoing experimental and theoretical challenge. Studies of defects in solids require the most information-intensive description of microstructure since it is not possible to describe a “defect” without understanding the morphology of the majority phase as well.The nature of defects in polymers has been discussed elsewhere, including other articles in this issue of the MRS Bulletin. The structure, properties, and mobility of defects in polymers are all p
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8

Ourmazd, A., M. Scheffler, M. Heinemann, and J.-L. Rouviere. "Microscopic Properties of Thin Films: Learning About Point Defects." MRS Bulletin 17, no. 12 (1992): 24–32. http://dx.doi.org/10.1557/s0883769400046923.

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Microscopic properties of thin films are often strongly influenced by departures from “perfection.” These can take the form of extended defects such as dislocations, interfacial roughness, or point defects. Direct imaging of extended defects was one of the early contributions of electron microscopy to solid-state science. Since then, the role of extended defects in controlling the fabrication and properties of thin films has been extensively studied and reviewed. Recently, in-situ observation of strain relaxation in thin-film structures has increased our understanding of dislocation kinetics a
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9

Street, R. "Defects and processes in nonmetallic solids." IEEE Journal of Quantum Electronics 22, no. 5 (1986): 739. http://dx.doi.org/10.1109/jqe.1986.1073029.

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10

Tadmor, E. B., M. Ortiz, and R. Phillips. "Quasicontinuum analysis of defects in solids." Philosophical Magazine A 73, no. 6 (1996): 1529–63. http://dx.doi.org/10.1080/01418619608243000.

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11

Smith, John R. "Quantum thermodynamics of defects in solids." Physical Review Letters 70, no. 18 (1993): 2774–77. http://dx.doi.org/10.1103/physrevlett.70.2774.

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12

Goworek, T. "Defects in Molecular Solids. Positron Studies." Physica Status Solidi (a) 102, no. 2 (1987): 511–26. http://dx.doi.org/10.1002/pssa.2211020206.

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13

Chertova, N. V. "Wave processes in solids with defects." Journal of Applied Mechanics and Technical Physics 49, no. 6 (2008): 1047–54. http://dx.doi.org/10.1007/s10808-008-0129-9.

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14

Kléman, M. "Defects in Liquid-Crystalline Polymers." MRS Bulletin 20, no. 9 (1995): 23–28. http://dx.doi.org/10.1557/s0883769400034898.

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The properties of imperfections (or defects) of the atomic or molecular order in condensed matter can be conveniently described under two headings: (1) Topological properties—Defects break a specific symmetry of the ordered system at a local scale, that is, along a point defect, a line defect (a dislocation or a disclination), or a surface defect (a wall). (2) Elastic properties—Defects are sources of two types of distortions of the order: long-range distortions, which depend crucially on the broken symmetry but also on the material constants, and short-range distortions in the “core” region o
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15

Yavari, Arash, and Alain Goriely. "Weyl geometry and the nonlinear mechanics of distributed point defects." Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 468, no. 2148 (2012): 3902–22. http://dx.doi.org/10.1098/rspa.2012.0342.

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The residual stress field of a nonlinear elastic solid with a spherically symmetric distribution of point defects is obtained explicitly using methods from differential geometry. The material manifold of a solid with distributed point defects—where the body is stress-free—is a flat Weyl manifold, i.e. a manifold with an affine connection that has non-metricity with vanishing traceless part, but both its torsion and curvature tensors vanish. Given a spherically symmetric point defect distribution, we construct its Weyl material manifold using the method of Cartan's moving frames. Having the mat
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16

Stoneham, A. M. "Theory of Solid-State Defects." MRS Bulletin 16, no. 12 (1991): 22–26. http://dx.doi.org/10.1557/s0883769400055305.

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Serious studies of materials are often serious studies of defects, for control of properties of materials implies control of defects or impurities. Understanding defect phenomena is crucial, and both theoretical ideas and modeling are enhancing key areas of materials properties and processing. I shall review some of the ways theory contributes. Theory enters into all aspects of materials science, even if you don't always realize you are using it.Even self-styled practical people, for whom theory is a luxury, use theory routinely in its first main role, as a framework for the data they lovingly
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17

Mueller, R., D. Gross, T. Rangelov, and P. Dineva. "Dynamic fracture of piezoelectric solids with defects." Procedia Engineering 10 (2011): 76–81. http://dx.doi.org/10.1016/j.proeng.2011.04.015.

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18

de Padua, A., Fernando Parisio-Filho, and Fernando Moraes. "Geodesics around line defects in elastic solids." Physics Letters A 238, no. 2-3 (1998): 153–58. http://dx.doi.org/10.1016/s0375-9601(97)00871-2.

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19

Myers, S. M., M. I. Baskes, H. K. Birnbaum, et al. "Hydrogen interactions with defects in crystalline solids." Reviews of Modern Physics 64, no. 2 (1992): 559–617. http://dx.doi.org/10.1103/revmodphys.64.559.

