MATH 133 Linear Algebra and Geometry • McGill University, Montreal

Corrected exercises: eigenvalues and eigenvectors (MATH 133)

This is the corrected exercise set for the eigenvalue chapter of MATH 133, Linear Algebra and Geometry, the first-year course taken at McGill University in science, engineering and management. It follows the first half of section 3.3 of Nicholson, with his convention for the characteristic polynomial, cA(x)=det⁡(xI−A)c_A(x) = \det(xI - A). Every number is chosen to be done by hand: the polynomials factor, the reductions stay in small integers, and the solutions name each row operation and each cofactor expansion, because that is where the marks are.

The thread running through the whole set: every eigen question is a singularity question about the matrix λI−A\lambda I - A. Its DETERMINANT finds the eigenvalues, its NULL SPACE finds the eigenvectors, and the zero vector is never an answer. An eigenvector is a direction that AA keeps on its LINE, possibly reversed, not a vector that keeps pointing the same way. And when the reduction of λI−A\lambda I - A leaves no free variable, it is the λ\lambda that is wrong, never the eigenvector.

The traps named explicitly in the solutions: reading eigenvalues off a row reduced AA, rejecting an eigenvector because its eigenvalue is negative, reporting x=0x = 0 when the reduction gives no free variable, expanding a 3×33 \times 3 along the wrong row and then fighting a cubic, padding the eigenvector of a lower block with zeros, taking opposites instead of reciprocals for A−1A^{-1}, assuming AA and ATA^T share their eigenvectors, and losing the sign of cA(0)=(−1)ndet⁡Ac_A(0) = (-1)^n \det A.

10 corrected exercises • 100 points • 150 minutes

Revision sheet for this chapter → Every MATH 133 chapter →

Course recap

  • • xx is an eigenvector of AA for the eigenvalue λ\lambda when Ax=λxAx = \lambda x AND x≠0x \neq 0. The number λ=0\lambda = 0 is allowed.
  • • Characteristic polynomial (Nicholson): cA(x)=det⁡(xI−A)c_A(x) = \det(xI - A). Its real roots are the eigenvalues. det⁡(A−xI)=(−1)ncA(x)\det(A - xI) = (-1)^n c_A(x), same roots.
  • • Eigenspace: Eλ(A)E_\lambda(A) is the null space of λI−A\lambda I - A; its basic solutions are the basic eigenvectors. The reduction MUST leave a free variable.
  • • If Ax=λxAx = \lambda x: Akx=λkxA^k x = \lambda^k x, (A+cI)x=(λ+c)x(A + cI)x = (\lambda + c)x, (kA)x=kλx(kA)x = k\lambda x, and A−1x=1λxA^{-1}x = \frac{1}{\lambda}x when AA is invertible. ATA^T has the same eigenvalues, not the same eigenvectors.
  • • 00 is an eigenvalue of AA if and only if AA is not invertible.
  • • When cAc_A splits into real factors: tr A=λ1+⋯+λn\text{tr}\,A = \lambda_1 + \dots + \lambda_n and det⁡A=λ1⋯λn\det A = \lambda_1 \cdots \lambda_n, counted with repetition.
  • • Block triangular (BC0D)\begin{pmatrix} B & C \\ 0 & D \end{pmatrix}: cA=cB cDc_A = c_B \, c_D. Reflection: 11 and −1-1. Projection: 11 and 00. Rotation by 90∘90^\circ: no real eigenvalue.

Part A: the basics (/50)

Exercise 1: Is it an eigenvector? One multiplication decides

A non-zero vector xx is an eigenvector of a square matrix AA when Ax=λxAx = \lambda x for some number λ\lambda, called the eigenvalue. The definition asks for nothing more than this: AxAx must land on the line through xx. Testing a vector you are given therefore needs no polynomial at all, only one product and one comparison.

