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Change of basis

In mathematics, an ordered basis of a vector space of finite dimension n allows representing uniquely any element of the vector space by a coordinate vector, which is a sequence of n scalars called coordinates. If two different bases are considered, the coordinate vector that represents a vector v on one basis is, in general, different from the coordinate vector that represents v on the other basis. A change of basis consists of converting every assertion expressed in terms of coordinates relative to one basis into an assertion expressed in terms of coordinates relative to the other basis.[1][2][3]

Not to be confused with Change of base.

Such a conversion results from the change-of-basis formula which expresses the coordinates relative to one basis in terms of coordinates relative to the other basis. Using matrices, this formula can be written


where "old" and "new" refer respectively to the firstly defined basis and the other basis, and are the column vectors of the coordinates of the same vector on the two bases, and is the change-of-basis matrix (also called transition matrix), which is the matrix whose columns are the coordinates of the new basis vectors on the old basis.


This article deals mainly with finite-dimensional vector spaces. However, many of the principles are also valid for infinite-dimensional vector spaces.

a linear function,

a ,

polynomial function

a ,

continuous function

a ,

differentiable function

a ,

smooth function

an ,

analytic function

A function that has a vector space as its domain is commonly specified as a multivariate function whose variables are the coordinates on some basis of the vector on which the function is applied.


When the basis is changed, the expression of the function is changed. This change can be computed by substituting the "old" coordinates for their expressions in terms of the "new" coordinates. More precisely, if f(x) is the expression of the function in terms of the old coordinates, and if x = Ay is the change-of-base formula, then f(Ay) is the expression of the same function in terms of the new coordinates.


The fact that the change-of-basis formula expresses the old coordinates in terms of the new one may seem unnatural, but appears as useful, as no matrix inversion is needed here.


As the change-of-basis formula involves only linear functions, many function properties are kept by a change of basis. This allows defining these properties as properties of functions of a variable vector that are not related to any specific basis. So, a function whose domain is a vector space or a subset of it is


if the multivariate function that represents it on some basis—and thus on every basis—has the same property.


This is specially useful in the theory of manifolds, as this allows extending the concepts of continuous, differentiable, smooth and analytic functions to functions that are defined on a manifold.

Active and passive transformation

Covariance and contravariance of vectors

the continuous analogue of change of basis.

Integral transform

 — application in computational chemistry

Chirgwin-Coulson weights

Anton, Howard (1987), Elementary Linear Algebra (5th ed.), New York: , ISBN 0-471-84819-0

Wiley

Beauregard, Raymond A.; Fraleigh, John B. (1973), , Boston: Houghton Mifflin Company, ISBN 0-395-14017-X

A First Course In Linear Algebra: with Optional Introduction to Groups, Rings, and Fields

Nering, Evar D. (1970), Linear Algebra and Matrix Theory (2nd ed.), New York: , LCCN 76091646

Wiley

from MIT OpenCourseWare

MIT Linear Algebra Lecture on Change of Basis

from Khan Academy

Khan Academy Lecture on Change of Basis