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20

Harding, J. H. "Computer simulation of defects in ionic solids." Reports on Progress in Physics 53, no. 11 (1990): 1403–66. http://dx.doi.org/10.1088/0034-4885/53/11/002.

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21

Cherepanov, G. P. "The motion of point defects in solids." Journal of Applied Mathematics and Mechanics 50, no. 3 (1986): 380–88. http://dx.doi.org/10.1016/0021-8928(86)90136-x.

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22

Mosseri, Rémy, and Jean-François Sadoc. "Frustration and defects in non-periodic solids." Comptes Rendus Physique 15, no. 1 (2014): 90–99. http://dx.doi.org/10.1016/j.crhy.2013.09.006.

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23

Ericksen, J. L. "Some surface defects in unstressed thermoelastic solids." Archive for Rational Mechanics and Analysis 88, no. 4 (1985): 337–45. http://dx.doi.org/10.1007/bf00250870.

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24

Ziatdinov, Maxim, Ondrej Dyck, Xin Li, et al. "Building and exploring libraries of atomic defects in graphene: Scanning transmission electron and scanning tunneling microscopy study." Science Advances 5, no. 9 (2019): eaaw8989. http://dx.doi.org/10.1126/sciadv.aaw8989.

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The presence and configurations of defects are primary components determining materials functionality. Their population and distribution are often nonergodic and dependent on synthesis history, and therefore rarely amenable to direct theoretical prediction. Here, dynamic electron beam–induced transformations in Si deposited on a graphene monolayer are used to create libraries of possible Si and carbon vacancy defects. Deep learning networks are developed for automated image analysis and recognition of the defects, creating a library of (meta) stable defect configurations. Density functional th
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25

Gali, Adam. "Defects in SiC: Theory." Materials Science Forum 679-680 (March 2011): 225–32. http://dx.doi.org/10.4028/www.scientific.net/msf.679-680.225.

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A brief overview about the recent progress in developing the methods to calculate the properties of defects in solids is given and some recent examples on vacancy-related defects in SiC are presented.
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26

Yoffe, A. D. "Theory of Defects in Solids: Electronic Structure Defects in Insulators and Semiconductors." Physics Bulletin 37, no. 6 (1986): 266–67. http://dx.doi.org/10.1088/0031-9112/37/6/029.

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27

Pantelides, Sokrates T., D. Maroudas, and D. B. Laks. "Defects in Heterogeneous Solids - From Microphysics to Macrophysics." Materials Science Forum 143-147 (October 1993): 1–8. http://dx.doi.org/10.4028/www.scientific.net/msf.143-147.1.

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28

Savvatimskiy, A. I. "Nonequilibrium Defects upon the Pulsed Heating of Solids." Bulletin of the Russian Academy of Sciences: Physics 82, no. 4 (2018): 359–62. http://dx.doi.org/10.3103/s1062873818040172.

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29

Vinetskii, V. L., Yu Kh Kalnin', E. A. Kotomin, and A. A. Ovchinnikov. "Radiation-stimulated aggregation of Frenkel defects in solids." Uspekhi Fizicheskih Nauk 160, no. 10 (1990): 1. http://dx.doi.org/10.3367/ufnr.0160.199010a.0001.

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30

Ariza, Pilar, Michael Ortiz, and Viggo Tvergaard. "IUTAM symposium on micromechanics of defects in solids." Mechanics of Materials 90 (November 2015): 1. http://dx.doi.org/10.1016/j.mechmat.2015.05.009.

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31

Kunz, A. Barry, and Donald R. Beck. "Possible role of charged defects in molecular solids." Physical Review B 36, no. 14 (1987): 7580–85. http://dx.doi.org/10.1103/physrevb.36.7580.

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32

MacKay, R. S. "Defects in solids, large molecules and space structures." Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences 456, no. 2000 (2000): 1883–95. http://dx.doi.org/10.1098/rspa.2000.0592.

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33

Vinetskiĭ, V. L., Yu Kh Kalnin', E. A. Kotomin, and A. A. Ovchinnikov. "Radiation-stimulated aggregation of Frenkel defects in solids." Soviet Physics Uspekhi 33, no. 10 (1990): 793–811. http://dx.doi.org/10.1070/pu1990v033n10abeh002634.

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34

Dereli, T., and A. Verçin. "A gauge model of amorphous solids containing defects." Philosophical Magazine B 56, no. 5 (1987): 625–31. http://dx.doi.org/10.1080/13642818708220167.

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35

Xu, X. L., and R. K. N. D. Rajapakse. "Boundary element analysis of piezoelectric solids with defects." Composites Part B: Engineering 29, no. 5 (1998): 655–69. http://dx.doi.org/10.1016/s1359-8368(98)00022-5.

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36

Kröner, E. "The internal mechanical state of solids with defects." International Journal of Solids and Structures 29, no. 14-15 (1992): 1849–57. http://dx.doi.org/10.1016/0020-7683(92)90176-t.

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37

Freysoldt, Christoph, Blazej Grabowski, Tilmann Hickel, et al. "First-principles calculations for point defects in solids." Reviews of Modern Physics 86, no. 1 (2014): 253–305. http://dx.doi.org/10.1103/revmodphys.86.253.

