Crystalline Architectures
An in-depth exploration of the hexagonal crystal family, detailing its lattice systems, crystal systems, and associated structures.
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Lattice Systems
Defining the Framework
In crystallography, the hexagonal crystal family encompasses two fundamental lattice systems: the hexagonal and the rhombohedral. Each system is characterized by a unique arrangement of points in space that repeats periodically, forming the underlying structure of crystals.
Hexagonal Lattice
The hexagonal lattice system is defined by a unit cell with two equal axes (a = b) that are 120ยฐ apart (ฮณ = 120ยฐ), and a third axis (c) perpendicular to the plane of the other two. This system is represented by the Pearson symbol 'hP' for its primitive form.
Rhombohedral Lattice
The rhombohedral lattice system, denoted by 'hR', is characterized by a unit cell where all axes are equal in length (a = b = c) and all angles are equal but not 90ยฐ (ฮฑ = ฮฒ = ฮณ โ 90ยฐ). While it can be described using rhombohedral axes, it is conventionally represented by a hexagonal unit cell for practical crystallographic descriptions.
Crystal Systems
Trigonal System
The trigonal crystal system is defined by the presence of at least one threefold rotation axis. It comprises 5 point groups and is associated with 7 space groups. Notably, these space groups are distributed across both the rhombohedral (7 groups) and hexagonal (18 groups) lattice systems, making it unique among crystal systems.
Hexagonal System
The hexagonal crystal system is characterized by the presence of a single sixfold rotation axis. It includes 7 point groups and is exclusively associated with the hexagonal lattice system, comprising 27 distinct space groups. This system represents a higher degree of symmetry compared to the trigonal system.
Atomic Packing
Hexagonal Close-Packed (HCP)
Hexagonal close-packed (HCP) is one of the most efficient ways to pack identical spheres, achieving a packing density of approximately 74%. Unlike the face-centered cubic (FCC) structure, HCP is not a Bravais lattice. It can be constructed from the hexagonal Bravais lattice by associating a two-atom motif with each lattice point, resulting in a non-primitive unit cell.
Symmetry and Properties
The HCP structure, while highly dense, lacks inversion symmetry. This characteristic is crucial as it enables materials exhibiting this packing to possess properties such as piezoelectricity and pyroelectricity, which are absent in centrosymmetric crystal structures.
Multi-Element Structures
Wurtzite Structure
The Wurtzite structure (Strukturbericht designation B4, Pearson symbol hP4) is a common arrangement for binary compounds. It is based on the hexagonal Bravais lattice with a two-atom motif. Each atom is tetrahedrally coordinated. The space group is P63mc (No. 186). This structure is non-centrosymmetric, leading to piezoelectric properties.
Nickel Arsenide Structure
The Nickel Arsenide (NiAs) structure involves two interpenetrating sublattices: a primitive hexagonal Ni sublattice and a hexagonal close-packed As sublattice. Each Ni atom is octahedrally coordinated by six As atoms, while each As atom is trigonal prismatically coordinated by six Ni atoms. This structure is typical for transition metal chalcogenides, arsenides, and antimonides.
Two-Dimensional Lattices
The Single 2D Hexagonal Lattice
In two dimensions, the hexagonal crystal family is represented by a single Bravais lattice: the hexagonal lattice. This lattice is characterized by a unit cell with two equal axes at a 120ยฐ angle, forming a perfectly symmetrical hexagonal arrangement of points in a plane.
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References
References
- Inorganic Chemistry by Duward Shriver and Peter Atkins, 3rd Edition, W.H. Freeman and Company, 1999, pp.47,48.
- http://www.mindat.org/min-2901.html Mindat.org
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Important Notice
This content has been generated by an Artificial Intelligence, drawing upon established scientific literature and data, primarily sourced from Wikipedia. It is intended for educational and informational purposes at a postgraduate level. While efforts have been made to ensure accuracy and clarity, this material should not be considered a substitute for rigorous academic study or consultation with expert crystallographers or materials scientists.
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