Definition
A vector space V over a field K (usually R or C) is a set with two operations:
- Addition: u+v∈V
- Scalar multiplication: au∈V for a∈K
satisfying:
| Property | Condition |
|---|
| Closure | u+v∈V, au∈V |
| Commutativity | u+v=v+u |
| Associativity | (u+v)+w=u+(v+w) |
| Zero vector | ∃0:u+0=u |
| Additive inverse | ∃(−u):u+(−u)=0 |
| Distributivity 1 | a(u+v)=au+av |
| Distributivity 2 | (a+b)u=au+bu |
| Compatibility | a(bu)=(ab)u |
| Identity | 1u=u |
Examples
| Vector Space | Elements | Field |
|---|
| Rn | n-tuples (x1,…,xn) | R |
| Matrices Mm,n | m×n matrices | R |
| Polynomials Pn | Degree ≤n polynomials | R |
| Functions C[a,b] | Continuous functions on [a,b] | R |
Linear Combinations
A linear combination of vectors v1,…,vm is:
a1v1+a2v2+⋯+amvm
where ai∈K are scalars.
Linear Independence
Vectors v1,…,vm are linearly independent if:
a1v1+⋯+amvm=0⇒a1=⋯=am=0

Equivalently: no vector can be written as a combination of the others.
Test: Set up the linear combination equal to zero, solve for coefficients.
Span
The span of vectors v1,…,vm is:
span{v1,…,vm}={a1v1+⋯+amvm:ai∈K}
All linear combinations of the vectors.
Basis and Dimension
A basis for V is a set of vectors that:
- Is linearly independent
- Spans V
The dimension dim(V) is the number of vectors in any basis.
Key theorem: All bases have the same number of vectors.
Example: R3
Standard basis: e1=(1,0,0), e2=(0,1,0), e3=(0,0,1)
Any vector: v=v1e1+v2e2+v3e3
Dimension: dim(R3)=3
Important Result
If v1,…,vm are linearly independent in V and dim(V)=m, then they form a basis.
In Rn:
- More than n vectors → linearly dependent
- Fewer than n vectors → cannot span
Why Vector Spaces Matter
- Unify disparate objects (vectors, matrices, functions) under one framework
- Enable general results applicable to all linear problems
- Foundation for quantum mechanics (Hilbert spaces)
- Underpin linear algebra (matrices represent linear maps between vector spaces)
The abstraction reveals common structure across seemingly different mathematical objects.