Review : Eigenvalues & Eigenvectors — Question 2

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Question 2

An eigenpair satisfies Av=λvAv=\lambda v with v≠0v\ne 0. The eigenspace Eλ=ker⁡(A−λI)E_\lambda=\ker(A-\lambda I) includes zero, although zero is not an eigenvector. Algebraic multiplicity counts roots of det⁡(λI−A)\det(\lambda I-A); geometric multiplicity is dim⁡Eλ\dim E_\lambda. Work over ℝ\mathbb R unless complex scalars are explicitly requested.

For real aa, consider Ba=(2a02).B_a=\begin{pmatrix}2&a\\0&2\end{pmatrix}. A student claims that a repeated eigenvalue automatically provides two independent eigenvectors.

Tasks

  1. Find the eigenvalue and both multiplicities for every aa, treating a=0a=0 separately.

  2. Classify diagonalizability over ℝ\mathbb R and over ℂ\mathbb C. Explain whether allowing complex eigenvectors repairs any failure.

  3. Find an exact formula for BamB_a^m for every nonnegative integer mm. Derive it rather than assuming diagonalization.

  4. For a fixed vector x=(x1,x2)Tx=(x_1,x_2)^T, classify when 2−mBamx2^{-m}B_a^m x stays bounded as m→∞m\to\infty. Compare this result with what the repeated eigenvalue alone suggests.

Original worksheet page 1: question and worked solution for 5-3-002
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Question 2 – Solution

Strategy. Root multiplicity and the number of independent eigenvectors answer different questions.

Step 1: Solve the eigenspace equation. The characteristic polynomial is (λ−2)2(\lambda-2)^2 for every aa. The equation (Ba−2I)x=0(B_a-2I)x=0 reduces to ax2=0a x_2=0. Thus the algebraic multiplicity is always 22, while a=0:E2=ℝ2,dim⁡E2=2;a≠0:E2=span⁡{(1,0)T},dim⁡E2=1.\boxed{a=0:\ E_2=\mathbb R^2,\ \dim E_2=2; \qquad a\ne 0:\ E_2=\operatorname{span}\{(1,0)^T\},\ \dim E_2=1.} A repeated root does not itself produce a second independent vector.

Step 2: Classify diagonalization in both fields. At a=0a=0, Ba=2IB_a=2I is already diagonal. At a≠0a\ne 0, there is only one independent eigenvector, so no eigenvector basis exists. The same equation ax2=0a x_2=0 holds over ℂ\mathbb C, with the same dimension count there. Hence Ba is diagonalizable exactly when a=0\boxed{B_a\text{ is diagonalizable exactly when }a=0} over either field.

Step 3: Derive the powers from a terminating product. Let N=Ba−2I=(0a00)N=B_a-2I=\begin{pmatrix}0&a\\0&0\end{pmatrix}, so N2=0N^2=0. The commuting binomial expansion gives Bam=2m(1ma/201).\boxed{B_a^m=2^m\begin{pmatrix}1&ma/2\\0&1\end{pmatrix}.} For m=0m=0 this is II. Multiplication by BaB_a adds a/2a/2 to the scaled upper-right entry, confirming the formula inductively without an eigenvector basis.

Step 4: Identify the remaining growth. The scaled iterate is 2−mBamx=(x1+max2/2,x2)T.2^{-m}B_a^m x=(x_1+ma x_2/2,\,x_2)^T. It is bounded exactly when ax2=0\boxed{a x_2=0}, and then is constant. For every a≠0a\ne 0 and x2≠0x_2\ne 0, its first coordinate grows in magnitude linearly. Dividing out the common exponential factor 2m2^m does not remove this extra growth. The missing eigenvector permits behavior that the list of eigenvalues, even with multiplicity, does not describe by itself.

Original worksheet page 2: question and worked solution for 5-3-002

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