Throughout, A=(1232)A = \begin{pmatrix} 1 & 2 \\ 3 & 2 \end{pmatrix}. The figure shows two vectors and their images: one stays on its own line, the other does not.

uAuvAvsame line: eigenvectorturned: not one
  • a) Compute AuAu for u=(1,−1)u = (1, -1) and AvAv for v=(1,0)v = (1, 0). Decide in each case whether the vector is an eigenvector of AA, and give the eigenvalue when it is.
  • b) Same question for w=(2,3)w = (2, 3) and for (−3,3)(-3, 3).
  • c) A classmate writes: the zero vector is an eigenvector for every λ\lambda, since A0=λ0A0 = \lambda 0. Explain why the definition excludes x=0x = 0, and why the number λ=0\lambda = 0 is NOT excluded.
  • d) Without computing the characteristic polynomial, decide whether 33 is an eigenvalue of AA, then whether 44 is, by testing the matrices 3I−A3I - A and 4I−A4I - A.
  • e) Using the figure, explain why the sentence an eigenvector keeps its direction is wrong, and write the correct sentence.
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Answers

  • a) Au=(−1,1)=−uAu = (-1, 1) = -u: eigenvector, λ=−1\lambda = -1. Av=(1,3)Av = (1, 3): not an eigenvector.
  • b) Aw=(8,12)=4wAw = (8, 12) = 4w: λ=4\lambda = 4. A(−3,3)=(3,−3)A(-3, 3) = (3, -3): eigenvector, λ=−1\lambda = -1.
  • c) x=0x = 0 would make every number an eigenvalue; λ=0\lambda = 0 is allowed and means AA is not invertible.
  • d) det⁡(3I−A)=−4≠0\det(3I - A) = -4 \neq 0: 33 is not an eigenvalue. det⁡(4I−A)=0\det(4I - A) = 0: 44 is.
  • e) An eigenvector stays on its own line through the origin; it may be stretched, shrunk or reversed.

a) Au=(1⋅1+2⋅(−1), 3⋅1+2⋅(−1))=(−1,1)Au = (1 \cdot 1 + 2 \cdot (-1),\ 3 \cdot 1 + 2 \cdot (-1)) = (-1, 1). Compare with uu: (−1,1)=−1⋅(1,−1)(-1, 1) = -1 \cdot (1, -1), so Au=−uAu = -u. The vector uu is an eigenvector and its eigenvalue is λ=−1\lambda = -1. Now Av=(1,3)Av = (1, 3), the first column of AA. For vv to be an eigenvector we would need (1,3)=λ(1,0)=(λ,0)(1, 3) = \lambda (1, 0) = (\lambda, 0), and the second entry 3≠03 \neq 0 makes that impossible: vv is NOT an eigenvector. The method in both cases is the same two steps, compute AxAx, then ask whether it is a multiple of xx by comparing entry by entry. Writing λ\lambda down before checking that the SAME number works in every entry is the classic slip: (4,6)(4, 6) is not a multiple of (1,3)(1, 3) even though 4/14/1 looks like a candidate.

b) Aw=(2+6, 6+6)=(8,12)=4(2,3)Aw = (2 + 6,\ 6 + 6) = (8, 12) = 4(2, 3), so ww is an eigenvector with λ=4\lambda = 4. Then A(−3,3)=(−3+6, −9+6)=(3,−3)=−1⋅(−3,3)A(-3, 3) = (-3 + 6,\ -9 + 6) = (3, -3) = -1 \cdot (-3, 3): an eigenvector again, with λ=−1\lambda = -1. That is no coincidence: (−3,3)=−3u(-3, 3) = -3u, and A(cu)=cAu=c(λu)=λ(cu)A(cu) = cAu = c(\lambda u) = \lambda (cu). Every non-zero multiple of an eigenvector is an eigenvector for the SAME eigenvalue. An eigenvector is really a whole line of them, which is why the next exercises ask for a basis of the eigenspace rather than for one vector.

c) If x=0x = 0 were allowed, then A0=0=λ0A0 = 0 = \lambda 0 would hold for EVERY real λ\lambda, and every number would be an eigenvalue of every matrix. The notion would carry no information, so the definition requires x≠0x \neq 0. The eigenvalue itself has no such restriction: λ=0\lambda = 0 is perfectly legal and says that some non-zero xx satisfies Ax=0Ax = 0, that is the homogeneous system has a non-trivial solution, that is AA is NOT invertible. Two different zeros, two different statements: the zero VECTOR is never an eigenvector, the zero NUMBER is an eigenvalue exactly when AA is singular.

