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Notes on Group Theory

David K. Zhang
Last Modified 2024-01-02

Introduction

Group theory is the first subject in a field of mathematics known as abstract algebra or modern algebra. Abstract algebra is one of the main branches of modern pure mathematics, and every mathematician, scientist, or engineer who wants a firm understanding of theoretical foundations should know a thing or two about group theory.

The goal of abstract algebra is to study the properties of algebraic systems and the interrelations between them. For example, you probably know about a handful of different number systems, including the integers Z\Z, the rational numbers Q\Q, the real numbers R\R, and possibly the complex numbers C\C. You may have also learned about their algebraic properties, such as the commutative property of addition, x+y=y+xx + y = y + x, and the associative property of multiplication, x⋅(y⋅z)=(x⋅y)⋅zx \cdot (y \cdot z) = (x \cdot y) \cdot z.

In abstract algebra, we will go beyond these familiar number systems to study the properties of algebraic systems in general. We will learn how these properties can inform us about the structure of an unknown algebraic system, and we will see how this knowledge can be used to quickly and easily solve problems that would otherwise be difficult or tedious.

To begin our study of abstract algebra, we will focus on one particular type of algebraic system, known as a group. Groups are an ideal starting point because they strike an excellent balance between simplicity and complexity. They are straightforward to define, involving only a single binary operation, and yet they capture most of the key ideas used to study more complicated algebraic structures. In addition, groups are widely used in both pure and applied contexts. Group theory plays a foundational role not only in abstract algebra itself, but also in mathematical analysis, combinatorics, cryptography, physics, chemistry, and materials science.

Groups

Definition: Group

A group is an algebraic structure ⟨G;1,−1,⋅⟩\alg{G; 1, {}^{-1}, \cdot} consisting of:

  • a set GG, called the underlying set;
  • a distinguished element 1∈G1 \in G, called the identity element;
  • a unary operation −1:G→G{}^{-1}: G \to G, written as x↦x−1x \mapsto x^{-1}, called inversion;
  • a binary operation ⋅:G×G→G\cdot : G \times G \to G, written as (x,y)↦x⋅y(x, y) \mapsto x \cdot y, called the group operation or group product;

satisfying the following requirements:

  • Associative property: (x⋅y)⋅z=x⋅(y⋅z)(x \cdot y) \cdot z = x \cdot (y \cdot z) for all x,y,z∈Gx, y, z \in G.
  • Identity property: 1⋅x=x1 \cdot x = x for all x∈Gx \in G.
  • Inverse property: x−1⋅x=1x^{-1} \cdot x = 1 for all x∈Gx \in G.

The commutative property (x⋅y=y⋅x)(x \cdot y = y \cdot x) is conspicuously absent from the definition of a group.

Identity is the Only Idempotent

Theorem: Let ⟨G;1,−1,⋅⟩\alg{G; 1, {}^{-1}, \cdot} be a group. The only element x∈Gx \in G having the property that x⋅x=xx \cdot x = x is the identity element.


Proof: First, to see that the identity element 1∈G1 \in G actually has the claimed property, observe that 1⋅1=11 \cdot 1 = 1 follows from the identity property.

Next, to see that no other element of GG has this property, let x∈Gx \in G be given, and suppose x⋅x=xx \cdot x = x. By multiplying both sides by x−1x^{-1} on the left, we have x−1⋅(x⋅x)=x−1⋅xx^{-1} \cdot (x \cdot x) = x^{-1} \cdot x, from which it follows that:

x=1⋅x=(x−1⋅x)⋅x=x−1⋅(x⋅x)=x−1⋅x=1 x = 1 \cdot x = (x^{-1} \cdot x) \cdot x = x^{-1} \cdot (x \cdot x) = x^{-1} \cdot x = 1

Thus, we have proven that x⋅x=xx \cdot x = x implies x=1x = 1. ∎

Right Inverse Property

Theorem: Let ⟨G;1,−1,⋅⟩\alg{G; 1, {}^{-1}, \cdot} be a group. For all x∈Gx \in G, we have x⋅x−1=1x \cdot x^{-1} = 1.


