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Two Cayley graphs of dihedral groups with conjugacy classes distinguished by color.

In mathematics, especially group theory, two elements and of a group are conjugate if there is an element in the group such that This is an equivalence relation whose equivalence classes are called conjugacy classes. In other words, each conjugacy class is closed under for all elements in the group.

Members of the same conjugacy class cannot be distinguished by using only the group structure, and therefore share many properties. The study of conjugacy classes of non-abelian groups is fundamental for the study of their structure.[1][2] For an abelian group, each conjugacy class is a set containing one element (singleton set).

Functions that are constant for members of the same conjugacy class are called class functions.

Motivation

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The concept of conjugacy classes may come from trying to formalize the idea that two group elements are considered the "same" after a relabeling of elements.

For example, consider the symmetric group of order 5, and elements and that are conjugate. An element can be viewed as simply "renaming" the elements to then applying the permutation on this new labeling.

The conjugacy action by does not change the underlying structure of . In a way, permutations and have the same "shape".[3]

Another way to view the conjugacy action is by considering the general linear group of invertible matrices. Two matrices and conjugate if there exist a matrix such that , which is the same condition as matrix similarity. The two matrices are conjugates if they are the "same" under two possibly different bases, with being the change-of-basis matrix.

Conjugates also come up in some important theorems of group theory. One example is the Sylow theorems, which state that every Sylow -subgroup of a finite group are conjugates to each other. It also appears in the proof of Cauchy's theorem, which makes use of conjugacy classes.

Definition

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Let be a group. Two elements are conjugate if there exists an element such that in which case is called a conjugate of and is called a conjugate of

In the case of the general linear group of invertible matrices, the conjugacy relation is called matrix similarity.

It can be easily shown that conjugacy is an equivalence relation and therefore partitions into equivalence classes. (This means that every element of the group belongs to precisely one conjugacy class, and the classes and are equal if and only if and are conjugate, and disjoint otherwise.) The equivalence class that contains the element is and is called the conjugacy class of The class number of is the number of distinct (nonequivalent) conjugacy classes. All elements belonging to the same conjugacy class have the same order.

Conjugacy classes may be referred to by describing them, or more briefly by abbreviations such as "6A", meaning "a certain conjugacy class with elements of order 6", and "6B" would be a different conjugacy class with elements of order 6; the conjugacy class 1A is the conjugacy class of the identity which has order 1. In some cases, conjugacy classes can be described in a uniform way; for example, in the symmetric group they can be described by cycle type.

Examples

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All 4! = 24 possible permutations from , partitioned into conjugacy classes. Two elements belong in the same class iff they have the same cycle type.
All 10 possible permutations from , partitioned into conjugacy classes.

The symmetric group consisting of the 6 permutations of three elements, has three conjugacy classes:

  1. No change:
  2. Transposing two:
  3. A cyclic permutation of all three:

These three classes also correspond to the classification of the isometries of an equilateral triangle.

The symmetric group consisting of the 24 permutations of four elements, has five conjugacy classes, listed with their members using cycle notation:[4]

  1. No change:
  2. Interchanging two:
  3. A cyclic permutation of three:
  4. A cyclic permutation of all four:
  5. Interchanging two, and also the other two:

In general, the number of conjugacy classes in the symmetric group is equal to the number of integer partitions of This is because each conjugacy class corresponds to exactly one partition of into cycles, up to permutation of the elements of

The dihedral group consisting of symmetries of a pentagon, has four conjugacy classes:[5]

  1. The identity element:
  2. Two conjugacy classes of size 2:
  3. All the reflections:

For an abelian group, each conjugacy class is a set containing one element (singleton set).

Properties

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  • The identity element is always the only element in its class, that is
  • If is abelian then for all , i.e. for all (and the converse is also true: if all conjugacy classes are singletons then is abelian).
  • If two elements belong to the same conjugacy class (that is, if they are conjugate), then they have the same order. More generally, every statement about can be translated into a statement about because the map is an automorphism of called an inner automorphism. See the next property for an example.
  • If and are conjugate, then so are their powers and (Proof: if then ) Thus taking kth powers gives a map on conjugacy classes, and one may consider which conjugacy classes are in its preimage. For example, in the symmetric group, the square of an element of type (3)(2) (a 3-cycle and a 2-cycle) is an element of type (3), therefore one of the power-up classes of (3) is the class (3)(2) (where is a power-up class of ).
  • An element lies in the center of if and only if its conjugacy class has only one element, itself. More generally, if denotes the centralizer of i.e., the subgroup consisting of all elements such that then the index is equal to the number of elements in the conjugacy class of (by the orbit-stabilizer theorem).
  • Take and let be the distinct integers which appear as lengths of cycles in the cycle type of (including 1-cycles). Let be the number of cycles of length in for each (so that ). Then the number of conjugates of is:[1]