d) λ\lambda is an eigenvalue exactly when (λI−A)x=0(\lambda I - A)x = 0 has a non-zero solution, that is when λI−A\lambda I - A is singular. Here 3I−A=(2−2−31)3I - A = \begin{pmatrix} 2 & -2 \\ -3 & 1 \end{pmatrix}, whose determinant is 2⋅1−(−2)(−3)=2−6=−4≠02 \cdot 1 - (-2)(-3) = 2 - 6 = -4 \neq 0. The matrix is invertible, the only solution is x=0x = 0, and 33 is NOT an eigenvalue. Next 4I−A=(3−2−32)4I - A = \begin{pmatrix} 3 & -2 \\ -3 & 2 \end{pmatrix}, with determinant 6−6=06 - 6 = 0: singular, so 44 IS an eigenvalue, which part b) had already shown with ww. Testing one candidate costs one 2×22 \times 2 determinant, far less than the full polynomial.

e) On the left of the figure, AuAu points exactly OPPOSITE to uu, yet uu is an eigenvector: the eigenvalue −1-1 reverses it. So keeps its direction is false as soon as an eigenvalue is negative, and students who believe it throw away half of the eigenvectors of reflections. On the right, AvAv leaves the dashed line of vv altogether: that is what failing looks like. The correct sentence: x≠0x \neq 0 is an eigenvector of AA when AxAx lies on the LINE through the origin spanned by xx; the eigenvalue says whether it is stretched (λ>1\lambda > 1), shrunk (0<λ<10 < \lambda < 1), reversed (λ<0\lambda < 0) or sent to 00 (λ=0\lambda = 0).

Exercise 2: The 2 by 2: characteristic polynomial, then the null space

Nicholson's convention, used throughout MATH 133: the characteristic polynomial of an n×nn \times n matrix AA is cA(x)=det⁡(xI−A)c_A(x) = \det(xI - A). Its roots are the eigenvalues, and for each eigenvalue λ\lambda the eigenspace Eλ(A)E_\lambda(A) is the null space of λI−A\lambda I - A, whose basic solutions are the basic eigenvectors.

Two different questions, two different tools: a DETERMINANT finds the numbers, a ROW REDUCTION finds the vectors. Here A=(12−26)A = \begin{pmatrix} 1 & 2 \\ -2 & 6 \end{pmatrix}.

  • a) Write xI−AxI - A, compute cA(x)c_A(x) and factor it.
  • b) For each eigenvalue λ\lambda, solve (λI−A)x=0(\lambda I - A)x = 0 naming every row operation, and give a basic eigenvector.
  • c) Check both eigenvectors with one multiplication each.
  • d) A student reduces 4I−A4I - A and obtains the identity matrix. What does that tell her, and what should she do next?
  • e) Another student uses det⁡(A−xI)\det(A - xI). Compare it with cA(x)c_A(x) for this 2×22 \times 2, and say what changes for a 3×33 \times 3 and what does not.
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Answers

  • a) cA(x)=x2−7x+10=(x−2)(x−5)c_A(x) = x^2 - 7x + 10 = (x - 2)(x - 5)
  • b) E2=span{(2,1)}E_2 = \text{span}\{(2, 1)\}, E5=span{(1,2)}E_5 = \text{span}\{(1, 2)\}
  • c) A(2,1)=(4,2)A(2, 1) = (4, 2) and A(1,2)=(5,10)A(1, 2) = (5, 10)
  • d) 44 is not an eigenvalue (cA(4)=−2c_A(4) = -2); recheck the polynomial.
  • e) det⁡(A−xI)=(−1)ncA(x)\det(A - xI) = (-1)^n c_A(x): same for n=2n = 2, opposite sign for n=3n = 3, same roots always.

a) xI−A=(x−1−22x−6)xI - A = \begin{pmatrix} x - 1 & -2 \\ 2 & x - 6 \end{pmatrix}. Every entry of AA changes sign except on the diagonal, where xx is added: the off-diagonal 22 becomes −2-2 and the −2-2 becomes 22. Then cA(x)=(x−1)(x−6)−(−2)(2)=x2−7x+6+4=x2−7x+10=(x−2)(x−5)c_A(x) = (x - 1)(x - 6) - (-2)(2) = x^2 - 7x + 6 + 4 = x^2 - 7x + 10 = (x - 2)(x - 5). The eigenvalues are 22 and 55. The sign of the product of the off-diagonal entries is where marks are lost: (−2)(2)=−4(-2)(2) = -4 is SUBTRACTED, which adds 44. Writing x2−7x+2x^2 - 7x + 2 gives a polynomial with no rational root, and in a course without calculators that alone is a signal that something is wrong.

