Review : Eigenvalues & Eigenvectors — Question 6

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Question 6

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.

Let A=(2112),B=(pqrs).A=\begin{pmatrix}2&1\\1&2\end{pmatrix},\qquad B=\begin{pmatrix}p&q\\r&s\end{pmatrix}. Two matrices commute when AB=BAAB=BA.

Tasks

  1. Find the full family of real matrices BB commuting with AA, by equating entries of the two products.

  2. Find a common eigenvector basis for every matrix in this family. Explain why simultaneous diagonalization always implies commutation.

  3. For B=(1221)B=\begin{pmatrix}1&2\\2&1\end{pmatrix}, find the eigenvalues of ABAB and A+BA+B using the common basis. Explain how two invertible matrices can have a singular sum.

  4. Within the commuting family, classify every invertible BB for which A+BA+B is singular. Identify when the sum has a one-dimensional kernel and when it is the zero matrix.

Original worksheet page 1: question and worked solution for 5-3-006
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Question 6 – Solution

Strategy. Commutation forces preservation of this matrix’s two distinct eigendirections, allowing scalar tests in a common basis.

Step 1: Equate the products. Subtracting the products gives AB−BA=(r−qs−pp−sq−r).AB-BA=\begin{pmatrix}r-q&s-p\\p-s&q-r\end{pmatrix}. Thus r=qr=q and s=ps=p, with no further restrictions. Thus the entire commuting family is B=(pqqp)\boxed{B=\begin{pmatrix}p&q\\q&p\end{pmatrix}}.

Step 2: Use the common directions. For u=(1,1)Tu=(1,1)^T and v=(1,−1)Tv=(1,-1)^T, the eigenvalues of AA are 3,13,1, and those of BB are p+q,p−qp+q,p-q, respectively. These independent vectors form a common eigenvector basis, even if the two eigenvalues of BB coincide. Conversely, if A=PDP−1A=PDP^{-1} and B=PEP−1B=PEP^{-1} with D,ED,E diagonal, then AB=PDEP−1=PEDP−1=BAAB=PDE P^{-1}=PED P^{-1}=BA.

Step 3: Analyze the concrete sum and product. For p=1,q=2p=1,q=2, the eigenvalues of BB on u,vu,v are 3,−13,-1. Therefore the eigenvalues of ABAB are 9,−19,-1 and those of A+BA+B are 6,06,0. Both AA and BB are invertible, but their actions on vv cancel in the sum. The sum has kernel span⁡{v}\operatorname{span}\{v\}.

Step 4: Classify all cancellation cases. Invertibility of BB requires (p+q)(p−q)≠0(p+q)(p-q)\ne 0. Singularity of the sum requires (p+q+3)(p−q+1)=0(p+q+3)(p-q+1)=0. Equivalently the full allowed set is {p+q=−3,p−q≠0}∪{p−q=−1,p+q≠0}.\boxed{\{p+q=-3,\ p-q\ne 0\}\ \cup\ \{p-q=-1,\ p+q\ne 0\}.} On the first line only, the kernel is the line through uu; on the second only, it is the line through vv. Their intersection is (p,q)=(−2,−1)(p,q)=(-2,-1), where B=−AB=-A and A+B=0A+B=0, so the kernel is the entire plane. The excluded points are (−3/2,−3/2)(-3/2,-3/2) and (−1/2,1/2)(-1/2,1/2), where BB itself is singular. The diagram marks these exclusions with open circles.

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Original worksheet page 2: question and worked solution for 5-3-006

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