Aperiodic crystal

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Cristal apériodique (Fr). Cristallo aperiodico (It). 非周期性結晶 (Ja)


A periodic crystal is a structure with, ideally, sharp diffraction peaks on the positions of a reciprocal lattice. The structure then is invariant under the translations of the direct lattice. Periodicity here means lattice periodicity. Any structure without this property is aperiodic. For example, an amorphous system is aperiodic. An aperiodic crystal is a structure with sharp diffraction peaks, but without lattice periodicity. Therefore, amorphous systems are not aperiodic crystals. The positions of the sharp diffraction peaks of an aperiodic crystal belong to a vector module of finite rank. This means that the diffraction wave vectors are of the form

\textbf{k}=\sum_{i=1}^n h_i \textbf{a}_i^*, ( \textrm{integer}\ h_i).

The basis vectors a_i^* are supposed to be independent over the rational numbers, i.e. when a linear combination of them with rational coefficients is zero, all coefficients are zero. The minimum number of basis vectors is the rank of the vector module. If the rank n is larger than the space dimension, the structure is not periodic, but aperiodic.


There are four classes of aperiodic structures, but these classes have an overlap:

  • incommensurately modulated crystal phases (See incommensurate modulated crystal phases),
  • incommensurate composite structures (See incommensurate composites),
  • quasicrystals (see quasicrystals),
  • and incommensurate magnetic structures (See incommensurate magnetic structures).

See also: Incommensurately modulated crystal phases, incommensurate composite structures, quasicrystals, incommensurate magnetic structures.