Chapter 2 Groups and Vector Spaces

2.2 Groups

2.2.4 Lagrange’s Theorem

Lemma 2.26

Every coset of in a group has the same number of elements.

Proof:

Let the coset be . Then we can make an one-to-one mapping between and :

So has the same number of elements as .

Lemma 2.28

The distinct cosets of in a group are disjoint.

Proof:

Assume and are 2 distinct cosets of , assume , then we can find such that

, so we have , so . That means .

Then we reach a contradiction.

Theorem 2.29 (Lagrange’s theorem)

Let be a group of finite order and let be a subgroup of . Then the order of divides the order of . That is, divides .

Proof:

Just apply Lemma 2.26 and Lemma 2.28.

2.2.5 Induced Operations; Isomorphism

Definition 2.36

Let be a group, a subgroup and let be the set of cosets of in . Then the induced operation between cosets and in is defined by

for any and some , provided that this operation is well defined. The operation is well defined if for every and ; there is thus no ambiguity in the induced operation.

Theorem 2.38

If is a subgroup of a commutative group , the induced operation on the set of cosets of satisfies

Furthermore, the operation is well defined.

Proof:

We will prove it's well defined, Let , we want to show

Since , we have . Similarly, we have .

Since is commutative, . Since is a subgroup, .

So we have

Then the operation is well defined.

2.4 Review of Linear Algebra

Definition 2.62

Let be a -dimensional subspace of a vector space . The set of all vectors which are orthogonal to all the vectors of is called the dual space of (sometimes called the orthogonal complement of or dual space), denoted . (The symbol is sometimes pronounced perp,” for “perpendicular.”) That is,

Theorem 2.64

Let be a finite-dimensional vector space of -tuples, , with a subspace of dimension . Let be the dual space of . Then

Proof:

We will use a different approach compare to the textbook.

Let be the standard basis of . And be the dual basis of .

Then we can construct an isomorphism from

Then in fact, is isomorphic to the annihilator of , i.e. . From Linear Algebra Done Right 4th edition, 3.125 dimension of the annihilator, we know

So