Basis and Dimension
Bases for Vector Spaces
Definition 19: Basis Set
Let be a subset of a vector space . is a basis for iff the following conditions hold:
- Linear independence. is a linearly independent set.
- Spanning set. is a spanning set for , i.e. .
The elements of are called the basis vectors of under .
Example: Show that is a basis for .
Let , where and . We must show that is a linearly independent set and a spanning set for .
Linear independence. Suppose that are scalars such that . Then we have:
This gives us the system of equations:
Using elementary algebra, we can solve for and to find that and is the only solution. By Theorem 16, is a linearly independent set.
Spanning set. Let be an arbitrary vector in . We will show that there exist scalars such that , that is:
This gives us the system of equations:
Using elementary algebra, we find that and . Thus, by choosing and as such, we have . Since was an arbitrary vector in , we have shown that every vector in can be expressed as a linear combination of the vectors in , so is a spanning set for .
Since is a linearly independent set and a spanning set for , is a basis for . ∎
Nonexample.
Nonexample.
Terminology: Finite-Dimensional and Infinite-Dimensional Vector Spaces
A vector space is finite-dimensional iff there exists a basis for that is a finite set (called a finite basis). Otherwise, is infinite-dimensional and has an infinite basis.
Combining the two criteria from Definition 19, we can deduce the following:
Theorem 20: Unique Representation Theorem
A set of vectors is a finite basis for a vector space over if and only if for any , there is exactly one solution for the equation:
This theorem states that a basis for a vector space is a set of vectors from such that every vector in can be uniquely expressed as a linear combination of the vectors in .
This is a statement of uniqueness and existence:
- Uniqueness. Every vector in can be expressed as a linear combination of the vectors in in at most one way.
- Existence. Every vector in can be expressed as a linear combination of the vectors in in at least one way.
Proof: Unique Representation Theorem.
Suppose that is a basis for over . By the definition of a basis, is a linearly independent set and a spanning set for . Particularly, spans , so for any , there exists at least one solution for the equation:
Suppose is another solution to this equation. That is, suppose that:
By the definition of linear independence, we must have . Thus, for any , there is exactly one solution for the equation
The converse is trivial. ∎
Note
A common pattern for uniqueness and existence in proofs is that by showing uniqueness and existence, we can conclude that there is exactly one of something.
Theorem 21: Spanning Sets can be Reduced to a Basis
Let be a vector space, and let be a finite spanning set for . Then there exists an improper subset of that is a basis for .
Proof: Theorem 21.
Theorem 22: Linearly Independent Sets can be Extended to a Basis
Let be a vector space, and let be a finite linearly independent set of vectors from . Then there exists an improper superset of that is a basis for .
Proof: Theorem 22.
Let be a vector space, and let be a finite linearly independent set of vectors from . By the Characterization of Linearly Independent Sets,
Dimension of Vector Spaces
Theorem 23: Unique Size Theorem
Let be a finite-dimensional vector space. If and are two bases for , then . That is, all bases for have the same number of vectors.
Proof: Unique Size Theorem.
As a result of this theorem, we can define the dimension of a finite-dimensional vector space as the number of vectors in any basis for the vector space:
Definition 20: Dimension of a Vector Space
Let be a finite-dimensional vector space. The dimension of , denoted , is the number of vectors (the cardinality) in any basis for . To say that V is -dimensional means that .
Combining Theorem 23 and Definition 20 together, we see that although a finite-dimensional vector space can have many different bases, they all have the same number of vectors, namely number of vectors.
Corollary 9
A vector space is finite-dimensional if and only if is well-defined.
Important
The dimension of the trivial vector space is 0. That is, . It would then follow that the empty set is the only basis for .
Notation
An infinite-dimensional vector space may be said to have infinite dimension, and may be used to denote that is infinite-dimensional. This is an abuse of notation since is not well-defined for infinite-dimensional vector spaces.
Theorem 24: Basis Theorem
Let be a finite-dimensional vector space with dimension .
- If is a linearly independent set of vectors from , then is a basis for .
- If is a spanning set of vectors from , then is a basis for .
That is, if we know the dimension of a vector space and we have a set of exactly vectors from that vector space, then we only need to check one of the two criteria from Definition 19 to determine if that set is a basis for the vector space.
