Dihedral group: Difference between revisions

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{{short description|Group of symmetries of a regular polygon}}
{{short description|Group of symmetries of a regular polygon}}
{{more inline|date=April 2015}}
{{Group theory sidebar|Finite}}
{{Group theory sidebar|Finite}}
[[File:Snowflake8.png|thumb|The [[symmetry group]] of a [[snowflake]] is D<sub>6</sub>, a dihedral symmetry, the same as for a regular [[hexagon]].]]


In [[mathematics]], a '''dihedral group''' is the [[group (mathematics)|group]] of [[symmetry|symmetries]] of a [[regular polygon]],<ref>{{MathWorld|urlname=DihedralGroup|title=Dihedral Group}}</ref><ref>{{cite book | last1=Dummit | first1=David S. | last2=Foote | first2=Richard M. | title=Abstract Algebra | publisher=[[John Wiley & Sons]] | year=2004 | edition=3rd | isbn=0-471-43334-9}}</ref> which includes [[rotational symmetry|rotations]] and [[reflection symmetry|reflections]]. Dihedral groups are among the simplest examples of [[finite group]]s, and they play an important role in [[group theory]], [[geometry]], and [[chemistry]].<ref>{{cite book |last1=Fink |first1=Johannes Karl |title=Physical chemistry in depth |date=2009 |publisher=Springer-Verlag |location=Berlin Heidelberg |isbn=9783642010149 |page=417 |url=https://books.google.com/books?id=QMCNpXahcfcC&pg=PA417}}</ref>
In [[mathematics]], a '''dihedral group''' is the [[group (mathematics)|group]] of [[symmetry|symmetries]] of a [[regular polygon]],<ref>{{MathWorld|urlname=DihedralGroup|title=Dihedral Group}}</ref><ref>{{cite book | last1=Dummit | first1=David S. | last2=Foote | first2=Richard M. | title=Abstract Algebra | publisher=[[John Wiley & Sons]] | year=2004 | edition=3rd | isbn=0-471-43334-9}}</ref> which includes [[rotational symmetry|rotations]] and [[reflection symmetry|reflections]]. Dihedral groups are among the simplest examples of [[finite group]]s, and they play an important role in [[group theory]], [[geometry]], and [[chemistry]].<ref>{{cite book |last1=Fink |first1=Johannes Karl |title=Physical chemistry in depth |date=2009 |publisher=Springer-Verlag |location=Berlin Heidelberg |isbn=9783642010149 |page=417 |url=https://books.google.com/books?id=QMCNpXahcfcC&pg=PA417}}</ref>
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==Definition==
==Definition==
The word "dihedral" comes from "di-" and "-hedron".
The word "dihedral" comes from "di-" and "-hedron".
The latter comes from the  Greek word hédra, which means "face of a geometrical solid". Overall it thus refers to the two faces of a polygon.
The latter comes from the  Greek word hédra, which means "face of a geometrical solid". Overall, it thus refers to the two faces of a polygon.


