Crystal Symmetry Groups PDF

Summary

This document details crystal symmetry groups, covering point and space groups and their corresponding symmetry operations. It explains macroscopic properties, including conductivity, and their dependence on crystal direction, as well as different symmetry operations. It also shows how to describe and classify crystal symmetries and how to represent different classes of symmetry operations graphically.

Full Transcript

## Chap 2: Groupes ponctuels de symétrie et groupes d'espace ### Introduction - The macroscopic properties of a crystal depend generally on direction, for example : conductivity, electrical susceptibility, piezoelectricity etc. - In certain equivalent directions, one can find the same macroscopic...

## Chap 2: Groupes ponctuels de symétrie et groupes d'espace ### Introduction - The macroscopic properties of a crystal depend generally on direction, for example : conductivity, electrical susceptibility, piezoelectricity etc. - In certain equivalent directions, one can find the same macroscopic properties. ### Example : Conductivity - The conductivity is the same in the two equivalent directions **Δ** and **Δ'** for the same electric field strength **E**. - These directions can be obtained from one another by symmetry operations. ### Symmetry operations - **Symmetry operation:** A geometric operation that transforms an object into itself without any change. - **Point symmetry operations:** Leave at least one point fixed in the crystal. - They include rotations, inversions, roto-inversions (roto-inversion), and roto-reflections (roto-reflection). - The set of point symmetry operations of a crystal forms a **point group** also called **symmetry class**. - There are 32 different point groups. - **Symmetry of position:** The arrangement of atoms inside the crystal lattice. ### Example : Rotation helicoïdal (helicoïdal axis) - The set of symmetry operations combined with translation form a **space group**. - There are 230 space groups (or spatial groups). ### Notation Internationale de Hermann-Maugin (adopted in 1935) - **X:** Direct axis of order X. - **X:** Inverse axis of order X. - **Xm:** Direct axis of order X and a mirror perpendicular to X. - **Xm:** Direct axis of order X and a mirror containing X. - **X2:** Direct axis of order X and a direct axis of order 2 perpendicular to X. - **X3:** Direct axis of order X and a direct axis of order 3 making an angle of 54° with X. - **Xm:** Direct axis of order X, a mirror perpendicular to X, and a mirror containing X. ### Definition of a group - A group is a set of elements (symmetry operations) P, Q, R, S, T, .. that meet the following conditions: - **Closure:** If R ∈ G and S ∈ G then R·S = T, where T ∈ G. - **Associativity:** R·(S·T) = (R·S)·T. - **Neutral element:** G contains a neutral element E, such that ∀R∈G ; R·E = E·R = R. - **Inverse element:** For every element R ∈ G, there exists a corresponding inverse element R-1 ∈ G, such that: R-1·R = R·R-1 = E. - **Order of a group:** The number of elements in a group. ### Classification of point groups in crystal systems | Crystal system | Minimal symmetry | Point groups | Laue groups | |---|---|---|---| | Triclinic | 1 (or 1) | 1, 1 | 1 | | Monoclinic | One axis 2 (or 2 = m) | 2, m, 2/m | 2, m | | Orthorhombic | Three axes 2 (perpendicular) | 222, mm2, mmm | mmm | | Tetragonal | One axis 4 (or 4) | 4, 4, 4/m, 422, 4mm, 42m, mm | 4, 4/m, 4/mmm | | Trigonal (or Rhombohedral) | One axis 3 (or 3) | 3, 3, 32, 3m, ¯3m | 3, 3m | | Hexagonal | One axis 6 (or 6) | 6, 6, 6/m, 6mm, 622, 6m2, 6/mmm | 6, 6/m, 6/mmm | | Cubic | Four axes 3 (or 3) | 23, m3, 432, 43m | m3, m3m | ### Theorems - The combination of symmetry elements leads to the creation of new symmetry elements, such as: - **Theorem 1:** The presence of a two-fold axis and a center of symmetry implies the existence of a mirror plane perpendicular to the axis and passing through the center of symmetry. - It also implies the existence of a center of symmetry located at the intersection of the axis and the mirror plane. - **Theorem 2:** If there exists an n-fold axis and a mirror plane containing the axis, n mirror planes exist perpendicular to the axis and making angles of π/n between them. - **Theorem 3:** If there are n two-fold axes in a plane that intersect at a point, then the normal to that plane is an n-fold axis. - If there exists an n-fold axis and a two-fold axis perpendicular to it, then there exists n-1 additional two-fold axes, each making an angle of π/ n with the others. - **Theorem 4:** The existence of an inverse n-fold axis (n) implies specific existence conditions for various symmetry elements. ### Stereographic projection - This projection is a method for visualising the symmetry relations of a crystal. - The crystal is centered at the point **O** of a sphere. - The North Pole (PN) and South Pole (PS) are defined. - A normal to each crystal face is drawn through the center **O**. - The intersection of the normal with the sphere is labeled **P**. - The stereographic projection of **P** is the point **p** where the line connecting **P** and **PS** intersects the equatorial plane. - The image of a point **R** in the southern hemisphere is projected onto the equatorial plane via the line connecting **R** and **PN**. - The image of point **r** can be represented with a cross on the equatorial plane. ### Figures 2.3, 2.9, 2.10, 2.11: - These figures show examples of rotations, roto-reflections, roto-inversions, helicoïdal axes, and reflection with glide. ### Table of the 230 space groups - This table classifies all the space groups based on their crystal system, Hermann-Maugin notation, and their lattice type. ### Figure 15: - This figure shows examples of symmetry elements, such as 4-fold, 63-fold, 64-fold and 65-fold axes.

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