Proof: Let x∈Gx \in G be given. We know, from the definition of a group, that x−1⋅x=1x^{-1} \cdot x = 1 and 1⋅x−1=x−11 \cdot x^{-1} = x^{-1}. It follows that:

x⋅x−1=x⋅(1⋅x−1)=x⋅((x−1⋅x)⋅x−1)=x⋅(x−1⋅(x⋅x−1))=(x⋅x−1)⋅(x⋅x−1) x \cdot x^{-1} = x \cdot (1 \cdot x^{-1}) = x \cdot ((x^{-1} \cdot x) \cdot x^{-1}) = x \cdot (x^{-1} \cdot (x \cdot x^{-1})) = (x \cdot x^{-1}) \cdot (x \cdot x^{-1})

This shows that the element x⋅x−1∈Gx \cdot x^{-1} \in G remains unchanged when it is multiplied by itself. Using the previous result, this proves that x⋅x−1=1x \cdot x^{-1} = 1. ∎

Right Identity Property

Theorem: Let ⟨G;1,−1,⋅⟩\alg{G; 1, {}^{-1}, \cdot} be a group. For all x∈Gx \in G, we have x⋅1=xx \cdot 1 = x.


Proof: Let x∈Gx \in G be given. We know, from the definition of a group, that x−1⋅x=1x^{-1} \cdot x = 1 and 1⋅x=x1 \cdot x = x. It follows that:

x⋅1=x⋅(x−1⋅x)=(x⋅x−1)⋅x=1⋅x=x x \cdot 1 = x \cdot (x^{-1} \cdot x) = (x \cdot x^{-1}) \cdot x = 1 \cdot x = x

This proves that x⋅1=xx \cdot 1 = x. ∎

Subgroups

Definition: Subgroup, H≤GH \le G

Let ⟨G;1,−1,⋅⟩\alg{G; 1, {}^{-1}, \cdot} be a group. A subgroup of ⟨G;1,−1,⋅⟩\alg{G; 1, {}^{-1}, \cdot} is a subset H⊆GH \subseteq G of its underlying set that satisfies the following requirements:

  • 1∈H1 \in H.
  • If x∈Hx \in H, then x−1∈Hx^{-1} \in H.
  • If x,y∈Hx, y \in H, then x⋅y∈Hx \cdot y \in H.

We write H≤GH \le G to denote that HH is a subgroup of ⟨G;1,−1,⋅⟩\alg{G; 1, {}^{-1}, \cdot}.

In other words, HH is a subgroup of GG if and only if the structure ⟨H;1,−1∣H,⋅∣H⟩\alg{H; 1, {}^{-1}|_H, \cdot|_H} is a group in its own right, where −1∣H{}^{-1}|_H and ⋅∣H\cdot|_H denote the inverse operation −1{}^{-1} and the group operation ⋅\cdot restricted to HH and H×HH \times H, respectively.

This definition introduces an important notational convention. We will often refer to a group ⟨G;1,−1,⋅⟩\alg{G; 1, {}^{-1}, \cdot} simply by the name of its underlying set GG, omitting explicit mention of the identity element, the inversion operation, and the group operation.

It is also common in the mathematics literature to not use any symbol, such as x×yx \times y or x⋅yx \cdot y, to denote the binary operation in a group. Instead, most mathematicians simply write xyxy, using juxtaposition to indicate application of the group operation. Note that the associative property allows us to write expressions like xyzxyz without needing to specify which product should be evaluated first, since both (xy)z(xy)z and x(yz)x(yz) are guaranteed to produce the same result.


Definition: Commute, Commutes

Let GG be a group. We say that two elements x,y∈Gx, y \in G commute, or we say that xx commutes with yy, if xy=yxxy = yx.

Definition: Central Element, Center, Z(G)Z(G)

Let GG be a group. An element x∈Gx \in G is central if xx commutes with every element of GG. The set of all central elements of GG is called the center of GG, and is denoted by Z(G)Z(G).

Z(G)≔{x∈G:∀y∈G, xy=yx} Z(G) \coloneqq \{ x \in G : \forall y \in G,\ xy = yx \}

Definition: Abelian Group

An abelian group is a group ⟨G;1,−1,⋅⟩\alg{G; 1, {}^{-1}, \cdot} that satisfies the following additional requirement:

  • Commutative property: x⋅y=y⋅xx \cdot y = y \cdot x for all x,y∈Gx, y \in G.