===Elements===
===Elements===
[[File:Hexagon reflections.svg|thumb|The six axes of [[reflection symmetry|reflection]] of a regular hexagon]]
A regular polygon with <math>n</math> sides has <math>2n</math> different symmetries: <math>n</math> [[rotational symmetry|rotational symmetries]] and <math>n</math> [[reflection symmetry|reflection symmetries]]; here, <math>n \ge 3</math>. The associated [[rotation]]s and [[reflection (mathematics)|reflections]] make up the dihedral group <math>\mathrm{D}_n</math>. If <math>n</math> is odd, each axis of symmetry connects the midpoint of one side to the opposite vertex. If <math>n</math> is even, there are <math>n/2</math> axes of symmetry connecting the midpoints of opposite sides and <math>n/2</math> axes of symmetry connecting opposite vertices. In either case, there are <math>n</math> axes of symmetry and <math>2n</math> elements in the symmetry group.<ref name="cameron">{{citation
A regular polygon with <math>n</math> sides has <math>2n</math> different symmetries: <math>n</math> [[rotational symmetry|rotational symmetries]] and <math>n</math> [[reflection symmetry|reflection symmetries]]. Usually, we take <math>n \ge 3</math> here. The associated [[rotation]]s and [[reflection (mathematics)|reflections]] make up the dihedral group <math>\mathrm{D}_n</math>. If <math>n</math> is odd, each axis of symmetry connects the midpoint of one side to the opposite vertex. If <math>n</math> is even, there are <math>n/2</math> axes of symmetry connecting the midpoints of opposite sides and <math>n/2</math> axes of symmetry connecting opposite vertices. In either case, there are <math>n</math> axes of symmetry and <math>2n</math> elements in the symmetry group.<ref>{{citation
  | last = Cameron | first = Peter Jephson
  | last = Cameron | first = Peter Jephson
  | title = Introduction to Algebra
  | title = Introduction to Algebra
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  | page = 95
  | page = 95
  | url = https://books.google.com/books?id=syYYl-NVM5IC&pg=PA95
  | url = https://books.google.com/books?id=syYYl-NVM5IC&pg=PA95
}}</ref> Reflecting in one axis of symmetry followed by reflecting in another axis of symmetry produces a rotation through twice the angle between the axes.<ref>{{citation
}}</ref> Reflecting in one axis of symmetry followed by reflecting in another axis of symmetry produces a rotation through twice the angle between the axes.<ref name="toth">{{citation
  | last = Toth | first = Gabor
  | last = Toth | first = Gabor
  | title = Glimpses of Algebra and Geometry
  | title = Glimpses of Algebra and Geometry
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  | url = https://books.google.com/books?id=IRwBCAAAQBAJ&pg=PA98
  | url = https://books.google.com/books?id=IRwBCAAAQBAJ&pg=PA98
}}</ref>
}}</ref>
[[File:Dihedral8.png|550px|thumb|center|This picture shows the effect of the sixteen elements of <math>\mathrm{D}_8</math> on a [[stop sign]]. Here, the first row shows the effect of the eight rotations, and the second row shows the effect of the eight reflections, in each case acting on the stop sign with the orientation as shown at the top left.]]
[[File:Dihedral8.png|550px|thumb|center|This picture shows the effect of the sixteen elements of <math>\mathrm{D}_8</math> on a [[stop sign]]. Here, the first row shows the effect of the eight rotations, and the second row shows the effect of the eight reflections, in each case acting on the stop sign with the orientation as shown at the top left.]]


===Group structure===
===Group structure===
As with any geometric object, the [[composition of functions|composition]] of two symmetries of a regular polygon is again a symmetry of this object.  With composition of symmetries to produce another as the binary operation, this gives the symmetries of a polygon the algebraic structure of a [[finite group]].<ref name=lovett>{{citation|title=Abstract Algebra: Structures and Applications|first=Stephen|last=Lovett|publisher=CRC Press|year=2015|isbn=9781482248913|page=71|url=https://books.google.com/books?id=jRUqCgAAQBAJ&pg=PA71}}</ref>
As with any geometric object, the [[composition of functions|composition]] of two symmetries of a regular polygon is again a symmetry of this object.  With composition of symmetries to produce another as the binary operation, this gives the symmetries of a polygon the algebraic structure of a [[finite group]].<ref name="lovett">{{citation
| title = Abstract Algebra: Structures and Applications
| first = Stephen | last = Lovett
| publisher = CRC Press
| year = 2015
| isbn = 9781482248913
| page = 71
| url = https://books.google.com/books?id=jRUqCgAAQBAJ&pg=PA71
}}</ref>


[[File:Labeled Triangle Reflections.svg|thumb|The lines of reflection labelled S<sub>0</sub>, S<sub>1</sub>, and S<sub>2</sub> remain fixed in space (on the page) and do not themselves move when a symmetry operation (rotation or reflection) is done on the triangle (this matters when doing compositions of symmetries).]]
[[File:Labeled Triangle Reflections.svg|thumb|The lines of reflection labelled {{math|1=S<sub>0</sub>}}, {{math|1=S<sub>1</sub>}}, and {{math|1=S<sub>2</sub>}} remain fixed in space (on the page) and do not themselves move when a symmetry operation (rotation or reflection) is done on the triangle (this matters when doing compositions of symmetries).]]
[[File:Two Reflection Rotation.svg|thumb|The composition of these two reflections is a rotation.]]
The following [[Cayley table]] shows the effect of composition in the [[dihedral group of order 6]], <math> \mathrm{D}_3 </math>&mdash;the symmetries of an [[equilateral triangle]]. Here, <math> \mathrm{r}_0 </math> denotes the identity, <math> \mathrm{r}_1 </math> and <math> \mathrm{r}_2 </math> denote counterclockwise rotations by 120° and 240° respectively, as well as <math> \mathrm{s}_0 </math>, <math> \mathrm{s}_1 </math>, and <math> \mathrm{s}_2 </math> denote reflections across the three lines shown in the adjacent picture.
The following [[Cayley table]] shows the effect of composition in the group [[Dihedral group of order 6|D<sub>3</sub>]] (the symmetries of an [[equilateral triangle]]). r<sub>0</sub> denotes the identity; r<sub>1</sub> and r<sub>2</sub> denote counterclockwise rotations by 120° and 240° respectively, and s<sub>0</sub>, s<sub>1</sub> and s<sub>2</sub> denote reflections across the three lines shown in the adjacent picture.