Conjugacy as group action

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For any two elements let This defines a group action of on The orbits of this action are the conjugacy classes, and the stabilizer of a given element is the element's centralizer.[6]

Similarly, we can define a group action of on the set of all subsets of by writing or on the set of the subgroups of

Conjugacy class equation

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If is a finite group, then for any group element the elements in the conjugacy class of are in one-to-one correspondence with cosets of the centralizer This can be seen by observing that any two elements and belonging to the same coset (and hence, for some in the centralizer ) give rise to the same element when conjugating : That can also be seen from the orbit-stabilizer theorem, when considering the group as acting on itself through conjugation, so that orbits are conjugacy classes and stabilizer subgroups are centralizers. The converse holds as well.

Thus the number of elements in the conjugacy class of is the index of the centralizer in ; hence the size of each conjugacy class divides the order of the group.

Furthermore, if we choose a single representative element from every conjugacy class, we infer from the disjointness of the conjugacy classes that where is the centralizer of the element Observing that each element of the center forms a conjugacy class containing just itself gives rise to the class equation:[7] where the sum is over a representative element from each conjugacy class that is not in the center.

Knowledge of the divisors of the group order can often be used to gain information about the order of the center or of the conjugacy classes.

Example

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Consider a finite -group (that is, a group with order where is a prime number and ). We are going to prove that every finite -group has a non-trivial center.

Since the order of any conjugacy class of must divide the order of it follows that each conjugacy class that is not in the center also has order some power of where But then the class equation requires that From this we see that must divide so

In particular, when then is an abelian group since any non-trivial group element is of order or If some element of is of order then is isomorphic to the cyclic group of order hence abelian. On the other hand, if every non-trivial element in is of order hence by the conclusion above then or We only need to consider the case when then there is an element of which is not in the center of Note that includes and the center which does not contain but at least elements. Hence the order of is strictly larger than therefore therefore is an element of the center of a contradiction. Hence is abelian and in fact isomorphic to the direct product of two cyclic groups each of order

Average Centralizer

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Let be a finite group. Consider the group action of on itself given by conjugation. The orbits are the conjugacy classes of and the set of fixed points of an element is the centralizer .

Thus by Burnside's lemma, the number of conjugacy classes is equal to , that is, the average size of the centralizer.

Conjugacy of subgroups and general subsets

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More generally, given any subset ( not necessarily a subgroup), define a subset to be conjugate to if there exists some such that Let be the set of all subsets such that is conjugate to

A frequently used theorem is that, given any subset the index of (the normalizer of ) in equals the cardinality of :

This follows since, if then if and only if in other words, if and only if are in the same coset of

By using this formula generalizes the one given earlier for the number of elements in a conjugacy class.

The above is particularly useful when talking about subgroups of The subgroups can thus be divided into conjugacy classes, with two subgroups belonging to the same class if and only if they are conjugate. Conjugate subgroups are isomorphic, but isomorphic subgroups need not be conjugate. For example, an abelian group may have two different subgroups which are isomorphic, but they are never conjugate.

Geometric interpretation

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Conjugacy classes in the fundamental group of a path-connected topological space can be thought of as equivalence classes of free loops under free homotopy.

Conjugacy class and irreducible representations in finite group

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In any finite group, the number of nonisomorphic irreducible representations over the complex numbers is precisely the number of conjugacy classes.

