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Amorphous solid

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"Amorphous" redirects here. For other uses, see Amorphous (disambiguation).

In condensed matter physics and materials science, an amorphous solid (or non-crystalline solid) is a solid that lacks the long-range order that is characteristic of a crystal. The terms "glass" and "glassy solid" are sometimes used synonymously with amorphous solid; however, these terms refer specifically to amorphous materials that undergo a glass transition.[1] Examples of amorphous solids include glasses, metallic glasses, and certain types of plastics and polymers.[2][3]

Etymology

The term comes from the Greek a ("without"), and morphé ("shape, form").

Structure

Crystalline vs. amorphous solid

Amorphous materials have an internal structure consisting of interconnected structural blocks that can be similar to the basic structural units found in the corresponding crystalline phase of the same compound.[4] Unlike in crystalline materials, however, no long-range order exists. Amorphous materials therefore cannot be defined by a finite unit cell. Statistical methods, such as the atomic density function and radial distribution function, are more useful in describing the structure of amorphous solids.[1][3]

Glass is a commonly encountered example of amorphous solids.

Although amorphous materials lack long range order, they exhibit localized order on small length scales. Localized order in amorphous materials can be categorized as short or medium range order.[1] By convention, short range order extends only to the nearest neighbor shell, typically only 1-2 atomic spacings.[5] Medium range order is then defined as the structural organization extending beyond the short range order, usually by 1-2 nm.[5]

Fundamental properties of amorphous solids

Glass transition at high temperatures

The freezing from liquid state to amorphous solid - glass transition - is considered one of the very important and unsolved problems of physics.

Universal low-temperature properties of amorphous solids

At very low temperatures (below 1-10 K), large family of amorphous solids have various similar low-temperature properties. Although there are various theoretical models, neither glass transition nor low-temperature properties of glassy solids are well understood on the fundamental physics level.

Amorphous solids is an important area of condensed matter physics aiming to understand these substances at high temperatures of glass transition and at low temperatures towards absolute zero. From 1970s, low-temperature properties of amorphous solids were studied experimentally in great detail. [6] [7] For all of these substances, specific heat has a (nearly) linear dependence as a function of temperature, and thermal conductivity has nearly quadratic temperature dependence. These properties are conventionally called anomalous being very different from properties of crystalline solids.

On the phenomenological level, many of these properties were described by a collection of tunneling two-level systems.[8] [9] Nevertheless, the microscopic theory of these properties is still missing after more than 50 years of the research. [10]

Remarkably, a dimensionless quantity of internal friction is nearly universal in these materials. [11] This quantity is a dimensionless ratio (up to a numerical constant) of the phonon wavelength to the phonon mean free path. Since the theory of tunneling two-level states (TLSs) does not address the origin of the density of TLSs, this theory cannot explain the universality of internal friction, which in turn is proportional to the density of scattering TLSs. The theoretical significance of this important and unsolved problem was highlighted by Anthony Leggett. [12]


Nano-structured materials

Amorphous materials will have some degree of short-range order at the atomic-length scale due to the nature of intermolecular chemical bonding.[a] Furthermore, in very small crystals, short-range order encompasses a large fraction of the atoms; nevertheless, relaxation at the surface, along with interfacial effects, distorts the atomic positions and decreases structural order. Even the most advanced structural characterization techniques, such as X-ray diffraction and transmission electron microscopy, have difficulty distinguishing amorphous and crystalline structures at short-length scales.[13]

Characterization of amorphous solids

Due to the lack of long-range order, standard crystallographic techniques are often inadequate in determining the structure of amorphous solids.[14] A variety of electron, X-ray, and computation-based techniques have been used to characterize amorphous materials. Multi-modal analysis is very common for amorphous materials.

X-ray and neutron diffraction

Unlike crystalline materials which exhibit strong Bragg diffraction, the diffraction patterns of amorphous materials are characterized by broad and diffuse peaks.[15] As a result, detailed analysis and complementary techniques are required to extract real space structural information from the diffraction patterns of amorphous materials. It is useful to obtain diffraction data from both X-ray and neutron sources as they have different scattering properties and provide complementary data.[16] Pair distribution function analysis can be performed on diffraction data to determine the probability of finding a pair of atoms separated by a certain distance.[15] Another type of analysis that is done with diffraction data of amorphous materials is radial distribution function analysis, which measures the number of atoms found at varying radial distances away from an arbitrary reference atom.[17] From these techniques, the local order of an amorphous material can be elucidated.

