4.1 Groups

Every definition of an abstract object consists of two parts:

  1. in the first part we list all the data required for the definition,

  2. in the second part we list all the axioms the data must satisfy.

Groups


Data:

  • A set G G

  • An operation ○:G×G→G white circle colon G times G right arrow G

Axioms:

  • The operation ○ white circle is associative.

  • The operation ○ white circle has a neutral element.

  • Every element x∈G x is a member of G has an inverse.

In this case, we say that the pair (G,○) open paren G comma white circle close paren is a group. In order to simplify the notation, we usually say simply that G G is a group assuming that the operation in use is clear. If in addition we have

  • The operation ○ white circle is commutative.

Then the group G G is called abelian or simply commutative.

In short, a group is a set with a good operation.

Here, good means that we do not care about parentheses, we have neutral element and every element is invertible but the order of the elements still matters.

Abelian group means that additionally the order of the elements does not matter.

Subgroups


Let G G be a group. We define a subgroup H H of G G.

Data:

  • A subset H⊆G H subset of or equal to G.

Axioms:

  • The neutral element 1 1 of G G belongs to H H.

  • x⁢y∈H x y is a member of Hwheneverx⁢y∈H x y is a member of H.

  • x-1∈H x to the negative 1 power is a member of Hwheneverx∈H x is a member of H.

In this case, we say that H H is a subgroup of G G.

It should be noted that if H H is a subgroup of G G, then ⋅ times is a well-defined operation on H H and (H,⋅) open paren H comma times close paren becomes a group.

Cosets


Algebra usually tends to study groups using subgroups rather than elements. The main tool here is cosets.

Let G G be a group, H⊆G H subset of or equal to G a subgroup and g∈G g is a member of G an arbitrary element. Then the set

g⁢H={g⁢h|h∈H} g H equals the set of all g h such that h is a member of H

is called the left coset of H H with respect to g g. In a similar way, we define right cosets. The set

H⁢g={h⁢g|h∈H} H g equals the set of all h g such that h is a member of H

is called the right coset of H H with respect to g g.

The Lagrange Theorem


Let G G be a finite group and H⊆G H subset of or equal to G be a subgroup. Then, |G|=(G:H)⁢|H| the absolute value of G equals open paren G colon H close paren times the absolute value of H

Corollaries of The Lagrange Theorem


  1. Let G G be a finite group and H⊆G H subset of or equal to G be a subgroup. Then |H| the absolute value of H divides |G| the absolute value of G.

  2. Let G G be a finite group and g∈G g is a member of G be an arbitrary element. Then ord(g) g divides |G| the absolute value of G. Indeed, ord(g)=|⟨g⟩| g equals the absolute value of left angle bracket g right angle bracket. But |⟨g⟩| the absolute value of left angle bracket g right angle bracket divides |G| the absolute value of G by the previous item.

  3. Let G G be a finite group and g∈G g is a member of G be an arbitrary element. Then g|G|=1 the the absolute value of G power of g equals 1. Indeed, we already know that |G|= the absolute value of G equalsord(g)⁢k g times k. Hence,

    g|G|=gord⁢(g)⁢k=(gord⁢(g))k=1k=1 the the absolute value of G power of g equals the number o r d times g-th times k-th power of g equals open paren the number o r d times g-th power of g close paren to the k-th power equals 1 to the k-th power equals 1

  4. Let G G be a group of prime order p p. Then, G G is cyclic. Indeed, since the order of G G is prime, it is greater than 1 1. Hence, there is an element g∈G g is a member of G such that g≠1 g is not equal to 1. Hence ⟨g⟩ left angle bracket g right angle bracket has order greater than 1 1. But |⟨g⟩| the absolute value of left angle bracket g right angle bracket divides |G|=p the absolute value of G equals p. Since p p is prime, the only option is |⟨g⟩|=p=|G| the absolute value of left angle bracket g right angle bracket equals p equals the absolute value of G. The latter means that ⟨g⟩=G left angle bracket g right angle bracket equals G and we are done.

  5. The Fermat Little Theorem. Let p∈ℤ p is a member of the integers be a prime number and a∈ℤ a is a member of the integers. If p p does not divide a a, then p p divides ap-1-1 a raised to the p minus 1 power minus 1. Indeed, let us consider the group (ℤp∗,⋅) open paren the integers sub p raised to the asterisk power comma times close paren. For any element b∈ℤp∗ b is a member of the integers sub p raised to the asterisk power, we have b|ℤp∗|=1⁢mod⁡(p) b raised to the exponent the absolute value of the integers sub p raised to the asterisk power end exponent equals 1 mod p by item~3. 3 period But ℤp∗ the integers sub p raised to the asterisk power has p-1 p minus 1 elements. Now, let a∈ℤ a is a member of the integers be comprime with p p. We denote its remainder modulo p p by b b. Then ap-1=bp-1=1⁢mod⁡(p) a raised to the p minus 1 power equals b raised to the p minus 1 power equals 1 mod p and we are done.