See also

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Notes

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References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
In group theory, a conjugacy class of an element gg in a group GG is the set of all elements conjugate to gg, consisting of elements of the form x1gxx^{-1}gx for xGx \in G. Conjugation defines an on the elements of GG, partitioning the group into disjoint conjugacy classes where elements within the same class share similar algebraic properties, such as having the same order. The size of a conjugacy class of gg equals the index of the centralizer Z(g)={xGxg=gx}Z(g) = \{ x \in G \mid xg = gx \} in GG, and thus divides the order of GG. In abelian groups, every element forms its own singleton conjugacy class, while non-abelian groups exhibit larger classes that reflect the group's structure. The collection of conjugacy classes satisfies the class equation G=Cl(gi)|G| = \sum |Cl(g_i)|, where the sum is over representatives gig_i of each class, providing a fundamental tool for analyzing group orders and symmetries. Conjugacy classes play a central role in , where irreducible representations are constant on classes, and in the study of group actions, as they correspond to orbits under the conjugation action. For finite groups, the number and sizes of classes yield insights into solvability and other structural features, with explicit computations possible for small groups like the S3S_3, which has three classes: the identity, transpositions, and 3-cycles.

Fundamentals

Definition

In group theory, two elements gg and hh in a group GG are said to be conjugate, written hgh \sim g, if there exists an element kGk \in G such that h=k1gkh = k^{-1} g k. This operation defines the standard notion of right conjugation in groups. Left conjugation, by contrast, is given by h=kgk1h = k g k^{-1}, but the resulting sets of conjugate elements coincide because every group element admits an inverse, so substituting k=k1k' = k^{-1} yields the same collection. The conjugacy class of an element gGg \in G, commonly denoted Cl(g)\mathrm{Cl}(g) or , is the set of all elements conjugate to gg, namely Cl(g)={k1gkkG}\mathrm{Cl}(g) = \{ k^{-1} g k \mid k \in G \}. Other notations, such as gGg^G for the class generated by conjugation from GG, appear in some contexts. The conjugacy relation \sim is an on the set GG. Reflexivity holds since g=e1geg = e^{-1} g e for the identity eGe \in G. Symmetry follows because if h=k1gkh = k^{-1} g k, then g=khk1=(k1)1h(k1)g = k h k^{-1} = (k^{-1})^{-1} h (k^{-1}). Transitivity is verified by noting that if h=k1gkh = k^{-1} g k and m=l1hlm = l^{-1} h l, then m=(kl)1g(kl)m = (k l)^{-1} g (k l).

Examples

A concrete example of conjugacy classes arises in the symmetric group S3S_3, which consists of all permutations of three elements and has order 6. The conjugacy classes in S3S_3 are determined by cycle type: the identity element forms its own class {e}\{e\} of size 1; the three transpositions (12)(1\,2), (13)(1\,3), and (23)(2\,3) form a single class of size 3, as any transposition is conjugate to any other via an appropriate permutation; and the two 3-cycles (123)(1\,2\,3) and (132)(1\,3\,2) form another class of size 2. These classes partition S3S_3 and illustrate how elements of the same cycle structure are conjugate. In the quaternion group Q8={±1,±i,±j,±k}Q_8 = \{\pm 1, \pm i, \pm j, \pm k\} of order 8, the conjugacy classes are {1}\{1\}, {1}\{-1\}, {i,i}\{i, -i\}, {j,j}\{j, -j\}, and {k,k}\{k, -k\}. The center Z(Q8)={1,1}Z(Q_8) = \{1, -1\} consists of elements that commute with everything, so 11 and 1-1 each form singleton classes. The remaining elements pair with their negatives under conjugation: for instance, jij1=ij \cdot i \cdot j^{-1} = -i, and similarly for the other pairs, yielding classes of size 2. These five classes reflect the non-abelian structure of Q8Q_8. For any abelian group GG, the conjugacy classes are all singletons {g}\{g\} for each gGg \in G. This follows because, in an abelian group, elements commute, so xgx1=gx g x^{-1} = g for all x,gGx, g \in G, meaning no element is conjugate to a distinct one. Consequently, the number of conjugacy classes equals the order of GG, and this singleton property characterizes abelian groups among all groups. In the general linear group GL(n,F)\mathrm{GL}(n, F) over a field FF, conjugacy classes correspond precisely to similarity classes of invertible n×nn \times n matrices. Two matrices A,BGL(n,F)A, B \in \mathrm{GL}(n, F) are conjugate if there exists invertible PGL(n,F)P \in \mathrm{GL}(n, F) such that B=P1APB = P^{-1} A P, which is the definition of similarity; this equivalence preserves properties like eigenvalues and Jordan form. For example, in GL(2,C)\mathrm{GL}(2, \mathbb{C}), classes include diagonalizable matrices with distinct eigenvalues, scalar matrices, and non-diagonalizable Jordan blocks, each classified by their characteristic polynomials or minimal polynomials.

