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2.2. Bases.

The following definition is central to this topic.

Definition 2.15. A set ℬ = {v1,...,vr} is called a basis (for the vector space V  ) if ℬ  is a linearly independent spanning set. In other words, L(ℬ) = V  and ℬ  is linearly independent.

The following property of bases is fundamental.

Proposition 2.16. Let ℬ = {v ,...,v } 1     r be a basis for V  . Then every v ∈ V  can be written as a linear combination of the v
 i  in precisely one way.

Proof.Since ℬ  is a spanning set, every v ∈ V  can be written as a linear combination of elements in ℬ  . We must show that this linear combination is unique. Suppose that

∑r∑r
v =    λivi    and also    v =   λ ′ivi .i=1i=1

Then we have

∑r       ′     ∑r      ∑r   ′
   (λi - λi)vi =   λivi -    λivi = v- v = 0 .
i=1            i=1       i=1

Linear independence of ℬ  means that λi = λ′i  for all i  . □

Example 2.17. The set {e1,...,eN} consisting of elementary vectors in  N
ℝ  is called the canonical basis of  N
ℝ  .

Example 2.18. The set {eij} for i = 1,2,...,m  , j = 1,2,...,n  consisting of elementary matrices in Mm,n(ℝ)  is called the canonical basis of Mm,n( ℝ)  .

Proposition 2.19. If 𝒮  is a linearly independent subset of V  , it is a basis for L(𝒮)  .

Proof.By definition 𝒮  is a spanning set for L(𝒮)  . Since it is linearly independent, it is a basis for L(𝒮)  .□

There are two fundamental properties of vector spaces: there is always a basis and any two bases have the same cardinality. In particular, if a vector space is finite-dimensional (so that it has a finite spanning set), any two bases have the same number of elements. This will follow from the following two important results.