{| class=wikitable width=200
{| class=wikitable width=200
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|}
|}


For example, {{nowrap|1=s<sub>2</sub>s<sub>1</sub> = r<sub>1</sub>}}, because the reflection s<sub>1</sub> followed by the reflection s<sub>2</sub> results in a rotation of 120°.  The order of elements denoting the [[composition of functions|composition]] is right to left, reflecting the convention that the element acts on the expression to its right. The composition operation is not [[commutativity|commutative]].<ref name=lovett/>
For example, <math> \mathrm{s}_2 \mathrm{s}_1 = \mathrm{r}_1 </math>, because the reflection <math> \mathrm{s}_1 </math> followed by the reflection s<sub>2</sub> results in a rotation of 120°.  The order of elements denoting the [[composition of functions|composition]] is right to left, reflecting the convention that the element acts on the expression to its right. The composition operation is not [[commutativity|commutative]].<ref name=lovett/>


In general, the group D<sub>''n''</sub> has elements r<sub>0</sub>, ..., r<sub>''n''&minus;1</sub> and s<sub>0</sub>, ..., s<sub>''n''&minus;1</sub>, with composition given by the following formulae:
In general, the group <math> \mathrm{D}_n </math> has elements <math> r_0, \dots, r_{n-1} </math> and <math> s_0, \dots, s_{n-1} </math>, with composition given by the following formulae:
<math display="block"> \begin{align}
\mathrm{r}_i\,\mathrm{r}_j = \mathrm{r}_{i+j}, &\qquad \mathrm{r}_i\,\mathrm{s}_j = \mathrm{s}_{i+j}, \\
\mathrm{s}_i\,\mathrm{r}_j = \mathrm{s}_{i-j}, &\qquad \mathrm{s}_i\,\mathrm{s}_j = \mathrm{r}_{i-j}.
\end{align}</math>


:<math>\mathrm{r}_i\,\mathrm{r}_j = \mathrm{r}_{i+j}, \quad \mathrm{r}_i\,\mathrm{s}_j = \mathrm{s}_{i+j}, \quad \mathrm{s}_i\,\mathrm{r}_j = \mathrm{s}_{i-j}, \quad \mathrm{s}_i\,\mathrm{s}_j = \mathrm{r}_{i-j}.</math>
In all cases, addition and subtraction of subscripts are to be performed using [[modular arithmetic]] with modulus <math> n </math>.
 
In all cases, addition and subtraction of subscripts are to be performed using [[modular arithmetic]] with modulus ''n''.


===Matrix representation===
===Matrix representation===
[[File:Pentagon Linear.png|thumb|The symmetries of this pentagon are [[linear transformation]]s of the plane as a vector space.]]
Centering the regular polygon at the origin, elements of the dihedral group act as [[linear map|linear transformations]] of the [[Cartesian coordinate system|plane]]. This lets elements of <math> \mathrm{D}_n </math> represented as [[Matrix (mathematics)|matrices]], with composition being [[matrix multiplication]]. This is an example of a (two-dimensional) [[group representation]].
If we center the regular polygon at the origin, then elements of the dihedral group act as [[linear map|linear transformations]] of the [[Cartesian coordinate system|plane]]. This lets us represent elements of D<sub>''n''</sub> as [[Matrix (mathematics)|matrices]], with composition being [[matrix multiplication]].
This is an example of a (2-dimensional) [[group representation]].


For example, the elements of the group [[Dihedral group of order 8|D<sub>4</sub>]] can be represented by the following eight matrices:
For example, the elements of the group [[dihedral group of order 8]], <math> \mathrm{D}_4 </math>&mdash;the group symmetry of a [[square]]&mdash;can be represented by the following eight matrices:{{r|ers}}
 
