Skip to main content
Contents
Dark Mode Prev Up Next
\( \renewcommand{\Re}{\operatorname{Re}}
\renewcommand{\Im}{\operatorname{Im}}
\newcommand{\N}{{\mathbb N}}
\newcommand{\Z}{{\mathbb Z}}
\newcommand{\Q}{{\mathbb Q}}
\newcommand{\R}{{\mathbb R}}
\newcommand{\C}{{\mathbb C}}
\newcommand{\T}{{\mathbb T}}
\newcommand{\F}{{\mathbb F}}
\newcommand{\PP}{{\mathbb P}}
\newcommand{\HH}{{\mathbb H}}
\newcommand{\compose}{\circ}
\newcommand{\bolda}{{\mathbf a}}
\newcommand{\boldb}{{\mathbf b}}
\newcommand{\boldc}{{\mathbf c}}
\newcommand{\boldd}{{\mathbf d}}
\newcommand{\bolde}{{\mathbf e}}
\newcommand{\boldi}{{\mathbf i}}
\newcommand{\boldj}{{\mathbf j}}
\newcommand{\boldk}{{\mathbf k}}
\newcommand{\boldn}{{\mathbf n}}
\newcommand{\boldp}{{\mathbf p}}
\newcommand{\boldq}{{\mathbf q}}
\newcommand{\boldr}{{\mathbf r}}
\newcommand{\bolds}{{\mathbf s}}
\newcommand{\boldt}{{\mathbf t}}
\newcommand{\boldu}{{\mathbf u}}
\newcommand{\boldv}{{\mathbf v}}
\newcommand{\boldw}{{\mathbf w}}
\newcommand{\boldx}{{\mathbf x}}
\newcommand{\boldy}{{\mathbf y}}
\newcommand{\boldz}{{\mathbf z}}
\newcommand{\boldzero}{{\mathbf 0}}
\newcommand{\boldmod}{\boldsymbol{ \bmod }}
\newcommand{\boldT}{{\mathbf T}}
\newcommand{\boldN}{{\mathbf N}}
\newcommand{\boldB}{{\mathbf B}}
\newcommand{\boldF}{{\mathbf F}}
\newcommand{\boldS}{{\mathbf S}}
\newcommand{\boldE}{{\mathbf E}}
\newcommand{\boldG}{{\mathbf G}}
\newcommand{\boldK}{{\mathbf K}}
\newcommand{\boldL}{{\mathbf L}}
\DeclareMathOperator{\ch}{char}
\DeclareMathOperator{\lns}{lns}
\DeclareMathOperator{\lcm}{lcm}
\DeclareMathOperator{\Span}{span}
\DeclareMathOperator{\tr}{tr}
\DeclareMathOperator{\NS}{null}
\DeclareMathOperator{\RS}{row}
\DeclareMathOperator{\CS}{col}
\DeclareMathOperator{\im}{im}
\DeclareMathOperator{\range}{range}
\DeclareMathOperator{\rank}{rank}
\DeclareMathOperator{\nullity}{nullity}
\DeclareMathOperator{\sign}{sign}
\DeclareMathOperator{\Arg}{Arg}
\DeclareMathOperator{\Log}{Log}
\DeclareMathOperator{\Ext}{Ext}
\DeclareMathOperator{\Int}{Int}
\DeclareMathOperator{\Aut}{Aut}
\DeclareMathOperator{\Arcsin}{Arcsin}
\DeclareMathOperator{\Arccos}{Arccos}
\DeclareMathOperator{\Arctan}{Arctan}
\DeclareMathOperator{\Res}{Res}
\DeclareMathOperator{\res}{res}
\DeclareMathOperator{\Fix}{Fix}
\DeclareMathOperator{\Aff}{Aff}
\DeclareMathOperator{\Frac}{Frac}
\DeclareMathOperator{\Ann}{Ann}
\DeclareMathOperator{\Tor}{Tor}
\DeclareMathOperator{\id}{id}
\DeclareMathOperator{\mdeg}{mdeg}
\DeclareMathOperator{\Lt}{Lt}
\DeclareMathOperator{\Lc}{Lc}
\DeclareMathOperator{\disc}{disc}
\DeclareMathOperator{\Frob}{Frob}
\DeclareMathOperator{\adj}{adj}
\DeclareMathOperator{\ord}{ord}