Core Properties

Basic Properties

In group theory, the conjugacy class of an element gg in a group GG, denoted Cl(g)\mathrm{Cl}(g), consists of all elements of the form k1gkk^{-1} g k for kGk \in G. These classes partition the group GG into disjoint subsets, meaning every element of GG belongs to exactly one conjugacy class, and the classes are pairwise disjoint. The centralizer of gg in GG, denoted ZG(g)Z_G(g) or CG(g)C_G(g), is the subgroup defined by ZG(g)={kGk1gk=g}Z_G(g) = \{ k \in G \mid k^{-1} g k = g \}, which is equivalently the set of elements that commute with gg. The size of the conjugacy class Cl(g)\mathrm{Cl}(g) is given by the index of the centralizer in GG: Cl(g)=[G:ZG(g)]=G/ZG(g)|\mathrm{Cl}(g)| = [G : Z_G(g)] = |G| / |Z_G(g)|. This follows from the orbit-stabilizer theorem applied to the conjugation action, where ZG(g)Z_G(g) acts as the stabilizer of gg. The center of the group, Z(G)={zGzk=kz kG}Z(G) = \{ z \in G \mid z k = k z \ \forall k \in G \}, is the union of all singleton conjugacy classes, as each central element zz satisfies k1zk=zk^{-1} z k = z for all kGk \in G, making Cl(z)={z}\mathrm{Cl}(z) = \{ z \}. Conjugacy classes are invariant under inner s of GG, which are the automorphisms of the form ϕk:xk1xk\phi_k: x \mapsto k^{-1} x k for fixed kGk \in G; applying such an automorphism maps each class to itself.

Conjugacy Class Equation

The conjugacy class equation is a fundamental theorem in finite group theory that expresses the order of a finite group GG as the sum of the orders of its distinct conjugacy classes. Specifically, if {g1,g2,,gk}\{ g_1, g_2, \dots, g_k \} is a set of representatives, one from each conjugacy class of GG, then G=i=1kCl(gi),|G| = \sum_{i=1}^k |\mathrm{Cl}(g_i)|, where Cl(gi)\mathrm{Cl}(g_i) denotes the conjugacy class of gig_i. This equation arises from applying the orbit-stabilizer theorem to the conjugation action of GG on itself. For each element gGg \in G, the orbit under this action is precisely the conjugacy class Cl(g)\mathrm{Cl}(g), and the stabilizer is the centralizer CG(g)C_G(g) of gg in GG. The orbit-stabilizer theorem thus yields Cl(g)=G/CG(g)|\mathrm{Cl}(g)| = |G| / |C_G(g)|. Summing this relation over one representative from each conjugacy class partitions GG into disjoint classes and recovers the class equation. A key implication is that each conjugacy class size divides the order of the group, since CG(g)|C_G(g)| is the index of the centralizer in GG, and thus Cl(g)|\mathrm{Cl}(g)| divides G|G|. This divisibility property provides constraints on the possible structures of s. The conjugacy class equation emerged in the 19th-century development of finite group theory, with foundational contributions from , who introduced the notion of conjugate permutations in 1844.