<math display="block">\begin{matrix}
:<math>\begin{matrix}
   \mathrm{r}_0 = \left(\begin{smallmatrix}  1 &  0 \\[0.2em]  0 &  1 \end{smallmatrix}\right), &
   \mathrm{r}_0 = \left(\begin{smallmatrix}  1 &  0 \\[0.2em]  0 &  1 \end{smallmatrix}\right), &
     \mathrm{r}_1 = \left(\begin{smallmatrix}  0 & -1 \\[0.2em]  1 &  0 \end{smallmatrix}\right), &
     \mathrm{r}_1 = \left(\begin{smallmatrix}  0 & -1 \\[0.2em]  1 &  0 \end{smallmatrix}\right), &
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     \mathrm{s}_3 = \left(\begin{smallmatrix}  0 & -1 \\[0.2em] -1 &  0 \end{smallmatrix}\right).
     \mathrm{s}_3 = \left(\begin{smallmatrix}  0 & -1 \\[0.2em] -1 &  0 \end{smallmatrix}\right).
\end{matrix}</math>
\end{matrix}</math>
Here, these matrices [[Group representation|represents]] the symmetries of an axis-aligned square centered at the [[Origin (mathematics)|origin]], which acts on the plane by multiplication on [[column vector]]s of coordinates <math display="inline"> \bigl(\begin{smallmatrix}x\\y\end{smallmatrix}\bigr) </math>. The element <math> \mathrm{r}_1 </math> represents the identity. The elements <math> \mathrm{s}_0 </math> and <math> \mathrm{s}_2 </math> represents the [[Reflection (mathematics)|reflection]] across horizontal and vertical axis. The elements <math> \mathrm{s}_1 </math> and <math> \mathrm{s}_3 </math> represents the reflection across diagonals. Three other elements <math> \mathrm{r}_1 </math>, <math> \mathrm{r}_2 </math>, and <math> \mathrm{r}_3 </math> are [[Rotation (mathematics)|rotations]] around a center.{{r|ers}}
{{multiple image
| width = 180
| perrow = 4
| align = center
| caption_align = center
| image_style=border:none
| image1 = Square symmetry – I.png
| caption1 = {{math|1=r<sub>0</sub>}} <br> The square's initial position
| image2 = Square symmetry – R3.png
| caption2 = {{math|1=r<sub>1</sub>}} <br> Rotation by 270°
| image3 = Square symmetry – R2.png
| caption3 = {{math|1=r<sub>2</sub>}} <br> Rotation by 180°
| image4 = Square symmetry – R1.png
| caption4 = {{math|1=r<sub>3</sub>}} <br> Rotation by 90° anticlockwise
| image5 = Square symmetry – H.png
| caption5 = {{math|1=s<sub>0</sub>}} <br> Horizontal reflection
| image6 = Square symmetry – V.png
| caption6 = {{math|1=s<sub>1</sub>}} <br> Vertical reflection
| image7 = Square symmetry – D1.png
| caption7 = {{math|1=s<sub>2</sub>}} <br> Diagonal NW–SE reflection
| image8 = Square symmetry – D2.png
| caption8 = {{math|1=s<sub>3</sub>}} <br> Diagonal NE–SW reflection
}}


In general, the matrices for elements of D<sub>''n''</sub> have the following form:
In general, the matrices for elements of <math> \mathrm{D}_n </math> have the following form:
 
<math display="block">\begin{align}
:<math>\begin{align}
   \mathrm{r}_k & = \begin{pmatrix}
   \mathrm{r}_k & = \begin{pmatrix}
     \cos \frac{2\pi k}{n} & -\sin \frac{2\pi k}{n} \\
     \cos \frac{2\pi k}{n} & -\sin \frac{2\pi k}{n} \\
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     \cos \frac{2\pi k}{n} &  \sin \frac{2\pi k}{n} \\
     \cos \frac{2\pi k}{n} &  \sin \frac{2\pi k}{n} \\
     \sin \frac{2\pi k}{n} & -\cos \frac{2\pi k}{n}
     \sin \frac{2\pi k}{n} & -\cos \frac{2\pi k}{n}
   \end{pmatrix}
   \end{pmatrix}.
  .
\end{align}</math>
\end{align}</math>
 
Here, the element <math> \mathrm{r}_k </math> is a [[rotation matrix]], expressing a counterclockwise rotation through an angle of <math> 2\pi k/n </math>. The element <math> \mathrm{s}_k </math> is a reflection across a line that makes an angle of <math> \pi k/n </math> with the {{nowrap|1=<math> x </math>-axis}}.
r<sub>''k''</sub> is a [[rotation matrix]], expressing a counterclockwise rotation through an angle of {{nowrap|2''&pi;k''/''n''}}. s<sub>''k''</sub> is a reflection across a line that makes an angle of {{nowrap|''&pi;k''/''n''}} with the ''x''-axis.