Definition: Left Coset, Right Coset, G/HG/H, H\GH \backslash G

Let GG be a group, and let H≤GH \le G be a subgroup. A left coset of HH is a set of the form

gH≔{gh:h∈H} gH \coloneqq \{ gh : h \in H \}

for some fixed element g∈Gg \in G. Similarly, a right coset of HH is a set of the form

Hg≔{hg:h∈H} Hg \coloneqq \{ hg : h \in H \}

for some fixed element g∈Gg \in G. The collection of all left cosets of HH is denoted by G/HG/H, while the collection of all right cosets of HH is denoted by H\GH \backslash G.

This definition introduces a new notational convention. Whenever we apply a group operation, such as gHgH or H−1H^{-1}, to a subset of a group, we mean the set formed by applying that operation to each element of the subset. For example:

gH≔{gh:h∈H}H−1≔{h−1:h∈H}g1Hg2≔{g1hg2:h∈H} \begin{aligned} gH &\coloneqq \{ gh : h \in H \} \\ H^{-1} &\coloneqq \{ h^{-1} : h \in H \} \\ g_1 H g_2 &\coloneqq \{ g_1 h g_2 : h \in H \} \end{aligned}

Note that we can write g1Hg2g_1 H g_2 without ambiguity, since the associative property guarantees that (g1H)g2=g1(Hg2)(g_1 H) g_2 = g_1 (H g_2).

Definition: Index, ∣G:H∣\abs{G:H}

Let GG be a group, and let H≤GH \le G be a subgroup. The index of HH in GG, denoted by ∣G:H∣\abs{G:H}, is the cardinality of the

Cosets Partition a Group

Theorem: Let GG be a group, and let H≤GH \le G be a subgroup.


Proof:

Suppose two cosets xHxH and yHyH of HH intersect, i.e., there exists an element z∈xH∩yHz \in xH \cap yH

Definition: Normal Subgroup

Let GG be a group. We say that a subgroup H≤GH \le G is normal if for all g∈Gg \in G and h∈Hh \in H, we have g−1hg∈Hg^{-1}hg \in H.

left conjugation — this is a left action

gx≔gxg−1 {}^g x \coloneqq g x g^{-1} h(gx)=h(gxg−1)=h(gxg−1)h−1=(hg)x(hg)−1=hgx {}^h ({}^g x) = {}^h (g x g^{-1}) = h (g x g^{-1}) h^{-1} = (hg) x (hg)^{-1} = {}^{hg} x

right conjugation — this is a right action

xg≔g−1xg x^g \coloneqq g^{-1} x g (xg)h=(g−1xg)h=h−1(g−1xg)h=(gh)−1x(gh)=xgh (x^g)^h = (g^{-1} x g)^h = h^{-1} (g^{-1} x g) h = (gh)^{-1} x (gh) = x^{gh}

Center is a Subgroup

Theorem: Let GG be a group. Its center Z(G)Z(G) is a subgroup of GG.


Proof: We must show that Z(G)Z(G) contains the identity element 11 and is closed under taking inverses and products.

  • Clearly, 1∈Z(G)1 \in Z(G), since the identity element 11 commutes with everything.
  • Let a∈Z(G)a \in Z(G) and g∈Gg \in G. By definition, we have ag=gaag = ga. By multiplying on the left and right by a−1a^{-1}, we obtain ga−1=a−1gga^{-1} = a^{-1}g. Hence, a−1a^{-1} commutes with gg. Since g∈Gg \in G was arbitrary, this proves that a−1∈Z(G)a^{-1} \in Z(G).
  • Let a,b∈Z(G)a, b \in Z(G) and g∈Gg \in G. Because aa and bb are central, we can write abg=agb=gababg = agb = gab. Hence, abab commutes with gg. Again, because g∈Gg \in G was arbitrary, this proves that ab∈Z(G)ab \in Z(G). ∎

Center is a Normal Subgroup

Theorem: Let GG be a group. Its center Z(G)Z(G) is a normal subgroup of GG.


Proof: Let g∈Gg \in G and z∈Z(G)z \in Z(G). Because zz is central, we have g−1zg=zg−1g=z∈Z(G)g^{-1}zg = zg^{-1}g = z \in Z(G). ∎