\DeclareMathOperator{\curl}{curl}
\DeclareMathOperator{\grad}{grad}
\DeclareMathOperator{\diver}{div}
\DeclareMathOperator{\flux}{flux}
\DeclareMathOperator{\Hom}{Hom}
\DeclareMathOperator{\End}{End}
\DeclareMathOperator{\Isom}{Isom}
\DeclareMathOperator{\GL}{GL}
\DeclareMathOperator{\SL}{SL}
\DeclareMathOperator{\ML}{M}
\DeclareMathOperator{\Syl}{Syl}
\DeclareMathOperator{\Gal}{Gal}
\DeclareMathOperator{\ab}{ab}
\DeclareMathOperator{\sgn}{sgn}
\DeclareMathOperator{\len}{len}
\DeclareMathOperator{\proj}{proj}
\newcommand{\surjects}{\twoheadrightarrow}
\newcommand{\injects}{\hookrightarrow}
\newcommand{\bijects}{\leftrightarrow}
\newcommand{\isomto}{\overset{\sim}{\rightarrow}}
\newcommand{\floor}[1]{\lfloor#1\rfloor}
\newcommand{\ceiling}[1]{\left\lceil#1\right\rceil}
\newcommand{\mclass}[2][m]{[#2]_{#1}}
\newcommand{\val}[2][]{\left\lvert #2\right\rvert_{#1}}
\newcommand{\abs}[2][]{\left\lvert #2\right\rvert_{#1}}
\newcommand{\valuation}[2][]{\left\lvert #2\right\rvert_{#1}}
\newcommand{\norm}[1]{\left\lVert#1\right\rVert}
\newcommand{\anpoly}{a_nx^n+a_{n-1}x^{n-1}\cdots +a_1x+a_0}
\newcommand{\anmonic}{x^n+a_{n-1}x^{n-1}\cdots +a_1x+a_0}
\newcommand{\bmpoly}{b_mx^m+b_{m-1}x^{m-1}\cdots +b_1x+b_0}
\newcommand{\pder}[2]{\frac{\partial#1}{\partial#2}}
\newcommand{\normalin}{\trianglelefteq}
\newcommand{\angvec}[1]{\langle #1\rangle}
\newcommand{\varpoly}[2]{#1_{#2}x^{#2}+#1_{#2-1}x^{#2-1}\cdots +#1_1x+#1_0}
\newcommand{\varpower}[1][a]{#1_0+#1_1x+#1_1x^2+\cdots}
\newcommand{\limasto}[2][x]{\lim_{#1\rightarrow #2}}
\newcommand{\abcdmatrix}[4]{\begin{bmatrix}#1\amp #2\\ #3\amp #4 \end{bmatrix}
}
\newenvironment{amatrix}[1][ccc|c]{\left[\begin{array}{#1}}{\end{array}\right]}
\newenvironment{linsys}[2][m]{
\begin{array}[#1]{@{}*{#2}{rc}r@{}}
}{
\end{array}}
\newcommand{\eqsys}{\begin{array}{rcrcrcr}
a_{11}x_{1}\amp +\amp a_{12}x_{2}\amp +\cdots+\amp a_{1n}x_{n}\amp =\amp b_1\\
a_{21}x_{1}\amp +\amp a_{22}x_{2}\amp +\cdots+\amp a_{2n}x_{n}\amp =\amp b_2\\
\amp \vdots\amp \amp \vdots \amp \amp \vdots \amp \\
a_{m1}x_{1}\amp +\amp a_{m2}x_{2}\amp +\cdots +\amp a_{mn}x_{n}\amp =\amp b_m
\end{array}
}
\newcommand{\numeqsys}{\begin{array}{rrcrcrcr}
e_1:\amp a_{11}x_{1}\amp +\amp a_{12}x_{2}\amp +\cdots+\amp a_{1n}x_{n}\amp =\amp b_1\\
e_2: \amp a_{21}x_{1}\amp +\amp a_{22}x_{2}\amp +\cdots+\amp a_{2n}x_{n}\amp =\amp b_2\\
\amp \vdots\amp \amp \vdots \amp \amp \vdots \amp \\
e_m: \amp a_{m1}x_{1}\amp +\amp a_{m2}x_{2}\amp +\cdots +\amp a_{mn}x_{n}\amp =\amp b_m
\end{array}
}
\newcommand{\homsys}{\begin{array}{rcrcrcr}
a_{11}x_{1}\amp +\amp a_{12}x_{2}\amp +\cdots+\amp a_{1n}x_{n}\amp =\amp 0\\