X-ray absorption fine-structure spectroscopy

X-ray absorption fine-structure spectroscopy is an atomic scale probe making it useful for studying materials lacking in long range order. Spectra obtained using this method provide information on the oxidation state, coordination number, and species surrounding the atom in question as well as the distances at which they are found.[18]

Atomic electron tomography

The atomic electron tomography technique is performed in transmission electron microscopes capable of reaching sub-Angstrom resolution. A collection of 2D images taken at numerous different tilt angles is acquired from the sample in question, and then used to reconstruct a 3D image.[19] After image acquisition, a significant amount of processing must be done to correct for issues such as drift, noise, and scan distortion.[19] High quality analysis and processing using atomic electron tomography results in a 3D reconstruction of an amorphous material detailing the atomic positions of the different species that are present.

Fluctuation electron microscopy

Fluctuation electron microscopy is another transmission electron microscopy based technique that is sensitive to the medium range order of amorphous materials. Structural fluctuations arising from different forms of medium range order can be detected with this method.[20] Fluctuation electron microscopy experiments can be done in conventional or scanning transmission electron microscope mode.[20]

Computational techniques

Simulation and modeling techniques are often combined with experimental methods to characterize structures of amorphous materials. Commonly used computational techniques include density functional theory, molecular dynamics, and reverse Monte Carlo.[14]

Uses and observations

Amorphous thin films

Amorphous phases are important constituents of thin films. Thin films are solid layers of a few nanometres to tens of micrometres thickness that are deposited onto a substrate. So-called structure zone models were developed to describe the microstructure of thin films as a function of the homologous temperature (Th), which is the ratio of deposition temperature to melting temperature.[21][22] According to these models, a necessary condition for the occurrence of amorphous phases is that (Th) has to be smaller than 0.3. The deposition temperature must be below 30% of the melting temperature.[b][citation needed]

Superconductivity

Amorphous metals have low toughness, but high strength

Regarding their applications, amorphous metallic layers played an important role in the discovery of superconductivity in amorphous metals made by Buckel and Hilsch.[23][24] The superconductivity of amorphous metals, including amorphous metallic thin films, is now understood to be due to phonon-mediated Cooper pairing. The role of structural disorder can be rationalized based on the strong-coupling Eliashberg theory of superconductivity.[25]

Thermal protection

Amorphous solids typically exhibit higher localization of heat carriers compared to crystalline, giving rise to low thermal conductivity.[26] Products for thermal protection, such as thermal barrier coatings and insulation, rely on materials with ultralow thermal conductivity.[26]

Technological uses

Today, optical coatings made from TiO2, SiO2, Ta2O5 etc. (and combinations of these) in most cases consist of amorphous phases of these compounds. Much research is carried out into thin amorphous films as a gas separating membrane layer.[27] The technologically most important thin amorphous film is probably represented by a few nm thin SiO2 layers serving as isolator above the conducting channel of a metal-oxide semiconductor field-effect transistor (MOSFET). Also, hydrogenated amorphous silicon (Si:H) is of technical significance for thin-film solar cells.[c][28]

Pharmaceutical use

In the pharmaceutical industry, some amorphous drugs have been shown to offer higher bioavailability than their crystalline counterparts as a result of the higher solubility of the amorphous phase. However, certain compounds can undergo precipitation in their amorphous form in vivo, and can then decrease mutual bioavailability if administered together.[29][30]

In soils

Amorphous materials in soil strongly influence bulk density, aggregate stability, plasticity, and water holding capacity of soils. The low bulk density and high void ratios are mostly due to glass shards and other porous minerals not becoming compacted. Andisol soils contain the highest amounts of amorphous materials.[31]

Phase

The occurrence of amorphous phases turned out to be a phenomenon of particular interest for the studying of thin-film growth.[32] The growth of polycrystalline films is often used and preceded by an initial amorphous layer, the thickness of which may amount to only a few nm. The most investigated example is represented by the unoriented molecules of thin polycrystalline silicon films.[d][33] Wedge-shaped polycrystals were identified by transmission electron microscopy to grow out of the amorphous phase only after the latter has exceeded a certain thickness, the precise value of which depends on deposition temperature, background pressure, and various other process parameters. The phenomenon has been interpreted in the framework of Ostwald's rule of stages[34] that predicts the formation of phases to proceed with increasing condensation time towards increasing stability.[24][33][e]