===Other definitions===
===Other definitions===
{{math|D{{sub|''n''}}}} is the [[semidirect product]] of <math>\mathrm C_2 = \{1, s\}</math> acting on <math>\mathrm C_n</math> via the automorphism <math>\varphi_s(r) = r^{-1}</math>.<ref name="mac-lane">{{cite book |last1=Mac Lane |first1=Saunders |author-link1=Saunders Mac Lane |last2=Birkhoff |first2=Garrett |author-link2=Garrett Birkhoff |title=Algebra |edition=3rd |year=1999 |publisher=American Mathematical Society |isbn=0-8218-1646-2 |pages=414–415}}</ref>
{{math|D{{sub|''n''}}}} is the [[semidirect product]] of <math>\mathrm C_2 = \{1, s\}</math> acting on <math>\mathrm C_n</math> via the automorphism <math>\varphi_s(r) = r^{-1}</math>.<ref name="mac-lane">{{cite book |last1=Mac Lane |first1=Saunders |author-link1=Saunders Mac Lane |last2=Birkhoff |first2=Garrett |author-link2=Garrett Birkhoff |title=Algebra |edition=3rd |year=1999 |publisher=American Mathematical Society |isbn=0-8218-1646-2 |pages=414–415}}</ref>


It hence has [[presentation of a group|presentation]]<ref>{{cite book |last1=Johnson |first1=DL |title=Presentations of groups |date=1990 |publisher=Cambridge University Press |location=Cambridge, U.K. ; New York, NY, USA |isbn=9780521585422 |page=140 |url=https://archive.org/details/presentationsofg0000john_z8f6/page/140}}</ref>
It hence has [[presentation of a group|presentation]]<ref>{{cite book |last1=Johnson |first1=DL |title=Presentations of groups |date=1990 |publisher=Cambridge University Press |location=Cambridge, U.K.; New York, NY, USA |isbn=9780521585422 |page=140 |url=https://archive.org/details/presentationsofg0000john_z8f6/page/140}}</ref>
: <math>\begin{align}
: <math>\begin{align}
   \mathrm{D}_n &= \left\langle r, s \mid \operatorname{ord}(r) = n, \operatorname{ord}(s) = 2, srs^{-1} = r^{-1} \right\rangle \\
   \mathrm{D}_n &= \left\langle r, s \mid \operatorname{ord}(r) = n, \operatorname{ord}(s) = 2, srs^{-1} = r^{-1} \right\rangle \\
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* [[Cycle index#Dihedral group Dn|Cycle index of the dihedral group]]
* [[Cycle index#Dihedral group Dn|Cycle index of the dihedral group]]
* [[Dicyclic group]]
* [[Dicyclic group]]
* [[Dihedral group of order 6]]
* [[Dihedral group of order 8]]
* [[Point groups in three dimensions#Symmetry groups in 3D that are dihedral as abstract group|Dihedral symmetry groups in 3D]]
* [[Point groups in three dimensions#Symmetry groups in 3D that are dihedral as abstract group|Dihedral symmetry groups in 3D]]
* [[Dihedral symmetry in three dimensions]]
* [[Dihedral symmetry in three dimensions]]


==References==
==References==
{{reflist|2}}
{{reflist|2|refs=
 
<ref name="ers">{{cite conference
| last1 = Estévez | first1 = Manuel
| last2 = Roldán | first2 = Érika
| last3 = Segerman | first3 = Henry | author3-link = Henry Segerman
| editor1-last = Holdener | editor1-first = Judy | editor1-link = Judy Holdener
| editor2-last = Torrence | editor2-first = Eve | editor2-link = Eve Torrence
| editor3-last = Fong | editor3-first = Chamberlain
| editor4-last = Seaton | editor4-first = Katherine
| arxiv = 2311.06596
| contribution = Surfaces in the tesseract
| contribution-url = https://archive.bridgesmathart.org/2023/bridges2023-441.html
| isbn = 978-1-938664-45-8
| location = Phoenix, Arizona
| pages = 441–444
| publisher = Tessellations Publishing
| title = Proceedings of Bridges 2023: Mathematics, Art, Music, Architecture, Culture
| year = 2023}}</ref>
 
}}


==External links==
==External links==

Latest revision as of 06:35, 22 September 2025

Template:Short description Template:Group theory sidebar

In mathematics, a dihedral group is the group of symmetries of a regular polygon,[1][2] which includes rotations and reflections. Dihedral groups are among the simplest examples of finite groups, and they play an important role in group theory, geometry, and chemistry.[3]

The notation for the dihedral group differs in geometry and abstract algebra. In geometry, Template:Math or Template:Math refers to the symmetries of the [[n-gon|Template:Math-gon]], a group of order Template:Math. In abstract algebra, Template:Math refers to this same dihedral group.[4] This article uses the geometric convention, Template:Math.

Definition

The word "dihedral" comes from "di-" and "-hedron". The latter comes from the Greek word hédra, which means "face of a geometrical solid". Overall, it thus refers to the two faces of a polygon.

