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