Notes

  1. ^ See the structure of liquids and glasses for more information on non-crystalline material structure.
  2. ^ For higher values, the surface diffusion of deposited atomic species would allow for the formation of crystallites with long-range atomic order.
  3. ^ In the case of a hydrogenated amorphous silicon, the missing long-range order between silicon atoms is partly induced by the presence of hydrogen in the percent range.
  4. ^ An initial amorphous layer was observed in many studies of thin polycrystalline silicon films.
  5. ^ Experimental studies of the phenomenon require a clearly defined state of the substrate surface—and its contaminant density, etc.—upon which the thin film is deposited.

References

  1. ^ a b c Thorpe., M.F.; Tichy, L. (2001). Properties and Applications of Amorphous Materials (1st ed.). Springer Dordrecht. pp. 1–11. ISBN 978-0-7923-6811-3.
  2. ^ Ponçot, M.; Addiego, F.; Dahoun, A. (2013-01-01). "True intrinsic mechanical behaviour of semi-crystalline and amorphous polymers: Influences of volume deformation and cavities shape". International Journal of Plasticity. 40: 126–139. doi:10.1016/j.ijplas.2012.07.007. ISSN 0749-6419.
  3. ^ a b Zaccone, A. (2023). Theory of Disordered Solids. Lecture Notes in Physics. Vol. 1015 (1st ed.). Springer. doi:10.1007/978-3-031-24706-4. ISBN 978-3-031-24705-7. S2CID 259299183.
  4. ^ Mavračić, Juraj; Mocanu, Felix C.; Deringer, Volker L.; Csányi, Gábor; Elliott, Stephen R. (2018). "Similarity Between Amorphous and Crystalline Phases: The Case of TiO2". J. Phys. Chem. Lett. 9 (11): 2985–2990. doi:10.1021/acs.jpclett.8b01067. PMID 29763315.
  5. ^ a b Cheng, Y. Q.; Ma, E. (2011-05-01). "Atomic-level structure and structure–property relationship in metallic glasses". Progress in Materials Science. 56 (4): 379–473. doi:10.1016/j.pmatsci.2010.12.002. ISSN 0079-6425.
  6. ^ Stephens, Robert B.; Liu, Xiao (2021). Low-Energy Excitations in Disordered Solids. A Story of the 'Universal' Phenomena of Structural Tunneling. doi:10.1142/11746. ISBN 978-981-12-1724-1. S2CID 224844997.
  7. ^ Grushin, Adolfo G. (2022). Ramos, M. (ed.). Low-Temperature Thermal and Vibrational Properties of Disordered Solids. A Half-Century of Universal "Anomalies" of Glasses. arXiv:2010.02851. doi:10.1142/q0371. ISBN 978-1-80061-257-0. S2CID 222140882.
  8. ^ Anderson, P.W.; Halperin, B.I.; Varma, C.M (1972). "Anomalous low-temperature thermal properties of glasses and spin glasses". Philosophical Magazine. 25 (1): 1–9. Bibcode:1972PMag...25....1A. doi:10.1080/14786437208229210.
  9. ^ Phillips, W.A. (1972). "Tunneling states in amorphous solids". J. Low Temp. Phys., Pp 751. 7 (3–4): 351–360. Bibcode:1972JLTP....7..351P. doi:10.1007/BF00660072. S2CID 119873202.
  10. ^ Esquinazi, Pablo, ed. (1998). Tunneling Systems in Amorphous and Crystalline Solids. doi:10.1007/978-3-662-03695-2. ISBN 978-3-642-08371-6.
  11. ^ Pohl, R.O.; etc, etc (2002). "Low-temperature thermal conductivity and acoustic attenuation in amorphous solids". Revs. Mod Phys. 74 (1): 991. Bibcode:1972PMag...25....1A. doi:10.1080/14786437208229210.
  12. ^ Leggett, A.J. (1991). "Amorphous materials at low temperatures: why are they so similar?". Physica B. 169 (1–4): 322–327. Bibcode:1991PhyB..169..322L. doi:10.1016/0921-4526(91)90246-B.