If the set of vectors is linearly independent, it is a basis, so we get spanning for free. If the set of vectors is a spanning set, it is a basis, so we automatically get linear independence for free.
Proof: Basis Theorem.
Suppose is a finite-dimensional vector space with dimension .
- Suppose is a linearly independent set of vectors. For the sake of contradiction, assume that is not a basis for . Then is not a spanning set for ( is already linearly independent, so the other condition of a basis cannot be true.) That is, there exists some vector such that . By Corollary 8, then, the set is linearly independent.
Proposition 6: Relative Dimensions of Subspaces
Let be a subspace of a finite-dimensional vector space . Then . Furthermore, if and only if .
Proof: Proposition 6.
Let be a subspace of a finite-dimensional vector space . Let and . Let be a basis for , and let be a basis for .
By Theorem 22, there exists an improper superset of that is a basis for . Since is a basis for , it must have the same number of vectors as any other basis for , including the improper superset of . Thus, the number of vectors in the improper superset of is equal to the number of vectors in , which is . Since the improper superset of contains all the vectors in , the number of vectors in the improper superset of is greater than or equal to the number of vectors in , which is . Therefore, we have:
Furthermore, if , then the improper superset of that is a basis for has the same number of vectors as , so must be the same set as the improper superset of , which is a basis for . Thus, is a basis for , so . ∎
Theorem 25: Dimension Formula
Let and be subspaces of a finite-dimensional vector space . Then:
Proof: Dimension Formula.
If is a direct sum, then which has dimension , so:
Corollary 10
If is a finite-dimensional vector space, then . By extension, if is finite-dimensional, then .
Basis Coordinates and the Standard Basis
Definition 21: Strictly Ordered Sets
A set is strictly partially ordered if there exists a binary predicate on such that:
- Irreflexivity. .
- Asymmetry. , if , then .
- Transitivity. , if and , then .
A strictly partially ordered set is strictly totally ordered if in addition to the above conditions, additionally satisfies:
- Totality. , if , then either or .
Definition 22: Ordered Basis
An ordered basis for is a basis for that is a strictly totally ordered set.
In other words, an ordered basis is a basis which defines precisely which basis vector is “first,” which is “second,” and so on.
Notation
In the context of a basis, a basis set written in the form induces a strict total ordering on the vectors in in the order in which they are written. That is, a strict ordering is induced on such that .
Notation
An ordered finite basis may be denoted as a list or tuple instead of a set.
Recall that by the Unique Representation Theorem, every vector in a vector space can be represented as a unique linear combination of vectors from a basis . With ordered, the weights of that linear combination can be properly defined:
Definition 23: Basis Coordinates
Let be an ordered, finite basis for a vector space over , and let be a vector in . The coordinates of with respect to the basis are the unique weights such that:
That is, the coordinates of with respect to are the weights of the unique linear combination of the vectors that represents .
A basis for over a field has number of vectors, so there would be number of coordinates for each vector in with respect to that basis. Thus, we can represent each vector in as an -tuple of coordinates in , where . An -tuple of coordinates in is an element of , so we can represent each vector in as a vector from . Specifically:
Definition 24: Basis Coordinate Vector
If are the coordinates of with respect to an ordered, finite basis for a vector space over , then the basis coordinate vector of with respect to , denoted , is the vector in given by:
This naturally leads to the fact that the vector space should have dimension , since it takes coordinates to represent each vector in :
Corollary 11
The vector space is -dimensional, i.e., .
Since is a vector space, it has a basis. In particular, the basis that self-describes the coordinates of vectors in is called the standard basis for :
Definition 25: Standard Basis
The standard basis for the vector space is the ordered basis , where is the vector in with the th coordinate set to and all other coordinates set to :
Example.
Corollary 12
For any , .
Notation
The standard basis for may be denoted or even to indicate that it is the standard basis for .
Exercises
Exercise 35.
Exercise 36.
Exercise 37: Extension of Theorem 13.
Exercise 38.
Exercise 39.
Exercise 40.
Suppose is a vector space and is a basis for . Show that for any ,
Exercise 41.
Exercise 42.
Suppose is a linearly independent set in , and . Show that:
Exercise 43.
For any three subspaces , , and of a finite-dimensional vector space , show that:
Exercise 44.
For any three subspaces , , and of a finite-dimensional vector space , show that: