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A First Course in Linear Algebra, 2017a

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358 Spectral Theory<br />

Notice that the above equation can be rearranged as A = PDP −1 . Suppose we wanted to compute<br />

A 100 . By diagonaliz<strong>in</strong>g A first it suffices to then compute ( PDP −1) 100 , which reduces to PD 100 P −1 .This<br />

last computation is much simpler than A 100 . While this process is described <strong>in</strong> detail later, it provides<br />

motivation for diagonalization.<br />

7.2.2 Diagonaliz<strong>in</strong>g a Matrix<br />

The most important theorem about diagonalizability is the follow<strong>in</strong>g major result.<br />

Theorem 7.18: Eigenvectors and Diagonalizable Matrices<br />

An n × n matrix A is diagonalizable if and only if there is an <strong>in</strong>vertible matrix P given by<br />

P = [ X 1 X 2 ··· X n<br />

]<br />

where the X k are eigenvectors of A.<br />

Moreover if A is diagonalizable, the correspond<strong>in</strong>g eigenvalues of A are the diagonal entries of the<br />

diagonal matrix D.<br />

Proof. Suppose P is given as above as an <strong>in</strong>vertible matrix whose columns are eigenvectors of A. Then<br />

P −1 is of the form<br />

⎡ ⎤<br />

W1<br />

T P −1 W T = ⎢ ⎥<br />

⎣<br />

2. ⎦<br />

where Wk T X j = δ kj , which is the Kronecker’s symbol def<strong>in</strong>ed by<br />

{ 1ifi = j<br />

δ ij =<br />

0ifi ≠ j<br />

W T n<br />

Then<br />

P −1 AP =<br />

=<br />

=<br />

⎡<br />

⎢<br />

⎣<br />

⎡<br />

⎢<br />

⎣<br />

⎡<br />

⎢<br />

⎣<br />

W T 1<br />

W T 2<br />

.<br />

W T n<br />

W T 1<br />

W T 2<br />

.<br />

W T n<br />

⎤<br />

[ ]<br />

⎥ AX1 AX 2 ··· AX n<br />

⎦<br />

⎤<br />

[ ]<br />

⎥ λ1 X 1 λ 2 X 2 ··· λ n X n<br />

⎦<br />

⎤<br />

λ 1 0<br />

. ..<br />

⎥<br />

⎦<br />

0 λ n

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