Paracrystallinity

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Paracrystalline
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In materials science, paracrystalline materials are defined as having short- and medium-range ordering in their lattice (similar to the liquid crystal phases) but lacking crystal-like long-range ordering at least in one direction.[1]

Origin and definition

The words "paracrystallinity" and "paracrystal" were coined by the late Friedrich Rinne in the year 1933.[2] Their German equivalents, e.g. "Parakristall", appeared in print one year earlier.[3] A general theory of paracrystals has been formulated in a basic textbook,[4] and then further developed/refined by various authors.

Rolf Hosemann's definition of an ideal paracrystal is: "The electron density distribution of any material is equivalent to that of a paracrystal when there is for every building block one ideal point so that the distance statistics to other ideal points are identical for all of these points. The electron configuration of each building block around its ideal point is statistically independent of its counterpart in neighboring building blocks. A building block corresponds then to the material content of a cell of this "blurred" space lattice, which is to be considered a paracrystal."[5]

Theory

Ordering is the regularity in which atoms appear in a predictable lattice, as measured from one point. In a highly ordered, perfectly crystalline material, or

correlation
length . A paracrystalline material exhibits a correlation somewhere between the fully amorphous and fully crystalline.

The primary, most accessible source of crystallinity information is X-ray diffraction and cryo-electron microscopy,[6] although other techniques may be needed to observe the complex structure of paracrystalline materials, such as fluctuation electron microscopy[7] in combination with density of states modeling[8] of electronic and vibrational states. Scanning transmission electron microscopy can provide real-space and reciprocal space characterization of paracrystallinity in nanoscale material, such as quantum dot solids.[9]

The scattering of X-rays, neutrons and electrons on paracrystals is quantitatively described by the theories of the ideal[10] and real[11] paracrystal.

Numerical differences in analyses of diffraction experiments on the basis of either of these two theories of paracrystallinity can often be neglected.[12]

Just like ideal crystals, ideal paracrystals extend theoretically to infinity. Real paracrystals, on the other hand, follow the empirical α*-law,[13] which restricts their size. That size is also indirectly proportional to the components of the tensor of the paracrystalline distortion. Larger solid state aggregates are then composed of micro-paracrystals.[14]

Applications

The paracrystal model has been useful, for example, in describing the state of partially amorphous semiconductor materials after deposition. It has also been successfully applied to synthetic polymers, liquid crystals, biopolymers, quantum dot solids, and biomembranes.[15]

See also

References

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  2. ^ F. Rinne, Investigations and considerations concerning paracrystallinity, Transactions of the Faraday Society 29 (1933) 1016–1032
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  5. ^ R. Hosemann, Der ideale Parakristall und die von ihm gestreute kohaerente Roentgenstrahlung, Zeitschrift für Physik 128 (1950) 465–492
  6. PMID 19805028
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  9. PMID 27540863.{{cite journal}}: CS1 maint: multiple names: authors list (link
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  11. ^ R. Hosemann: Grundlagen der Theorie des Parakristalls und ihre Anwendungensmöglichkeiten bei der Untersuchung der Realstruktur kristalliner Stoffe, Kristall und Technik, Band 11, 1976, S. 1139–1151
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  13. ^ Hosemann, R.; Hentschel, M. P.; Balta-Calleja, F. J.; Cabarcos, E. Lopez; Hindeleh, A. M. (2001). "The α*-constant, equilibrium state and bearing netplanes in polymers, biopolymers and catalysts". Journal of Physics C: Solid State Physics. 18 (5): 249–254.
  14. S2CID 135930955
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  15. ^ Baianu I.C. (1978). "X-ray scattering by partially disordered membrane systems". Acta Crystallogr. A. 34 (5): 751–753. .