Equation Illustration

To illustrate the conjugacy class equation, consider the dihedral group D4D_4 of order 8, which consists of the symmetries of a square: four rotations and four reflections. This non-abelian group provides a concrete example where the equation G=Cl(g)|G| = \sum |Cl(g)| (sum over class representatives gg) can be computed explicitly, revealing the structure through class sizes greater than 1. The elements of D4D_4 are denoted as ee (identity), rr (90° rotation), r2r^2 (180° rotation), r3r^3 (270° rotation), and reflections ss, srsr, sr2sr^2, sr3sr^3, satisfying r4=er^4 = e, s2=es^2 = e, and srs1=r1srs^{-1} = r^{-1}. To determine the conjugacy classes, compute the orbit of each element under conjugation, or equivalently, use the formula Cl(g)=D4/CD4(g)|Cl(g)| = |D_4| / |C_{D_4}(g)|, where CD4(g)C_{D_4}(g) is the centralizer of gg. The identity ee commutes with all elements, so CD4(e)=D4C_{D_4}(e) = D_4 (order 8) and Cl(e)={e}Cl(e) = \{e\} (size 1). The element r2r^2 lies in the center Z(D4)={e,r2}Z(D_4) = \{e, r^2\} and also commutes with everything, yielding CD4(r2)=D4C_{D_4}(r^2) = D_4 (order 8) and Cl(r2)={r2}Cl(r^2) = \{r^2\} (size 1). For rr, the centralizer is the rotation subgroup r={e,r,r2,r3}\langle r \rangle = \{e, r, r^2, r^3\} (order 4), since reflections conjugate rr to r3r^3 (e.g., srs1=r1=r3s r s^{-1} = r^{-1} = r^3), but rotations fix it. Thus, Cl(r)=8/4=2|Cl(r)| = 8/4 = 2, and Cl(r)={r,r3}Cl(r) = \{r, r^3\}. By symmetry, Cl(r3)=Cl(r)Cl(r^3) = Cl(r). The reflections split into two classes. For ss (reflection over a horizontal axis), the centralizer is {e,r2,s,sr2}\{e, r^2, s, sr^2\} (order 4), as it includes the center and reflections over parallel axes; conjugations by rotations yield sr2sr^2, while others map to the other type. Thus, Cl(s)=8/4=2|Cl(s)| = 8/4 = 2 and Cl(s)={s,sr2}Cl(s) = \{s, sr^2\}. Similarly, for srsr (diagonal reflection), CD4(sr)={e,r2,sr,sr3}C_{D_4}(sr) = \{e, r^2, sr, sr^3\} (order 4), giving Cl(sr)={sr,sr3}Cl(sr) = \{sr, sr^3\} (size 2). The conjugacy classes are therefore {e}\{e\}, {r2}\{r^2\}, {r,r3}\{r, r^3\}, {s,sr2}\{s, sr^2\}, and {sr,sr3}\{sr, sr^3\}, with sizes 1, 1, 2, 2, 2. The class equation verifies: 8=1+1+2+2+28 = 1 + 1 + 2 + 2 + 2. The presence of three classes of size 2 highlights the non-abelian nature, as all classes would be singletons in an abelian group.

Group Action Perspective

Conjugacy as Group Action

The conjugation action provides a natural framework for understanding conjugacy classes through the lens of group actions. Consider a group GG acting on itself by conjugation, defined by the map ϕ:G×GG\phi: G \times G \to G where ϕ(k,g)=k1gk\phi(k, g) = k^{-1} g k for k,gGk, g \in G. This action satisfies the axioms: the acts as the identity map, and the action is compatible with the group operation in GG. Under this action, the orbit of an element gGg \in G is the set {k1gkkG}\{ k^{-1} g k \mid k \in G \}, which is precisely the conjugacy class of gg. Thus, the conjugacy classes of GG partition GG into the orbits of this conjugation action. The stabilizer of gg under this action is the centralizer CG(g)={kGk1gk=g}C_G(g) = \{ k \in G \mid k^{-1} g k = g \}, the subgroup of elements that commute with gg. By the orbit-stabilizer theorem, the size of the conjugacy class of gg is G/CG(g)|G| / |C_G(g)|, assuming GG is finite. This action corresponds to the ψ:GAut(G)\psi: G \to \mathrm{Aut}(G) given by ψ(k)(g)=k1gk\psi(k)(g) = k^{-1} g k, whose image is the group Inn(G)\mathrm{Inn}(G) and kernel is the center Z(G)={zGzg=gz gG}Z(G) = \{ z \in G \mid zg = gz \ \forall g \in G \}. Consequently, the conjugation action factors through the action of Inn(G)\mathrm{Inn}(G) on GG.