a_{21}x_{1}\amp +\amp a_{22}x_{2}\amp +\cdots+\amp a_{2n}x_{n}\amp =\amp 0\\
\amp \vdots\amp \amp \vdots \amp \amp \vdots \amp \\
a_{m1}x_{1}\amp +\amp a_{m2}x_{2}\amp +\cdots +\amp a_{mn}x_{n}\amp =\amp 0
\end{array}
}
\newcommand{\vareqsys}[4]{
\begin{array}{ccccccc}
#3_{11}x_{1}\amp +\amp #3_{12}x_{2}\amp +\cdots+\amp #3_{1#2}x_{#2}\amp =\amp #4_1\\
#3_{21}x_{1}\amp +\amp #3_{22}x_{2}\amp +\cdots+\amp #3_{2#2}x_{#2}\amp =\amp #4_2\\
\vdots \amp \amp \vdots \amp \amp \vdots \amp =\amp \\
#3_{#1 1}x_{1}\amp +\amp #3_{#1 2}x_{2}\amp +\cdots +\amp #3_{#1 #2}x_{#2}\amp =\amp #4_{#1}
\end{array}
}
\newcommand{\genmatrix}[1][a]{
\begin{bmatrix}
#1_{11} \amp #1_{12} \amp \cdots \amp #1_{1n} \\
#1_{21} \amp #1_{22} \amp \cdots \amp #1_{2n} \\
\vdots \amp \vdots \amp \ddots \amp \vdots \\
#1_{m1} \amp #1_{m2} \amp \cdots \amp #1_{mn}
\end{bmatrix}
}
\newcommand{\varmatrix}[3]{
\begin{bmatrix}
#3_{11} \amp #3_{12} \amp \cdots \amp #3_{1#2} \\
#3_{21} \amp #3_{22} \amp \cdots \amp #3_{2#2} \\
\vdots \amp \vdots \amp \ddots \amp \vdots \\
#3_{#1 1} \amp #3_{#1 2} \amp \cdots \amp #3_{#1 #2}
\end{bmatrix}
}
\newcommand{\augmatrix}{
\begin{amatrix}[cccc|c]
a_{11} \amp a_{12} \amp \cdots \amp a_{1n} \amp b_{1}\\
a_{21} \amp a_{22} \amp \cdots \amp a_{2n} \amp b_{2}\\
\vdots \amp \vdots \amp \ddots \amp \vdots \amp \vdots\\
a_{m1} \amp a_{m2} \amp \cdots \amp a_{mn}\amp b_{m}
\end{amatrix}
}
\newcommand{\varaugmatrix}[4]{
\begin{amatrix}[cccc|c]
#3_{11} \amp #3_{12} \amp \cdots \amp #3_{1#2} \amp #4_{1}\\
#3_{21} \amp #3_{22} \amp \cdots \amp #3_{2#2} \amp #4_{2}\\
\vdots \amp \vdots \amp \ddots \amp \vdots \amp \vdots\\
#3_{#1 1} \amp #3_{#1 2} \amp \cdots \amp #3_{#1 #2}\amp #4_{#1}
\end{amatrix}
}
\newcommand{\spaceforemptycolumn}{\makebox[\wd\boxofmathplus]{\ }}
\newcommand{\generalmatrix}[3]{
\left(
\begin{array}{cccc}
#1_{1,1} \amp #1_{1,2} \amp \ldots \amp #1_{1,#2} \\
#1_{2,1} \amp #1_{2,2} \amp \ldots \amp #1_{2,#2} \\
\amp \vdots \\
#1_{#3,1} \amp #1_{#3,2} \amp \ldots \amp #1_{#3,#2}
\end{array}
\right) }
\newcommand{\colvec}[2][c]{\begin{amatrix}[#1] #2 \end{amatrix}}
\newcommand{\rowvec}[1]{\begin{bmatrix} #1 \end{bmatrix}}
\newcommand{\lt}{<}
\newcommand{\gt}{>}
\newcommand{\amp}{&}
\definecolor{fillinmathshade}{gray}{0.9}
\newcommand{\fillinmath}[1]{\mathchoice{\colorbox{fillinmathshade}{$\displaystyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\textstyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\scriptstyle \phantom{\,#1\,}$}}{\colorbox{fillinmathshade}{$\scriptscriptstyle\phantom{\,#1\,}$}}}
\)
Section 1.18 Group actions: orbits
Definition 1.18.1 . Orbits.