b) For λ=2\lambda = 2: 2I−A=(1−22−4)2I - A = \begin{pmatrix} 1 & -2 \\ 2 & -4 \end{pmatrix}. R2→R2−2R1R_2 \to R_2 - 2R_1 gives (1−200)\begin{pmatrix} 1 & -2 \\ 0 & 0 \end{pmatrix}. One pivot, one free variable: x2=tx_2 = t, x1=2tx_1 = 2t, so x=t(2,1)x = t(2, 1) and the basic eigenvector is (2,1)(2, 1). For λ=5\lambda = 5: 5I−A=(4−22−1)5I - A = \begin{pmatrix} 4 & -2 \\ 2 & -1 \end{pmatrix}. R1↔R2R_1 \leftrightarrow R_2, then R2→R2−2R1R_2 \to R_2 - 2R_1 gives (2−100)\begin{pmatrix} 2 & -1 \\ 0 & 0 \end{pmatrix}, so 2x1=x22x_1 = x_2; with x1=tx_1 = t, x=t(1,2)x = t(1, 2) and the basic eigenvector is (1,2)(1, 2). The zero row is not a nuisance, it is the GUARANTEE: λI−A\lambda I - A is singular by construction, so its reduction must leave at least one free variable. The eigenspaces are E2=span{(2,1)}E_2 = \text{span}\{(2, 1)\} and E5=span{(1,2)}E_5 = \text{span}\{(1, 2)\}, two lines through the origin, drawn on the figure of the solution.

c) A(2,1)=(1⋅2+2⋅1, −2⋅2+6⋅1)=(4,2)=2(2,1)A(2, 1) = (1 \cdot 2 + 2 \cdot 1,\ -2 \cdot 2 + 6 \cdot 1) = (4, 2) = 2(2, 1), and A(1,2)=(1+4, −2+12)=(5,10)=5(1,2)A(1, 2) = (1 + 4,\ -2 + 12) = (5, 10) = 5(1, 2). Both hold. This check costs ten seconds and catches both kinds of error at once, a wrong eigenvalue and a wrong vector. A correct eigenvalue with a vector from the wrong null space fails it immediately, which is exactly what happens when a student solves (λI−A)x=0(\lambda I - A)x = 0 with the rows of AA instead of those of λI−A\lambda I - A.

d) If 4I−A4I - A reduces to II, then (4I−A)x=0(4I - A)x = 0 has only the solution x=0x = 0, and 44 is NOT an eigenvalue. Indeed 4I−A=(3−22−2)4I - A = \begin{pmatrix} 3 & -2 \\ 2 & -2 \end{pmatrix} has determinant −6+4=−2-6 + 4 = -2, and cA(4)=16−28+10=−2c_A(4) = 16 - 28 + 10 = -2: the same number, as it must be, since cA(4)c_A(4) IS det⁡(4I−A)\det(4I - A). What she must NOT do is declare the eigenspace to be {0}\{0\} or report x=0x = 0 as the eigenvector: that answer is always wrong. The reduction is telling her the λ\lambda is wrong, so she goes back to the polynomial, finds the arithmetic slip, and starts again with 22 and 55.

e) A−xI=−(xI−A)A - xI = -(xI - A), and multiplying an n×nn \times n matrix by −1-1 multiplies its determinant by (−1)n(-1)^n. So det⁡(A−xI)=(−1)ncA(x)\det(A - xI) = (-1)^n c_A(x). For this 2×22 \times 2 the two polynomials are equal. For a 3×33 \times 3 they are opposite: det⁡(A−xI)=−cA(x)\det(A - xI) = -c_A(x), with leading term −x3-x^3. The ROOTS never change, and neither do the eigenspaces, since (λI−A)x=0(\lambda I - A)x = 0 and (A−λI)x=0(A - \lambda I)x = 0 have the same solutions. What does change is any statement read off the coefficients, such as cA(0)c_A(0): keep one convention for the whole computation, and in MATH 133 that convention is det⁡(xI−A)\det(xI - A), monic, leading coefficient 11.

