Hermann-Mauguin Scheme
Preferred by crystallographers, this notation can be easily extended to include translational symmetry elements and specifies the directions of the symmetry axes.
Base Operations
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Proper rotations: Described by the order of rotation: e.g., $n$-fold axis, represented as $n$.
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Reflections: Described by the symbol $m$. The direction is taken as normal to $m$.
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Inversion: Described by the symbol $i$ or $\bar{1}$.
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Roto-inversion: Described by the symbol $\bar{n}$ (where $n$ is the order of rotation).
Positional Hierarchy
H-M notations consist of at most three components, each referring to a different direction.
- First position: Rotation axis of highest order.
- Second position: Symmetrically equivalent secondary directions.
- Third position: Symmetrically equivalent tertiary directions passing between secondary directions.
Note: The position of $m$ indicates the direction of normal to the mirror plane.
Interactive H-M Derivation Tool
Select a point group target and construct its symmetry step-by-step. Enable secondary/tertiary positions to see cross-generated symmetry elements sequentially map the points.
Target Group
Cyan shapes: symmetry elements.
Black points: target pattern.
Your Construction
Live BuildOperations duplicate iteratively.
Blue points mapped live.
Construct H-M Notation
In summary..
Full symbol in H-M notations is built by the following process:
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Identify the symmetry axes that might work as primary, secondary or tertiary directions
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$n$ = proper rotation, $\bar{n}$ = improper rotation (roto-inversion) and $m$ = mirror
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Primary, secondary and tertiary directions must not be equivalent by symmetry
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Symmetry axes are arranged in decreasing order (except for $23$ and $\frac{2}{m}\bar{3}$ in tetrahedral groups to avoid confusion with dihedral groups $32$ ($D_3$) and $\bar{3}\frac{2}{m}$ ($D_{3d}$))
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Secondary direction exists when a symmetry element in a direction other than the primary direction exists
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Tertiary direction exists when a symmetry element other than that described by primary and secondary directions and one that is not equivalent by symmetry to primary and secondary directions exists
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Inversion never appears in any group symbol
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$\bar{n}$ does not necessarily imply that an $n$ axis and a mirror exist independently
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For $n$ = odd, $\bar{n}$ implies presence of both $n$ and $i$
Schoenflies $\leftrightarrow$ Hermann-Mauguin
Comprehensive mapping table comparing Schoenflies notation with rigorous, full Hermann-Mauguin point group symbols.
| S. No. | Schoenflies | H-M | S. No. | Schoenflies | H-M | S. No. | Schoenflies | H-M | S. No. | Schoenflies | H-M |
|---|---|---|---|---|---|---|---|---|---|---|---|
| 1 | $C_1 = E$ | 1 | 9 | $S_4$ | $\bar{4}$ | 17 | $C_{6h}$ | $\frac{6}{m}$ | 25 | $D_{3h}$ | $\bar{6}m2$ |
| 2 | $C_2 = D_1$ | 2 | 10 | $S_6$ | $\bar{3}$ | 18 | $D_2$ | 222 | 26 | $D_{4h}$ | $\frac{4}{m}\frac{2}{m}\frac{2}{m}$ |
| 3 | $C_3$ | 3 | 11 | $C_{2v}$ | $2mm = mm2$ | 19 | $D_3$ | 32 | 27 | $D_{6h}$ | $\frac{6}{m}\frac{2}{m}\frac{2}{m}$ |
| 4 | $C_4$ | 4 | 12 | $C_{3v}$ | $3m$ | 20 | $D_4$ | 422 | 28 | $T$ | 23 |
| 5 | $C_6$ | 6 | 13 | $C_{4v}$ | $4mm$ | 21 | $D_6$ | 622 | 29 | $T_h$ | $\frac{2}{m}\bar{3}$ |
| 6 | $C_i$ | $\bar{1}$ | 14 | $C_{6v}$ | $6mm$ | 22 | $D_{2d}$ | $\bar{4}2m$ | 30 | $T_d$ | $\bar{4}3m$ |
| 7 | $S_1 = C_s$ | $\bar{2} = m$ | 15 | $C_{2h}$ | $\frac{2}{m}$ | 23 | $D_{3d}$ | $\bar{3}\frac{2}{m}$ | 31 | $O$ | 432 |
| 8 | $S_3 = C_{3h}$ | $\bar{6} = \frac{3}{m}$ | 16 | $C_{4h}$ | $\frac{4}{m}$ | 24 | $D_{2h}$ | $\frac{2}{m}\frac{2}{m}\frac{2}{m}$ | 32 | $O_h$ | $\frac{4}{m}\bar{3}\frac{2}{m}$ |