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13.1: Diagonalization

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Suppose we are lucky, and we have L:VV, and the ordered basis B=(v1,,vn) is a set of linearly independent eigenvectors for L, with eigenvalues λ1,,λn. Then:

L(v1)=λ1v1L(v2)=λ2v2L(vn)=λnvn

As a result, the matrix of L in the basis of eigenvectors B is diagonal:

L(x1x2xn)B=((λ1λ2λn)(x1x2xn))B,

where all entries off of the diagonal are zero.

Suppose that V is any n-dimensional vector space. We call a linear transformation L:VV diagonalizable if there exists a collection of n linearly independent eigenvectors for L. In other words, L is diagonalizable if there exists a basis for V of eigenvectors for L.

In a basis of eigenvectors, the matrix of a linear transformation is diagonal. On the other hand, if an n×n matrix is diagonal, then the standard basis vectors ei must already be a set of n linearly independent eigenvectors. We have shown:

Theorem 13.1.1:

Given an ordered basis B for a vector space V and a linear transformation L:VV, then the matrix for L in the basis B is diagonal if and only if B consists of eigenvectors for L.

Typically, however, we do not begin a problem with a basis of eigenvectors, but rather have to compute these. Hence we need to know how to change from one basis to another.

Contributor

This page titled 13.1: Diagonalization is shared under a not declared license and was authored, remixed, and/or curated by David Cherney, Tom Denton, & Andrew Waldron.

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