change of basis
Let V be a vector space. Given a basis A for V, each vector v∈V can be uniquely expressed in terms of the base elements vi∈A as follows:
v=∑vi∈Arivi |
where the sum is taken over a finite number of elements in A. Suppose now that B is another basis for V. By a change of basis from A to B we mean re-expressing v in terms of base elements wi∈B.
Formally, we can think of a change of basis as the identity function (viewed as a linear operator) on a vector space V, such that elements in the domain are expressed in terms of A and elements in the range are expressed in terms of B.
Note that, by the very design of a basis, a change of basis in a vector space is always possible.
Now, if V has dimension n<∞. We can total order bases A and B. Then a change of basis (from A to B) has the matrix representation
[I]AB, |
where I:V→V is the identity operator. [I]AB is called a change of basis matrix. By applying [I]AB to a vector v expressed in terms of A, we get v expressed in terms of B:
[v]B=[I]AB[v]A, |
where [v]A and [v]B are v expressed in the two bases A and B respectively.
Since I is obviously invertible, [I]AB is invertible also, whose inverse
is [I]BA. Furthermore, [I]A=In for any basis A. Here, In is the identity matrix
.
Examples.
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1.
Let V=ℝ3 and the following two sets
A={(1-12),(011),(230)} and B={(100),(010),(001)} be the two ordered bases for V, ordered in the way the elements are arranged in the set. For each vi∈A, I(vi)=vi=[vi]E3, we see that
[I]AB=(102-113210). Notice that the columns of [I]AB are exactly the elements of A. Indeed, each element of A is already written in terms of the standard basis elements (in B). For example, let v be the first basis element in A. Let us see what [v]A is, when expressed using base elements in B, the standard ordered basis:
[v]B=[I]AB[v]A=(102-113210)[v]A=(102-113210)(100)=(1-12), exactly as we have expected.
-
2.
Conversely, let w be the first basis element in B. What is w when expressed in terms of basis elements of A? In other words, we need to find
[w]A=[I]BA[w]B. Now, [w]B is just (100), so [w]A is nothing more than the first column of [I]BA, which is just the inverse of the matrix [I]AB, so
[I]BA=([I]AB)-1=(102-113210)-1=(1/3-2/92/9-2/34/95/91/31/9-1/9). Therefore, [w]A=(1/3-2/31/3). A quick verification shows that this is indeed the case:
(100)=(1/3)(1-12)+(-2/3)(011)+(1/3)(230). -
3.
Now let C be the set {(102),(011),(210)}. It is easy to check that C forms a basis for ℝ3 (determinant
is non-zero). Order C in the obvious manner. What is the change of basis matrix [I]CA? One way is to express each element of C in terms of the elements of A. Another way is to use the formula
[I]CA=[I]BA[I]CB. Applying the first example, we see that [I]CB is just the matrix whose columns are elements of C. As a result:
[I]CA=[I]BA[I]CB=(1/3-2/92/9-2/34/95/91/31/9-1/9)(102011210)=(7/904/94/91-8/91/907/9).
Remarks. Let us summarize what we have learned from the examples above, as well as list some additional facts. Let V be a finite dimensional vector space of dimension n.
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•
If E is the standard basis (ordered), then for any ordered basis A, [I]AE is the matrix whose columns are exactly the basis elements in A (assuming these elements have already been expressed in terms of E) such that the i-column corresponds to the i-th element in the ordered set A.
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•
This also means that every invertible matrix A corresponds to (in a one-to-one fashion) a change of basis from the basis SA whose elements are columns of A to E, the standard basis: A=[I]SAE.
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Continue to assume that E is the standard basis. Let A,B be any ordered bases for V. Using the above property, we can easily compute [I]AB, which is [I]EB[I]AE=([I]BE)-1[I]AE.
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•
Let A′ be a re-ordering of the ordered basis A, where each v′i∈A′ is just vπ(i) for some permutation in Sn. Then [I]A′A is the permutation matrix
corresponding to the permutation π.
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•
Suppose T is a linear transformation from V to W (both finite dimensional). Under a bases A⊂V and B⊂W, T has matrix representation [T]AB. Under changes of basis from A to A′, and B to B′, we have
[T]A′B′=[ITI]A′B′=[I]BB′[T]AB[I]A′A. -
•
If T is a linear operator on V, then setting V=W, A=B and A′=B′ from above, we have that
[T]A′=P-1[T]AP, where P is the change of basis matrix [I]A′A. This shows that [T]A and [T]A′ are similar matrices
. In other words, under a change of basis, the linear transformation T is basically the same.
References
- 1 Friedberg, Insell, Spence. Linear Algebra. Prentice-Hall Inc., 1997.
Title | change of basis |
Canonical name | ChangeOfBasis |
Date of creation | 2013-03-22 17:30:18 |
Last modified on | 2013-03-22 17:30:18 |
Owner | CWoo (3771) |
Last modified by | CWoo (3771) |
Numerical id | 20 |
Author | CWoo (3771) |
Entry type | Definition |
Classification | msc 15A04 |
Synonym | change of coordinates |
Synonym | change of bases |
Synonym | basis change |
Synonym | base change |
Synonym | base change matrix |
Defines | change of basis matrix |