Subgroups and Subsets

In group theory, the concept of conjugacy extends naturally from individual elements to subgroups. For a subgroup HH of a group GG and an element gGg \in G, the conjugate subgroup HgH^g is defined as Hg=g1Hg={g1hghH}H^g = g^{-1} H g = \{ g^{-1} h g \mid h \in H \}. This set HgH^g is itself a subgroup of GG isomorphic to HH, preserving the group structure under conjugation. The conjugacy classes of subgroups arise from the action of GG by conjugation on the lattice of its subgroups. Specifically, two subgroups HH and KK of GG belong to the same conjugacy class if there exists gGg \in G such that K=HgK = H^g; the conjugacy class of HH is then the {HggG}\{ H^g \mid g \in G \} under this action. A subgroup HH forms a singleton conjugacy class—meaning it is fixed under conjugation by every element of GG, so Hg=HH^g = H for all gGg \in G—precisely when HH is normal in GG. This conjugation action applies more broadly to arbitrary subsets of GG. For a subset SGS \subseteq G and gGg \in G, the conjugate SgS^g is Sg=g1Sg={g1sgsS}S^g = g^{-1} S g = \{ g^{-1} s g \mid s \in S \}. The conjugacy classes of such subsets are the orbits under the conjugation action, partitioning the power set of GG into equivalence classes where subsets are related by relabeling via inner automorphisms. A significant application of subgroup conjugacy appears in the , which describe the structure of s via their Sylow pp-subgroups for primes pp dividing the group order. The second Sylow theorem states that all Sylow pp-subgroups of a GG are conjugate to each other, forming a single conjugacy class under the action of GG by conjugation. This conjugacy ensures that Sylow pp-subgroups are indistinguishable up to relabeling, providing a tool to classify group structures and count such subgroups modulo pp.

Interpretations and Applications

Geometric Interpretation

In the general linear group GL(n,R)\mathrm{GL}(n, \mathbb{R}), conjugacy classes correspond to similarity classes of matrices, where two matrices AA and BB are conjugate if there exists an PGL(n,R)P \in \mathrm{GL}(n, \mathbb{R}) such that B=P1APB = P^{-1} A P. Geometrically, this equivalence means that AA and BB describe the same linear transformation relative to different bases, preserving the intrinsic structure of eigenspaces and generalized eigenspaces in the Rn\mathbb{R}^n. Over algebraically closed fields such as C\mathbb{C}, these classes are determined by the Jordan canonical form, which decomposes the matrix into a block-diagonal arrangement of Jordan blocks; each block visualizes a chain of generalized eigenvectors associated with an eigenvalue, highlighting the of the kernel (geometric multiplicity) and the full eigenspace deficiency relative to diagonalizability. This form provides a spatial to the "shape" of the transformation, where larger blocks indicate longer chains of non-trivial actions beyond mere scaling. In the symmetric group SnS_n, conjugacy classes are indexed by partitions of nn corresponding to cycle types, which geometrically represent the permutation as a disjoint union of cycles acting on the set {1,2,,n}\{1, 2, \dots, n\}, akin to orbiting subsets or loops in a graphical decomposition. Two permutations belong to the same class if they induce the same pattern of cycle lengths, interpretable as the topology of the permutation's action: for instance, a cycle of length kk traces a kk-sided polygon in the functional graph, while multiple cycles of equal length suggest symmetric rearrangements like parallel circuits. This cycle-type classification offers a visual pattern recognition, where the partition visually encodes the "skeleton" of the permutation's dynamics without regard to labeling of elements. A particularly intuitive visualization arises in S3S_3, isomorphic to the of symmetries of an , where the three conjugacy classes align with geometric transformation types: the identity (cycle type 1+1+11+1+1), the three transpositions (cycle type 2+12+1) as reflections over altitudes, and the two 3-cycles (cycle type 33) as 120° and 240° rotations around the . This separation geometrically distinguishes orientation-preserving motions (rotations, forming the alternating subgroup A3A_3) from orientation-reversing flips (reflections), illustrating how conjugacy classes capture distinct "motions" in the of a spatial object. For Lie groups, conjugacy classes in the group GG correspond to adjoint orbits in the Lie algebra g\mathfrak{g} under the adjoint action Adg(X)=gXg1\mathrm{Ad}_g(X) = g X g^{-1} for XgX \in \mathfrak{g}, providing a differential geometric interpretation as submanifolds foliating g\mathfrak{g}. These orbits geometrically represent the "level sets" of the adjoint representation, where each orbit is a homogeneous space diffeomorphic to G/ZG(X)G / Z_G(X) (with ZG(X)Z_G(X) the centralizer), and their symplectic structure (via Kirillov-Kostant-Souriau) endows them with a phase-space analogy, visualizing the decomposition of elements into semisimple and nilpotent parts through coadjoint orbits in g\mathfrak{g}^*. In compact Lie groups, such orbits are compact Kähler manifolds, offering a spatial embedding that highlights the curvature and connectivity induced by the group's exponential map.

Representations Connection

In the representation theory of finite groups over the complex numbers, characters play a central role in connecting conjugacy classes to irreducible representations. A character χV\chi_V of a representation (V,ρ)(V, \rho) of a finite group GG is defined by χV(g)=tr(ρ(g))\chi_V(g) = \operatorname{tr}(\rho(g)) for gGg \in G, and it is a class function, meaning χV(hgh1)=χV(g)\chi_V(hgh^{-1}) = \chi_V(g) for all hGh \in G. Thus, the value of χV\chi_V is constant on each conjugacy class of GG, allowing characters to be viewed as functions on the set of conjugacy classes rather than individual elements. The space of all class functions, denoted cf(G)\operatorname{cf}(G), forms a vector space of dimension equal to the number of conjugacy classes in GG. The irreducible characters {χi}\{\chi_i\}, where each χi\chi_i is the character of an irreducible representation, form an orthonormal basis for cf(G)\operatorname{cf}(G) with respect to the inner product ϕ,ψ=1GgGϕ(g)ψ(g)\langle \phi, \psi \rangle = \frac{1}{|G|} \sum_{g \in G} \phi(g) \overline{\psi(g)}. Since class functions are constant on conjugacy classes, this inner product can be rewritten as a sum over conjugacy classes: χi,χj=1Gclasses ClClχi(Cl)χj(Cl)\langle \chi_i, \chi_j \rangle = \frac{1}{|G|} \sum_{\text{classes } Cl} |\mathrm{Cl}| \chi_i(\mathrm{Cl}) \overline{\chi_j(\mathrm{Cl})}, where the orthogonality yields χi,χj=δij\langle \chi_i, \chi_j \rangle = \delta_{ij}. Equivalently, the unnormalized orthogonality relation is classes Clχi(Cl)χj(Cl)Cl=Gδij\sum_{\text{classes } Cl} \chi_i(\mathrm{Cl}) \overline{\chi_j(\mathrm{Cl})} |\mathrm{Cl}| = |G| \delta_{ij}. This basis property implies that the number of irreducible representations (up to isomorphism) equals the dimension of cf(G)\operatorname{cf}(G), which is the number of conjugacy classes in GG. The Frobenius-Schur indicator provides further insight into the nature of irreducible representations by detecting whether they are realizable over the real numbers, with a direct computation involving character values on conjugacy classes. For an irreducible character χ\chi of GG, the indicator is ε(χ)=1GgGχ(g2)\varepsilon(\chi) = \frac{1}{|G|} \sum_{g \in G} \chi(g^2), which takes values in {0,1,1}\{0, 1, -1\}. This sum groups terms by conjugacy classes of squares g2g^2, but more importantly, ε(χ)=1\varepsilon(\chi) = 1 if and only if χ\chi is real-valued (i.e., χ(g)R\chi(g) \in \mathbb{R} for all gGg \in G, hence on all conjugacy classes) and the representation is realizable over R\mathbb{R} with a symmetric invariant bilinear form; ε(χ)=1\varepsilon(\chi) = -1 if χ\chi is real-valued but the representation requires quaternions with a skew-symmetric form; and ε(χ)=0\varepsilon(\chi) = 0 otherwise, indicating no real realization. Real conjugacy classes, those satisfying Cl(g)=Cl(g1)\mathrm{Cl}(g) = \mathrm{Cl}(g^{-1}), are precisely the classes on which all irreducible characters take real values, linking the indicator to the group's real class structure. A key application arises from these relations in counting irreducible representations via averaging over the group. The orthogonality of irreducible characters implies that the regular representation decomposes as a direct sum of each irreducible representation with multiplicity equal to its degree, leading to the identity G=iχi(1)2|G| = \sum_i \chi_i(1)^2, where the sum is over irreducible characters. By projecting onto class functions using the inner product (an averaging process), one recovers the basis property and confirms that the number of irreducible representations equals the number of conjugacy classes, a fundamental result in character theory often proved by decomposing the space of class functions. This averaging technique underscores how conjugacy classes parametrize the irreducible representations, enabling explicit computations of character tables for groups like symmetric groups.

References

  1. https://groupprops.subwiki.org/wiki/Symmetric_group:S3
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