  13. ^ Goldstein, Joseph I.; Newbury, Dale E.; Michael, Joseph R.; Ritchie, Nicholas W. M.; Scott, John Henry J.; Joy, David C. (2018). Scanning Electron Microscopy and X-ray Microanalysis (Fourth ed.). New York, NY. ISBN 978-1493966745.{{cite book}}: CS1 maint: location missing publisher (link)
  14. ^ a b Yang, Yao; Zhou, Jihan; Zhu, Fan; Yuan, Yakun; Chang, Dillan J.; Kim, Dennis S.; Pham, Minh; Rana, Arjun; Tian, Xuezeng; Yao, Yonggang; Osher, Stanley J.; Schmid, Andreas K.; Hu, Liangbing; Ercius, Peter; Miao, Jianwei (March 31, 2021). "Determining the three-dimensional atomic structure of an amorphous solid". Nature. 592 (7852): 60–64. arXiv:2004.02266. Bibcode:2021Natur.592...60Y. doi:10.1038/s41586-021-03354-0. ISSN 1476-4687. PMID 33790443. S2CID 214802235.
  15. ^ a b Billinge, Simon J. L. (2019-06-17). "The rise of the X-ray atomic pair distribution function method: a series of fortunate events". Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences. 377 (2147): 20180413. Bibcode:2019RSPTA.37780413B. doi:10.1098/rsta.2018.0413. PMC 6501893. PMID 31030657.
  16. ^ Ren, Yang; Zuo, Xiaobing (2018-06-13). "Synchrotron X‐Ray and Neutron Diffraction, Total Scattering, and Small‐Angle Scattering Techniques for Rechargeable Battery Research". Small Methods. 2 (8): 1800064. doi:10.1002/smtd.201800064. ISSN 2366-9608. OSTI 1558997. S2CID 139693137.
  17. ^ Senjaya, Deriyan; Supardi, Adri; Zaidan, Andi (2020-12-09). "Theoretical formulation of amorphous radial distribution function based on wavelet transformation". AIP Conference Proceedings. 2314 (1): 020001. Bibcode:2020AIPC.2314b0001S. doi:10.1063/5.0034410. ISSN 0094-243X. S2CID 234542087.
  18. ^ Newville, Matthew (July 22, 2004). "Fundamentals of XAFS" (PDF).
  19. ^ a b Zhou, Jihan; Yang, Yongsoo; Ercius, Peter; Miao, Jianwei (April 9, 2020). "Atomic electron tomography in three and four dimensions". MRS Bulletin. 45 (4): 290–297. Bibcode:2020MRSBu..45..290Z. doi:10.1557/mrs.2020.88. ISSN 0883-7694. S2CID 216408488.
  20. ^ a b Voyles, Paul; Hwang, Jinwoo (2012-10-12), Kaufmann, Elton N. (ed.), "Fluctuation Electron Microscopy", Characterization of Materials, Hoboken, NJ, USA: John Wiley & Sons, Inc., pp. com138, doi:10.1002/0471266965.com138, ISBN 978-0-471-26696-9, retrieved 2022-12-07
  21. ^ Movchan, B. A.; Demchishin, A. V. (1969). "Study of the Structure and Properties of Thick Vacuum Condensates of Nickel, Titanium, Tungsten, Aluminium Oxide and Zirconium Dioxide". Phys. Met. Metallogr. 28: 83–90.
    Russian-language version: Fiz. Metal Metalloved (1969) 28: 653-660.
  22. ^ Thornton, John A. (1974), "Influence of Apparatus Geometry and Deposition Conditions on the Structure and Topography of Thick Sputtered Coatings", Journal of Vacuum Science and Technology, 11 (4): 666–670, Bibcode:1974JVST...11..666T, doi:10.1116/1.1312732
  23. ^ Buckel, W.; Hilsch, R. (1956). "Supraleitung und elektrischer Widerstand neuartiger Zinn-Wismut-Legierungen". Z. Phys. 146 (1): 27–38. Bibcode:1956ZPhy..146...27B. doi:10.1007/BF01326000. S2CID 119405703.
  24. ^ a b Buckel, W. (1961). "The influence of crystal bonds on film growth". Elektrische en Magnetische Eigenschappen van dunne Metallaagies. Leuven, Belgium.