(2, 1)times 2(1, 2)times 5eigenvalue 2eigenvalue 5

Exercise 3: The 3 by 3: expand along the row of zeros

On a 3×33 \times 3 the characteristic polynomial is a cubic, and a cubic handed over expanded is a cubic you have to factor by hunting for roots. The way out is to choose the expansion: a row or a column of xI−AxI - A with two zeros produces the polynomial ALREADY FACTORED.

Here A=(41−2050111)A = \begin{pmatrix} 4 & 1 & -2 \\ 0 & 5 & 0 \\ 1 & 1 & 1 \end{pmatrix}, so that xI−A=(x−4−120x−50−1−1x−1)xI - A = \begin{pmatrix} x-4 & -1 & 2 \\ 0 & x-5 & 0 \\ -1 & -1 & x-1 \end{pmatrix}.

  • a) Compute cA(x)c_A(x) by cofactor expansion along the second row of xI−AxI - A. Say why this row, and give the sign of the cofactor used.
  • b) Give the eigenvalues of AA.
  • c) Find a basis of each eigenspace, naming every row operation.
  • d) Check each basic eigenvector by multiplication, and check the eigenvalues against the trace of AA.
  • e) A student expanded along the first row, obtained x3−10x2+31x−30x^3 - 10x^2 + 31x - 30 and stopped there. Show it is the same polynomial, and explain what his route costs.
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Answers

  • a) cA(x)=(x−5)[(x−4)(x−1)+2]=(x−5)(x−2)(x−3)c_A(x) = (x - 5)\left[(x - 4)(x - 1) + 2\right] = (x - 5)(x - 2)(x - 3)
  • b) λ=2\lambda = 2, 33, 55
  • c) E2=span{(1,0,1)}E_2 = \text{span}\{(1, 0, 1)\}, E3=span{(2,0,1)}E_3 = \text{span}\{(2, 0, 1)\}, E5=span{(1,3,1)}E_5 = \text{span}\{(1, 3, 1)\}
  • d) A(1,0,1)=(2,0,2)A(1, 0, 1) = (2, 0, 2), A(2,0,1)=(6,0,3)A(2, 0, 1) = (6, 0, 3), A(1,3,1)=(5,15,5)A(1, 3, 1) = (5, 15, 5); trace 10=2+3+510 = 2 + 3 + 5.
  • e) Same cubic; it has to be factored by trying divisors of 3030, where row 2 gave (x−5)(x - 5) for free.

a) The second row of xI−AxI - A is (0, x−5, 0)(0,\ x - 5,\ 0): two zeros, so only one cofactor survives. The entry sits in position (2,2)(2, 2) and its sign is (−1)2+2=+1(-1)^{2+2} = +1. Deleting row 2 and column 2 leaves (x−42−1x−1)\begin{pmatrix} x - 4 & 2 \\ -1 & x - 1 \end{pmatrix}, so cA(x)=(x−5)[(x−4)(x−1)−(2)(−1)]=(x−5)(x2−5x+4+2)=(x−5)(x2−5x+6)c_A(x) = (x - 5)\left[(x - 4)(x - 1) - (2)(-1)\right] = (x - 5)(x^2 - 5x + 4 + 2) = (x - 5)(x^2 - 5x + 6). The quadratic factors as (x−2)(x−3)(x - 2)(x - 3), since 2+3=52 + 3 = 5 and 2⋅3=62 \cdot 3 = 6. Final answer: cA(x)=(x−2)(x−3)(x−5)c_A(x) = (x - 2)(x - 3)(x - 5). The factor (x−5)(x - 5) came out without ever being looked for: that is what the choice of row buys, and it is the method the marker expects to see named.

b) The roots of cAc_A: λ=2\lambda = 2, λ=3\lambda = 3 and λ=5\lambda = 5, three distinct real eigenvalues.

