Conjugacy Class Equation
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Theorem
Let $G$ be a group.
Let $\left|{G}\right|$ be the order of $G$.
Let $Z \left({G}\right)$ be the center of $G$.
Let $x \in G$.
Let $N_G \left({x}\right)$ be the normalizer of $x$ in $G$.
Let $\left[{G : N_G \left({x}\right)}\right]$ be the index of $N_G \left({x}\right)$ in $G$.
Let $m$ be the number of non-singleton conjugacy classes of $G$.
Then:
- $\displaystyle \left|{G}\right| = \left|{Z \left({G}\right)}\right| + \sum_{j \mathop = 1}^m \left[{G : N_G \left({x_j}\right)}\right]$
Proof 1
From Conjugacy Classes of Center Elements are Singletons, all elements of $Z \left({G}\right)$ form their own singleton conjugacy classes.
Abelian Group
Suppose $G$ is abelian.
Then from Group is Abelian iff Center Equals Group we have $Z \left({G}\right) = G$.
So there are as many conjugacy classes as there are elements in $Z \left({G}\right)$ and hence in $G$.
So in this case the result certainly holds.
$\Box$
Non-Abelian Group
Now suppose $G$ is non-abelian.
Thus $Z \left({G}\right) \ne G$ and therefore $G \setminus Z \left({G}\right) \ne \varnothing$.
From Conjugacy Classes of Center Elements are Singletons, all the non-singleton conjugacy classes of $G$ are in $G \setminus Z \left({G}\right)$.
From the way the theorem has been worded, there are $m$ of them.
Let us choose one element from each of the non-singleton conjugacy classes and call them $x_1, x_2, \ldots, x_m$.
Thus, these conjugacy classes can be written:
- $\mathrm C_{x_1}, \mathrm C_{x_2}, \ldots, \mathrm C_{x_m}$
So:
- $\displaystyle \left|{G \setminus Z \left({G}\right)}\right| = \sum_{j \mathop = 1}^m \left|{\mathrm C_{x_j}}\right|$
or:
- $\displaystyle \left|{G}\right| \setminus \left|{Z \left({G}\right)}\right| = \sum_{j \mathop = 1}^m \left|{\mathrm C_{x_j}}\right|$
From Size of Conjugacy Class is Index of Normalizer:
- $\left|{\mathrm C_{x_j}}\right| = \left[{G : N_G \left({x_j}\right)}\right]$
and the result follows.
$\blacksquare$
Proof 2
Let the distinct orbits of $G$ under the Conjugacy Action be $\operatorname{Orb} \left({x_1}\right), \operatorname{Orb} \left({x_2}\right), \ldots, \operatorname{Orb} \left({x_s}\right)$.
Then from the Partition Equation:
- $\left|{G}\right| = \left|{\operatorname{Orb} \left({x_1}\right)}\right| + \left|{\operatorname{Orb} \left({x_2}\right)}\right| + \cdots + \left|{\operatorname{Orb} \left({x_s}\right)}\right|$
From the Orbit-Stabilizer Theorem:
- $\left|{\operatorname{Orb} \left({x_i}\right)}\right| \backslash \left|{G}\right|, i = 1, \ldots, s$
The result follows from the definition of the Conjugacy Action.
$\blacksquare$
Sources
- Seth Warner: Modern Algebra (1965)... (previous)... (next): Exercise $25.16 \ \text{(c)}$