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38

Mura, R., and T. C. T. Ting. "Micromechanics of Defects in Solids (2nd rev. ed.)." Journal of Applied Mechanics 56, no. 2 (1989): 487–88. http://dx.doi.org/10.1115/1.3176116.

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39

Fan, Hui, and Leon M. Keer. "Two-dimensional line defects in anisotropic elastic solids." International Journal of Fracture 62, no. 1 (1993): 25–42. http://dx.doi.org/10.1007/bf00032523.

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40

Gai-Boyes, Pratibha L. "Structural Evolution of Extended Defects in Nonstoichiometric Solids." Journal of Solid State Chemistry 104, no. 1 (1993): 119–30. http://dx.doi.org/10.1006/jssc.1993.1146.

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41

Meltzer, R. S., K. W. Jang, Kug Sun Hong, Y. Sun, and S. P. Feofilov. "Defects and Optical Dephasing of Ions in Solids." Materials Science Forum 239-241 (January 1997): 207–12. http://dx.doi.org/10.4028/www.scientific.net/msf.239-241.207.

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42

Wijtmans, Sven, and M. Lisa Manning. "Disentangling defects and sound modes in disordered solids." Soft Matter 13, no. 34 (2017): 5649–55. http://dx.doi.org/10.1039/c7sm00792b.

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Adding an artificial potential to simulations of disordered solids isolates localized excitations from phonon-like modes in the vibrational spectrum. These structural defects predict locations and displacements in particle rearrangements.
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43

Grinyaev, Yu V., and N. V. Chertova. "Dynamic theory of defects and creep in solids." Technical Physics Letters 26, no. 8 (2000): 723–25. http://dx.doi.org/10.1134/1.1307825.

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44

Ruffoni, Davide, John William Chapman Dunlop, Peter Fratzl, and Richard Weinkamer. "Effect of minimal defects in periodic cellular solids." Philosophical Magazine 90, no. 13 (2010): 1807–18. http://dx.doi.org/10.1080/14786430903571404.

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45

Selvadurai, A. P. S. "Bridged defects in continuously and discretely reinforced solids." Journal of Engineering Mathematics 95, no. 1 (2015): 359–80. http://dx.doi.org/10.1007/s10665-014-9779-1.

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46

Voevodin, V. G., and V. E. Stepanov. "Interaction of ultrasound with macroscopic defects in solids." Russian Physics Journal 37, no. 11 (1994): 1013–17. http://dx.doi.org/10.1007/bf00559208.

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47

Vanpoucke, Danny E. P. "Partitioning the vibrational spectrum: Fingerprinting defects in solids." Computational Materials Science 181 (August 2020): 109736. http://dx.doi.org/10.1016/j.commatsci.2020.109736.

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48

Mansur, L. K. "Defect reactions and clustering in irradiated solids." Canadian Journal of Physics 68, no. 9 (1990): 887–905. http://dx.doi.org/10.1139/p90-126.

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Irradiation of solid materials with energetic neutrons or charged particles can lead to profound changes in defect structure, microcomposition, and macroscopic properties. Such changes occur by atomic and microstructural mechanisms, some of which are familiar in "classical" physical metallurgy and materials science. However, other cases appear to be unique to irradiation. Irradiation has considerably broadened and indeed provided an entirely new dimension in materials science, since the energetic displacement of atoms potentially reaches to every property or process. The initial damaging event
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49

Demouchy, Sylvie. "Defects in olivine." European Journal of Mineralogy 33, no. 3 (2021): 249–82. http://dx.doi.org/10.5194/ejm-33-249-2021.

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Abstract. Olivine, a ferromagnesian orthosilicate, is the most abundant mineral in Earth's upper mantle and is stable down to the olivine–wadsleyite phase transition, which defines the 410 km depth mantle transition zone. Olivine also occurs in crustal environments in metamorphic and hydrothermal rocks and is expected to be the major mineral constituent of the Martian and Venusian mantles. The olivine atomic structure is also used in materials science to manufacture lithium batteries. Like any other crystalline solid, including minerals, olivine never occurs with a perfect crystalline structur
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50

Bernstock-Kopaczyńska, E., and Magdalena Jabłońska. "Determination of Thermal Diffusivity and Influence of Defect Structure in Alloys Based on the Fe-Al System." Defect and Diffusion Forum 336 (March 2013): 129–34. http://dx.doi.org/10.4028/www.scientific.net/ddf.336.129.

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Alloys of the Fe-Al system are interesting due to occurrence of long-range order and many thermal vacancies at high temperature, which lead to not only significant hardening, but also cause changes of physical properties. High temperature diffusion is conditioned by structural defects in solids, such as vacancies, foreign atoms and dislocations influencing thermal characteristics of a solid solution, among others the thermal diffusivity coefficient. Measurement of thermal diffusivity was performed at room temperature using the laser flash method. For characterization of the defect structure, p
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