  25. ^ Baggioli, Matteo; Setty, Chandan; Zaccone, Alessio (2020). "Effective Theory of Superconductivity in Strongly Coupled Amorphous Materials". Physical Review B. 101 (21): 214502. arXiv:2001.00404. Bibcode:2020PhRvB.101u4502B. doi:10.1103/PhysRevB.101.214502. hdl:10486/703598. S2CID 209531947.
  26. ^ a b Zhou, Wu‐Xing; Cheng, Yuan; Chen, Ke‐Qiu; Xie, Guofeng; Wang, Tian; Zhang, Gang (September 9, 2019). "Thermal Conductivity of Amorphous Materials". Advanced Functional Materials. 30 (8): 1903829. doi:10.1002/adfm.201903829. ISSN 1616-301X. S2CID 203143442.
  27. ^ de Vos, Renate M.; Verweij, Henk (1998). "High-Selectivity, High-Flux Silica Membranes for Gas Separation". Science. 279 (5357): 1710–1711. Bibcode:1998Sci...279.1710D. doi:10.1126/science.279.5357.1710. PMID 9497287.
  28. ^ "Hydrogenated Amorphous Silicon - an overview | ScienceDirect Topics". www.sciencedirect.com. Retrieved 2023-10-17.
  29. ^ Hsieh, Yi-Ling; Ilevbare, Grace A.; Van Eerdenbrugh, Bernard; Box, Karl J.; Sanchez-Felix, Manuel Vincente; Taylor, Lynne S. (2012-05-12). "pH-Induced Precipitation Behavior of Weakly Basic Compounds: Determination of Extent and Duration of Supersaturation Using Potentiometric Titration and Correlation to Solid State Properties". Pharmaceutical Research. 29 (10): 2738–2753. doi:10.1007/s11095-012-0759-8. ISSN 0724-8741. PMID 22580905. S2CID 15502736.
  30. ^ Dengale, Swapnil Jayant; Grohganz, Holger; Rades, Thomas; Löbmann, Korbinian (May 2016). "Recent Advances in Co-amorphous Drug Formulations". Advanced Drug Delivery Reviews. 100: 116–125. doi:10.1016/j.addr.2015.12.009. ISSN 0169-409X. PMID 26805787.
  31. ^ Encyclopedia of Soil Science. Marcel Dekker. pp. 93–94.
  32. ^ Magnuson, Martin; Andersson, Matilda; Lu, Jun; Hultman, Lars; Jansson, Ulf (2012). "Electronic Structure and Chemical Bonding of Amorphous Chromium Carbide Thin Films". J. Phys. Condens. Matter. 24 (22): 225004. arXiv:1205.0678. Bibcode:2012JPCM...24v5004M. doi:10.1088/0953-8984/24/22/225004. PMID 22553115. S2CID 13135386.
  33. ^ a b Birkholz, M.; Selle, B.; Fuhs, W.; Christiansen, S.; Strunk, H. P.; Reich, R. (2001). "Amorphous-crystalline phase transition during the growth of thin films: The case of microcrystalline silicon" (PDF). Phys. Rev. B. 64 (8): 085402. Bibcode:2001PhRvB..64h5402B. doi:10.1103/PhysRevB.64.085402. Archived (PDF) from the original on 2010-03-31.
  34. ^ Ostwald, Wilhelm (1897). "Studien über die Bildung und Umwandlung fester Körper" (PDF). Z. Phys. Chem. (in German). 22: 289–330. doi:10.1515/zpch-1897-2233. S2CID 100328323. Archived (PDF) from the original on 2017-03-08.

Further reading

  • R. Zallen (1969). The Physics of Amorphous Solids. Wiley Interscience.
  • S.R. Elliot (1990). The Physics of Amorphous Materials (2nd ed.). Longman.
  • A. Zaccone (2023). Theory of Disordered Solids. Springer.
  • N. Cusack (1969). The Physics of Structurally Disordered Matter: An Introduction. IOP Publishing.
  • N.H. March; R.A. Street; M.P. Tosi, eds. (1969). Amorphous Solids and the Liquid State. Springer.
  • D.A. Adler; B.B. Schwartz; M.C. Steele, eds. (1969). Physical Properties of Amorphous Materials. Springer.
  • A. Inoue; K. Hasimoto, eds. (1969). Amorphous and Nanocrystalline Materials. Springer.


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