Elements

A regular polygon with n sides has 2n different symmetries: n rotational symmetries and n reflection symmetries; here, n3. The associated rotations and reflections make up the dihedral group Dn. If n is odd, each axis of symmetry connects the midpoint of one side to the opposite vertex. If n is even, there are n/2 axes of symmetry connecting the midpoints of opposite sides and n/2 axes of symmetry connecting opposite vertices. In either case, there are n axes of symmetry and 2n elements in the symmetry group.[5] Reflecting in one axis of symmetry followed by reflecting in another axis of symmetry produces a rotation through twice the angle between the axes.[6]

File:Dihedral8.png
This picture shows the effect of the sixteen elements of D8 on a stop sign. Here, the first row shows the effect of the eight rotations, and the second row shows the effect of the eight reflections, in each case acting on the stop sign with the orientation as shown at the top left.

Group structure

As with any geometric object, the composition of two symmetries of a regular polygon is again a symmetry of this object. With composition of symmetries to produce another as the binary operation, this gives the symmetries of a polygon the algebraic structure of a finite group.[7]

File:Labeled Triangle Reflections.svg
The lines of reflection labelled Template:Math, Template:Math, and Template:Math remain fixed in space (on the page) and do not themselves move when a symmetry operation (rotation or reflection) is done on the triangle (this matters when doing compositions of symmetries).

The following Cayley table shows the effect of composition in the dihedral group of order 6, D3—the symmetries of an equilateral triangle. Here, r0 denotes the identity, r1 and r2 denote counterclockwise rotations by 120° and 240° respectively, as well as s0, s1, and s2 denote reflections across the three lines shown in the adjacent picture.

r0 r1 r2 s0 s1 s2
r0 r0 r1 r2 s0 s1 s2
r1 r1 r2 r0 s1 s2 s0
r2 r2 r0 r1 s2 s0 s1
s0 s0 s2 s1 r0 r2 r1
s1 s1 s0 s2 r1 r0 r2
s2 s2 s1 s0 r2 r1 r0

For example, s2s1=r1, because the reflection s1 followed by the reflection s2 results in a rotation of 120°. The order of elements denoting the composition is right to left, reflecting the convention that the element acts on the expression to its right. The composition operation is not commutative.[7]

In general, the group Dn has elements r0,,rn1 and s0,,sn1, with composition given by the following formulae: rirj=ri+j,risj=si+j,sirj=sij,sisj=rij.

In all cases, addition and subtraction of subscripts are to be performed using modular arithmetic with modulus n.

Matrix representation

Centering the regular polygon at the origin, elements of the dihedral group act as linear transformations of the plane. This lets elements of Dn represented as matrices, with composition being matrix multiplication. This is an example of a (two-dimensional) group representation.

For example, the elements of the group dihedral group of order 8, D4—the group symmetry of a square—can be represented by the following eight matrices:Template:R r0=(1001),r1=(0110),r2=(1001),r3=(0110),s0=(1001),s1=(0110),s2=(1001),s3=(0110). Here, these matrices represents the symmetries of an axis-aligned square centered at the origin, which acts on the plane by multiplication on column vectors of coordinates (xy). The element r1 represents the identity. The elements s0 and s2 represents the reflection across horizontal and vertical axis. The elements s1 and s3 represents the reflection across diagonals. Three other elements r1, r2, and r3 are rotations around a center.Template:R Template:Multiple image

In general, the matrices for elements of Dn have the following form: rk=(cos2πknsin2πknsin2πkncos2πkn)  andsk=(cos2πknsin2πknsin2πkncos2πkn). Here, the element rk is a rotation matrix, expressing a counterclockwise rotation through an angle of 2πk/n. The element sk is a reflection across a line that makes an angle of πk/n with the x-axis.

Other definitions

Template:Math is the semidirect product of C2={1,s} acting on Cn via the automorphism φs(r)=r1.[8]

It hence has presentation[9]

Dn=r,sord(r)=n,ord(s)=2,srs1=r1=r,sord(r)=n,ord(s)=2,srs=r1=r,srn=s2=(sr)2=1.

Using the relation s2=1, we obtain the relation r=ssr. It follows that Dn is generated by s and t:=sr. This substitution also shows that Dn has the presentation

Dn=s,ts2=1,t2=1,(st)n=1.

In particular, Template:Math belongs to the class of Coxeter groups.

Small dihedral groups

File:Regular hexagon symmetries.svg
Example subgroups from a hexagonal dihedral symmetry

Template:Math is isomorphic to Template:Math, the cyclic group of order 2.