Let \(G\times A\rightarrow A\) be a group action. Given \(a\in A\text{,}\) we define its orbit \(O_a\) as
\begin{equation}
O_a=\{a'\mid a'=g\cdot a \text{ for some } g\in G\}=\{g\cdot a\mid g\in G\}\text{.}\tag{1.18.1}
\end{equation}
Definition 1.18.2 . Transitive group action.
A group action
\(G\times A\rightarrow A\) is transitive if for all
\(a,a'\in A\) there is a
\(g\in G\) satisfying
\(a'=g\cdot a\text{.}\)
Theorem 1.18.3 . Orbit-stabilizer.
Let \(G\times A\rightarrow A\) be a group action.
For all \(a\in A\text{,}\) the function
\begin{align*}
f\colon G/G_a \amp \rightarrow O_a\\
gG_a \amp \mapsto g\cdot a
\end{align*}
is an isomorphism of \(G\) -sets, where \(G\) acts on \(G/G_a\) by left multiplication, and the action of \(G\) on \(O_a\) is given by restriction.
For all \(a\in A\) we have
\begin{equation}
\abs{O_a}=[G\colon G_a]\text{.}\tag{1.18.2}
\end{equation}
Proof.
Example 1.18.4 . Rotational symmetries of a tetrahedron.
Let
\(T\) be a regular tetrahedron in
\(\R^3\) and let
\(G\) be the group of rotations in
\(\R^3\) that map
\(T\) to itself. Establish an isomorphism between
\(G\) and one of our familiar groups.
Example 1.18.5 . Rotational symmetries of a tetrahedron.
Let
\(C\) be a cube in
\(\R^3\) and let
\(G\) be the group of rotational symmetries of
\(C\text{.}\) Establish an isomorphism between
\(G\) and one of our familiar groups.
Theorem 1.18.6 . Orbit decomposition theorem.
Let \(G\times A\rightarrow A\) be a group action.
The relation \(a\sim a'\) if and only if \(a'\in O_a\) is an equivalence relation whose equivalence classes are the distinct orbits \(O_a\) of the group action. As a result, we have a partition
\begin{equation*}
A=\bigcup_{a\in A}O_a
\end{equation*}
of \(A\) into disjoint orbits, and \(O_a=O_{a'}\) if and only if \(a'\in O_a\text{.}\)
As a
\(G\) -set,
\(A\) decomposes into a disjoint union of orbits, each of which is isomorphic as a
\(G\) -set to
\(G/H\) for some subgroup
\(H\leq G\text{.}\)
Proof.
We end this section with a fantastic result commonly known as
Burnsideβs lemma even though it was first proved (using modern group-theoretic language) by Frobenius. Consequently, some mathematical wags refer to the result as the
lemma that is not Burnsideβs . We confuse things even further by giving it the designation of a theorem! The result allows us to count the distinct orbits of a group action in terms of so-called fix sets, which we now define.
Definition 1.18.7 . Fix sets.
Let \(G\times A\rightarrow A\) be a group action. Given an element \(g\in G\text{,}\) the fix set of \(g\) under this action, denoted \(\Fix(g)\text{,}\) is defined as
\begin{equation}
\Fix(g)=\{a\in A\mid g\cdot a=a\}\text{.}\tag{1.18.3}
\end{equation}
More generally, given a subset \(X\subseteq G\text{,}\) we define its fix set \(\Fix(X)\) as
\begin{equation}
\Fix(X)=\{a\in A\mid g\cdot a=a \text{ for all } g\in X\}=\bigcap_{g\in X}\Fix(g)\text{.}\tag{1.18.4}
\end{equation}
Theorem 1.18.8 (Frobenius) . Burnsideβs lemma.
Let \(G\) be a finite group acting on a finite nonempty set \(A\text{,}\) and let \(O\) be the set of orbits of the group action. We have
\begin{equation}
\abs{O}=\frac{1}{\abs{G}}\sum_{g\in G}\Fix(g)\text{.}\tag{1.18.5}
\end{equation}
Proof.