**At-a-Glance**

*MedeA*^{®}[1] *Crystals* controls all crystal structure information as
specified by the lattice vectors in terms of their lengths and
the angles between them, the positions of the atoms in the
primitive unit cell in terms of their coordinates, and
the space-group symmetry.

**Key Benefits**

- Full control of all crystal structure information
- Symmetry-related atomic positions are automaticlly created
- Straightforward modification of initial magnetic moments and isotope masses
- Freezing of selected atomic coordinates to suppress atomic displacements in structure relaxations, molecular-dynamics simulations, and phonon calculations

The unique characteristic, which distinguishes crystals from all other
forms of matter, is discrete translational symmetry. This became
obvious from the early x-ray diffraction studies, which revealed that
most materials form almost perfect periodic arrays at low temperatures
[2]^{,}[3]. Of course, crystalline periodicity may be
viewed as a purely mathematical concept, and in this respect crystals
remind you of paintings of M. C. Escher such as that displayed in the figure above.

The mathematical perspective seamlessly leads to the classification of
crystals in terms of the well-known 14 Bravais lattices.
Each lattice point, *i.e.* each unit cell of the periodic
lattice, may comprise not just a single atom but a complex group of
atoms. This is just like the basic unit in the painting by Escher, shown in
the above figure, which consists of six lizards, two white, two red, and two
black.

On the theoretical side, translational
symmetry of a crystal ultimately originates from the corresponding symmetry of
the underlying potential generated by the atomic nuclei and seen by
the electrons. This led Bloch to formulate his famous theorem, which reduces
the problem of describing the electronic states in a macroscopic
crystal to that of electronic states in a microscopic unit cell and
thus forms the basis for electronic structure calculations using codes
like *MedeA VASP* [4].

*MedeA Crystals* controls all information about the Bravais lattice and
the internal arrangement of the atoms in the unit cell. This is done
by the basic graphical user interface displayed in the figure below. It
allows you to modify the lattice parameters and angles, to lower the
symmetry, *e.g.* prior to the insertion of symmetry-breaking defects,
and to modify the properties of the particular atoms.

The unique characteristic, which distinguishes crystals from all other forms of matter, is discrete translational symmetry.

As an example, the below figure displays the unit cell of FeS_{2}. It
crystallizes in a simple cubic lattice with space group Pa-3, which,
from a group-theoretical point of view, is exceptional among the 230
space groups [5]^{,}[6]. The arrangement of the atoms is
characterized by an FeS_{6} octahedron at the center of the
cube, which is rotated away from the Cartesian axes by about
23^{°}, as well as strongly bonded sulfur pairs oriented along
the <111> axis.

Finally, creation and modification of the crystal structure with *MedeA
Crystals* provides the basis for use with a large number of other tools
implemented in the computational *MedeA Environment*, such as *MedeA VASP*,
the *MedeA Interface Builder*, and the builder tools for surfaces,
supercells, and random substitutions.

- An intuitive user interface controls all parameters affecting the crystal structure, such as the lattice parameters and angles, the atomic positions, and the space group

- Three-dimensional crystal structure as specified by the length of the lattice vectors, the angle between them and the positions of the atoms in Cartesian and fractional coordinates.
- Initial magnetic moments and isotope masses
- Selected suppression of atomic displacements

*MedeA Environment*

Learn more about *MedeA Crystals* Builder from the Materials Design online video tutorial How to Create Vacancies and Substitutions in Bulk Materials.

[1] | MedeA and Materials Design are registered trademarks of Materials Design, Inc. |

[2] | W. Friedrich, P. Knipping, and M. Laue,
“Interferenz-Erscheinungen bei Röntgenstrahlen”,
Ann. Phys. 346, 971 (1912)
(DOI) |

[3] | W. H. Bragg and W. L. Bragg,
“The Reflexion of X-rays by Crystals”,
Proc. Royal Soc. Lond. A 88, 428 (1913)
(DOI) |

[4] | F. Bloch,
“Über die Quantenmechanik der Elektronen in Kristallgittern”,
Z. Phys. 52, 555 (1929)
(DOI) |

[5] | C. J. Bradley and A. P. Cracknell, “The Mathematical Theory of Symmetry in Solids”, (Clarendon Press, Oxford 1972) |

[6] | V. Eyert, K.-H. Höck, S. Fiechter, and H. Tributsch,
“Electronic structure of FeS_{2}: The crucial role of
electron-lattice interaction”,
Phys. Rev. B 57, 6350 (1998).
(DOI) |

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