Template:Math is isomorphic to Template:Math, the Klein four-group.

Template:Math and Template:Math are exceptional in that:

The cycle graphs of dihedral groups consist of an n-element cycle and n 2-element cycles. The dark vertex in the cycle graphs below of various dihedral groups represents the identity element, and the other vertices are the other elements of the group. A cycle consists of successive powers of either of the elements connected to the identity element.

Cycle graphs
D1 = Z2 D2 = Z22 = K4 D3 D4 D5
File:GroupDiagramMiniC2.svg File:GroupDiagramMiniD4.svg File:GroupDiagramMiniD6.svg File:GroupDiagramMiniD8.svg File:GroupDiagramMiniD10.svg
File:GroupDiagramMiniD12.svg File:GroupDiagramMiniD14.svg File:GroupDiagramMiniD16.svg File:GroupDiagramMiniD18.png File:GroupDiagramMiniD20.png
D6 = D3 × Z2 D7 D8 D9 D10 = D5 × Z2
D3 = S3 D4
File:Symmetric group 3; cycle graph.svg File:Dih4 cycle graph.svg

The dihedral group as symmetry group in 2D and rotation group in 3D

An example of abstract group Template:Math, and a common way to visualize it, is the group of Euclidean plane isometries which keep the origin fixed. These groups form one of the two series of discrete point groups in two dimensions. Template:Math consists of Template:Math rotations of multiples of Template:Math about the origin, and reflections across Template:Math lines through the origin, making angles of multiples of Template:Math with each other. This is the symmetry group of a regular polygon with Template:Math sides (for Template:Math; this extends to the cases Template:Math and Template:Math where we have a plane with respectively a point offset from the "center" of the "1-gon" and a "2-gon" or line segment).

Template:Math is generated by a rotation Template:Math of order Template:Math and a reflection Template:Math of order 2 such that

srs=r1

In geometric terms: in the mirror a rotation looks like an inverse rotation.

In terms of complex numbers: multiplication by e2πin and complex conjugation.

In matrix form, by setting

r1=[cos2πnsin2πnsin2πncos2πn]s0=[1001]

and defining rj=r1j and sj=rjs0 for j{1,,n1} we can write the product rules for Dn as

rjrk=r(j+k) mod nrjsk=s(j+k) mod nsjrk=s(jk) mod nsjsk=r(jk) mod n

(Compare coordinate rotations and reflections.)

The dihedral group D2 is generated by the rotation r of 180 degrees, and the reflection s across the x-axis. The elements of D2 can then be represented as {e, r, s, rs}, where e is the identity or null transformation and rs is the reflection across the y-axis.

File:Dihedral4.png
The four elements of D2 (x-axis is vertical here)

D2 is isomorphic to the Klein four-group.

For n > 2 the operations of rotation and reflection in general do not commute and Dn is not abelian; for example, in D4, a rotation of 90 degrees followed by a reflection yields a different result from a reflection followed by a rotation of 90 degrees.

File:D8isNonAbelian.png
D4 is nonabelian (x-axis is vertical here).

Thus, beyond their obvious application to problems of symmetry in the plane, these groups are among the simplest examples of non-abelian groups, and as such arise frequently as easy counterexamples to theorems which are restricted to abelian groups.

The Template:Math elements of Template:Math can be written as Template:Math, Template:Math, Template:Math, ... , Template:Math, Template:Math, Template:Math, Template:Math, ... , Template:Math. The first Template:Math listed elements are rotations and the remaining Template:Math elements are axis-reflections (all of which have order 2). The product of two rotations or two reflections is a rotation; the product of a rotation and a reflection is a reflection.

So far, we have considered Template:Math to be a subgroup of Template:Math, i.e. the group of rotations (about the origin) and reflections (across axes through the origin) of the plane. However, notation Template:Math is also used for a subgroup of SO(3) which is also of abstract group type Template:Math: the proper symmetry group of a regular polygon embedded in three-dimensional space (if n ≥ 3). Such a figure may be considered as a degenerate regular solid with its face counted twice. Therefore, it is also called a dihedron (Greek: solid with two faces), which explains the name dihedral group (in analogy to tetrahedral, octahedral and icosahedral group, referring to the proper symmetry groups of a regular tetrahedron, octahedron, and icosahedron respectively).

Examples of 2D dihedral symmetry

Properties

The properties of the dihedral groups Template:Math with Template:Math depend on whether Template:Math is even or odd. For example, the center of Template:Math consists only of the identity if n is odd, but if n is even the center has two elements, namely the identity and the element rn/2 (with Dn as a subgroup of O(2), this is inversion; since it is scalar multiplication by −1, it is clear that it commutes with any linear transformation).

