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Part IA Michaelmas, Lent, Easter Term

Vector Spaces

Definition

A vector space VV over a field KK (usually R\mathbb{R} or C\mathbb{C}) is a set with two operations:

  • Addition: u+vV\mathbf{u} + \mathbf{v} \in V
  • Scalar multiplication: auVa\mathbf{u} \in V for aKa \in K

satisfying:

PropertyCondition
Closureu+vV\mathbf{u} + \mathbf{v} \in V, auVa\mathbf{u} \in V
Commutativityu+v=v+u\mathbf{u} + \mathbf{v} = \mathbf{v} + \mathbf{u}
Associativity(u+v)+w=u+(v+w)(\mathbf{u} + \mathbf{v}) + \mathbf{w} = \mathbf{u} + (\mathbf{v} + \mathbf{w})
Zero vector0:u+0=u\exists\,\mathbf{0}: \mathbf{u} + \mathbf{0} = \mathbf{u}
Additive inverse(u):u+(u)=0\exists\,(-\mathbf{u}): \mathbf{u} + (-\mathbf{u}) = \mathbf{0}
Distributivity 1a(u+v)=au+ava(\mathbf{u} + \mathbf{v}) = a\mathbf{u} + a\mathbf{v}
Distributivity 2(a+b)u=au+bu(a + b)\mathbf{u} = a\mathbf{u} + b\mathbf{u}
Compatibilitya(bu)=(ab)ua(b\mathbf{u}) = (ab)\mathbf{u}
Identity1u=u1\mathbf{u} = \mathbf{u}

Examples

Vector SpaceElementsField
Rn\mathbb{R}^nnn-tuples (x1,,xn)(x_1, \ldots, x_n)R\mathbb{R}
Matrices Mm,nM_{m,n}m×nm \times n matricesR\mathbb{R}
Polynomials PnP_nDegree n\leq n polynomialsR\mathbb{R}
Functions C[a,b]C[a,b]Continuous functions on [a,b][a,b]R\mathbb{R}

Linear Combinations

A linear combination of vectors v1,,vm\mathbf{v}_1, \ldots, \mathbf{v}_m is:

a1v1+a2v2++amvma_1\mathbf{v}_1 + a_2\mathbf{v}_2 + \cdots + a_m\mathbf{v}_m

where aiKa_i \in K are scalars.


Linear Independence

Vectors v1,,vm\mathbf{v}_1, \ldots, \mathbf{v}_m are linearly independent if:

a1v1++amvm=0a1==am=0a_1\mathbf{v}_1 + \cdots + a_m\mathbf{v}_m = \mathbf{0} \Rightarrow a_1 = \cdots = a_m = 0

Linear independence in 2D - two non-collinear vectors are independent; three vectors in 2D are dependent

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\mathbf{v}_1, \ldots, \mathbf{v}_m is:

span{v1,,vm}={a1v1++amvm:aiK}\text{span}\{\mathbf{v}_1, \ldots, \mathbf{v}_m\} = \{a_1\mathbf{v}_1 + \cdots + a_m\mathbf{v}_m : a_i \in K\}

All linear combinations of the vectors.


Basis and Dimension

A basis for VV is a set of vectors that:

  1. Is linearly independent
  2. Spans VV

The dimension dim(V)\dim(V) is the number of vectors in any basis.

Key theorem: All bases have the same number of vectors.


Example: R3\mathbb{R}^3

Standard basis: e1=(1,0,0)\mathbf{e}_1 = (1,0,0), e2=(0,1,0)\mathbf{e}_2 = (0,1,0), e3=(0,0,1)\mathbf{e}_3 = (0,0,1)

Any vector: v=v1e1+v2e2+v3e3\mathbf{v} = v_1\mathbf{e}_1 + v_2\mathbf{e}_2 + v_3\mathbf{e}_3

Dimension: dim(R3)=3\dim(\mathbb{R}^3) = 3


Important Result

If v1,,vm\mathbf{v}_1, \ldots, \mathbf{v}_m are linearly independent in VV and dim(V)=m\dim(V) = m, then they form a basis.

In Rn\mathbb{R}^n:

  • More than nn vectors → linearly dependent
  • Fewer than nn 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.