Reduced cell
From Online Dictionary of Crystallography
Maille réduite (Fr). Cella ridotta (It). 既約単位胞 (Ja).
A primitive basis a, b, c is called a reduced basis if it is right-handed and if the components of the metric tensor satisfy the conditions below. Because of lattice symmetry there can be two or more possible orientations of the reduced basis in a given lattice but, apart from orientation, the reduced basis is unique.
The type of a cell depends on the sign of
[math]T = (\mathbf{a}\cdot\mathbf{b})(\mathbf{b}\cdot\mathbf{c})(\mathbf{c}\cdot\mathbf{a})[/math].
If T > 0, the cell is of type I, if T ≤ 0 it is of type II.
The conditions for a primitive cell to be a reduced cell can all be stated analytically as follows.
Contents
Type-I cell
Main conditions
- [math]\mathbf{a}\cdot\mathbf{a}[/math] ≤ [math]\mathbf{b}\cdot\mathbf{b}[/math] ≤ [math]\mathbf{c}\cdot\mathbf{c}[/math]
- [math]|\mathbf{b}\cdot\mathbf{c}|[/math] ≤ [math](\mathbf{b}\cdot\mathbf{b})/2[/math]
- [math]|\mathbf{a}\cdot\mathbf{c}|[/math] ≤ [math](\mathbf{a}\cdot\mathbf{a})/2[/math]
- [math]|\mathbf{a}\cdot\mathbf{b}|[/math] ≤ [math](\mathbf{a}\cdot\mathbf{a})/2[/math]
- [math]\mathbf{b}\cdot\mathbf{c} \gt 0[/math]
- [math]\mathbf{a}\cdot\mathbf{c} \gt 0[/math]
- [math]\mathbf{a}\cdot\mathbf{b} \gt 0[/math]
Special conditions
- if [math]\mathbf{a}\cdot\mathbf{a} = \mathbf{b}\cdot\mathbf{b}[/math] then [math]\mathbf{b}\cdot\mathbf{c}[/math] ≤ [math]\mathbf{a}\cdot\mathbf{c}[/math]
- if [math]\mathbf{b}\cdot\mathbf{b} = \mathbf{c}\cdot\mathbf{c}[/math] then [math]\mathbf{a}\cdot\mathbf{c}[/math] ≤ [math]\mathbf{a}\cdot\mathbf{b}[/math]
- if [math]\mathbf{b}\cdot\mathbf{c} = (\mathbf{b}\cdot\mathbf{b})[/math]/2 then [math]\mathbf{a}\cdot\mathbf{b}[/math] ≤ [math]2\mathbf{a}\cdot\mathbf{c}[/math]
- if [math] \mathbf{a}\cdot\mathbf{c} = (\mathbf{a}\cdot\mathbf{a})[/math]/2 then [math]\mathbf{a}\cdot\mathbf{b}[/math] ≤ [math]2\mathbf{b}\cdot\mathbf{c}[/math]
- if [math] \mathbf{a}\cdot\mathbf{b} = (\mathbf{a}\cdot\mathbf{a})[/math]/2 then [math]\mathbf{a}\cdot\mathbf{c}[/math] ≤ [math]2\mathbf{b}\cdot\mathbf{c}[/math]
Type-II cell
Main conditions
- [math]\mathbf{a}\cdot\mathbf{a}[/math] ≤ [math]\mathbf{b}\cdot\mathbf{b}[/math] ≤ [math]\mathbf{c}\cdot\mathbf{c}[/math]
- [math]|\mathbf{b}\cdot\mathbf{c}|[/math] ≤ [math](\mathbf{b}\cdot\mathbf{b})/2[/math]
- [math]|\mathbf{a}\cdot\mathbf{c}|[/math] ≤ [math](\mathbf{a}\cdot\mathbf{a})/2[/math]
- [math]|\mathbf{a}\cdot\mathbf{b}|[/math] ≤ [math](\mathbf{a}\cdot\mathbf{a})/2[/math]
- [math](|\mathbf{b}\cdot\mathbf{c}|+ |\mathbf{a}\cdot\mathbf{c}|+|\mathbf{a}\cdot\mathbf{b}|)[/math] ≤ [math](\mathbf{a}\cdot\mathbf{a}+\mathbf{b}\cdot\mathbf{b})/2[/math]
- [math]\mathbf{b}\cdot\mathbf{c}[/math] ≤ 0
- [math]\mathbf{a}\cdot\mathbf{c}[/math] ≤ 0
- [math]\mathbf{a}\cdot\mathbf{b}[/math] ≤ 0
Special conditions
- if [math]\mathbf{a}\cdot\mathbf{a} = \mathbf{b}\cdot\mathbf{b}[/math] then [math]|\mathbf{b}\cdot\mathbf{c}|[/math] ≤ [math]|\mathbf{a}\cdot\mathbf{c}|[/math]
- if [math]\mathbf{b}\cdot\mathbf{b} = \mathbf{c}\cdot\mathbf{c}[/math] then [math]|\mathbf{a}\cdot\mathbf{c}|[/math] ≤ [math]|\mathbf{a}\cdot\mathbf{b}|[/math]
- if [math]|\mathbf{b}\cdot\mathbf{c}| = (\mathbf{b}\cdot\mathbf{b})/2[/math] then [math]\mathbf{a}\cdot\mathbf{b} = 0[/math]
- if [math]|\mathbf{a}\cdot\mathbf{c}| = (\mathbf{a}\cdot\mathbf{a})[/math]/2 then [math]\mathbf{a}\cdot\mathbf{b} = 0[/math]
- if [math]\mathbf{a}\cdot\mathbf{b} = (\mathbf{a}\cdot\mathbf{a})[/math]/2 then [math]\mathbf{a}\cdot\mathbf{c} = 0[/math]
- if [math](|\mathbf{b}\cdot\mathbf{c}|+ |\mathbf{a}\cdot\mathbf{c}|+|\mathbf{a}\cdot\mathbf{b}|) = (\mathbf{a}\cdot\mathbf{a}+\mathbf{b}\cdot\mathbf{b})/2[/math] then [math]\mathbf{a}\cdot\mathbf{a}[/math] ≤ [math]2|\mathbf{a}\cdot\mathbf{c}|+ |\mathbf{a}\cdot\mathbf{b}|[/math]
Geometrical meaning of the reduced cell
The main conditions express the following two requirements:
- Of all lattice vectors, none is shorter than a; of those not directed along a, none is shorter than b; of those not lying in the ab plane, none is shorter than c.
- The three angles between basis vectors are either all acute (type I) or all non-acute (type II).
See also
- Conventional cell
- Crystallographic basis
- Direct lattice
- Unit cell
- Chapter 3.1.3. of International Tables for Crystallography, Volume A, 6th edition