In the case of 2D isometries, this corresponds to adding inversion, giving rotations and mirrors in between the existing ones.

For n twice an odd number, the abstract group Template:Math is isomorphic with the direct product of Template:Math and Template:Math. Generally, if m divides n, then Template:Math has n/m subgroups of type Template:Math, and one subgroup m. Therefore, the total number of subgroups of Template:Math (n ≥ 1), is equal to d(n) + σ(n), where d(n) is the number of positive divisors of n and σ(n) is the sum of the positive divisors of n. See list of small groups for the cases n ≤ 8.

The dihedral group of order 8 (D4) is the smallest example of a group that is not a T-group. Any of its two Klein four-group subgroups (which are normal in D4) has as normal subgroup order-2 subgroups generated by a reflection (flip) in D4, but these subgroups are not normal in D4.

Conjugacy classes of reflections

All the reflections are conjugate to each other whenever n is odd, but they fall into two conjugacy classes if n is even. If we think of the isometries of a regular n-gon: for odd n there are rotations in the group between every pair of mirrors, while for even n only half of the mirrors can be reached from one by these rotations. Geometrically, in an odd polygon every axis of symmetry passes through a vertex and a side, while in an even polygon there are two sets of axes, each corresponding to a conjugacy class: those that pass through two vertices and those that pass through two sides.

Algebraically, this is an instance of the conjugate Sylow theorem (for n odd): for n odd, each reflection, together with the identity, form a subgroup of order 2, which is a Sylow 2-subgroup (2 = 21 is the maximum power of 2 dividing 2n = 2[2k + 1]), while for n even, these order 2 subgroups are not Sylow subgroups because 4 (a higher power of 2) divides the order of the group.

For n even there is instead an outer automorphism interchanging the two types of reflections (properly, a class of outer automorphisms, which are all conjugate by an inner automorphism).

Automorphism group

The automorphism group of Template:Math is isomorphic to the holomorph of /n, i.e., to Hol(/n) = {ax + b | (a, n) = 1} and has order (n), where ϕ is Euler's totient function, the number of k in 1, ..., n − 1 coprime to n.

It can be understood in terms of the generators of a reflection and an elementary rotation (rotation by k(2π/n), for k coprime to n); which automorphisms are inner and outer depends on the parity of n.

  • For n odd, the dihedral group is centerless, so any element defines a non-trivial inner automorphism; for n even, the rotation by 180° (reflection through the origin) is the non-trivial element of the center.
  • Thus for n odd, the inner automorphism group has order 2n, and for n even (other than n = 2) the inner automorphism group has order n.
  • For n odd, all reflections are conjugate; for n even, they fall into two classes (those through two vertices and those through two faces), related by an outer automorphism, which can be represented by rotation by π/n (half the minimal rotation).
  • The rotations are a normal subgroup; conjugation by a reflection changes the sign (direction) of the rotation, but otherwise leaves them unchanged. Thus automorphisms that multiply angles by k (coprime to n) are outer unless k = ±1.

Examples of automorphism groups

Template:Math has 18 inner automorphisms. As 2D isometry group D9, the group has mirrors at 20° intervals. The 18 inner automorphisms provide rotation of the mirrors by multiples of 20°, and reflections. As isometry group these are all automorphisms. As abstract group there are in addition to these, 36 outer automorphisms; e.g., multiplying angles of rotation by 2.

Template:Math has 10 inner automorphisms. As 2D isometry group D10, the group has mirrors at 18° intervals. The 10 inner automorphisms provide rotation of the mirrors by multiples of 36°, and reflections. As isometry group there are 10 more automorphisms; they are conjugates by isometries outside the group, rotating the mirrors 18° with respect to the inner automorphisms. As abstract group there are in addition to these 10 inner and 10 outer automorphisms, 20 more outer automorphisms; e.g., multiplying rotations by 3.

Compare the values 6 and 4 for Euler's totient function, the multiplicative group of integers modulo n for n = 9 and 10, respectively. This triples and doubles the number of automorphisms compared with the two automorphisms as isometries (keeping the order of the rotations the same or reversing the order).

The only values of n for which φ(n) = 2 are 3, 4, and 6, and consequently, there are only three dihedral groups that are isomorphic to their own automorphism groups, namely Template:Math (order 6), Template:Math (order 8), and Template:Math (order 12).[10][11][12]

Inner automorphism group

The inner automorphism group of Template:Math is isomorphic to:[13]

Generalizations

There are several important generalizations of the dihedral groups:

See also

Template:Sister project

References

Template:Reflist

External links

Template:Group navbox

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