c) For λ=2\lambda = 2: 2I−A=(−2−120−30−1−11)2I - A = \begin{pmatrix} -2 & -1 & 2 \\ 0 & -3 & 0 \\ -1 & -1 & 1 \end{pmatrix}. R1↔R3R_1 \leftrightarrow R_3, then R3→R3−2R1R_3 \to R_3 - 2R_1 turns the new third row into (0,1,0)(0, 1, 0); R2→−13R2R_2 \to -\frac{1}{3}R_2 gives (0,1,0)(0, 1, 0), R3→R3−R2R_3 \to R_3 - R_2 gives a zero row, R1→−R1R_1 \to -R_1 then R1→R1−R2R_1 \to R_1 - R_2 gives (1,0,−1)(1, 0, -1). So x2=0x_2 = 0, x1=x3=tx_1 = x_3 = t: E2=span{(1,0,1)}E_2 = \text{span}\{(1, 0, 1)\}. For λ=3\lambda = 3: 3I−A=(−1−120−20−1−12)3I - A = \begin{pmatrix} -1 & -1 & 2 \\ 0 & -2 & 0 \\ -1 & -1 & 2 \end{pmatrix}. R3→R3−R1R_3 \to R_3 - R_1 gives a zero row, R2→−12R2R_2 \to -\frac{1}{2}R_2 gives (0,1,0)(0, 1, 0), R1→−R1R_1 \to -R_1 then R1→R1−R2R_1 \to R_1 - R_2 gives (1,0,−2)(1, 0, -2). So x2=0x_2 = 0, x1=2x3x_1 = 2x_3: E3=span{(2,0,1)}E_3 = \text{span}\{(2, 0, 1)\}. For λ=5\lambda = 5: 5I−A=(1−12000−1−14)5I - A = \begin{pmatrix} 1 & -1 & 2 \\ 0 & 0 & 0 \\ -1 & -1 & 4 \end{pmatrix}. R3→R3+R1R_3 \to R_3 + R_1 gives (0,−2,6)(0, -2, 6), R2↔R3R_2 \leftrightarrow R_3, R2→−12R2R_2 \to -\frac{1}{2}R_2 gives (0,1,−3)(0, 1, -3), R1→R1+R2R_1 \to R_1 + R_2 gives (1,0,−1)(1, 0, -1). So x2=3x3x_2 = 3x_3, x1=x3x_1 = x_3: E5=span{(1,3,1)}E_5 = \text{span}\{(1, 3, 1)\}. Each reduction left exactly one free variable, as it must for a singular λI−A\lambda I - A.

d) A(1,0,1)=(4−2, 0, 1+1)=(2,0,2)A(1, 0, 1) = (4 - 2,\ 0,\ 1 + 1) = (2, 0, 2), twice the vector. A(2,0,1)=(8−2, 0, 2+1)=(6,0,3)A(2, 0, 1) = (8 - 2,\ 0,\ 2 + 1) = (6, 0, 3), three times. A(1,3,1)=(4+3−2, 15, 1+3+1)=(5,15,5)A(1, 3, 1) = (4 + 3 - 2,\ 15,\ 1 + 3 + 1) = (5, 15, 5), five times. The trace of AA is 4+5+1=104 + 5 + 1 = 10 and 2+3+5=102 + 3 + 5 = 10: the sum of the eigenvalues matches, a check that takes three seconds and catches most sign slips in the polynomial.

e) Expanding the factored form: (x−5)(x2−5x+6)=x3−5x2+6x−5x2+25x−30=x3−10x2+31x−30(x - 5)(x^2 - 5x + 6) = x^3 - 5x^2 + 6x - 5x^2 + 25x - 30 = x^3 - 10x^2 + 31x - 30, the same polynomial. His route is correct but expensive twice over: three 2×22 \times 2 minors instead of one, and then a cubic whose roots must be found by testing the divisors of 3030 (c(1)=−8c(1) = -8, c(2)=0c(2) = 0, then a division) before the quadratic appears. On an exam without a calculator this is where time runs out and sign errors multiply. The rule: before expanding xI−AxI - A, scan it for the row or column with the most zeros, and expand along that one.

Exercise 4: Reflection, projection, rotation: eigenvalues read off the geometry

When a matrix has a geometric description, its eigenvectors can be SEEN before anything is computed: they are the lines through the origin that the transformation sends onto themselves.

Three maps of the plane: Q=15(344−3)Q = \frac{1}{5}\begin{pmatrix} 3 & 4 \\ 4 & -3 \end{pmatrix} is the reflection in the line LL of equation y=x2y = \frac{x}{2}, P=15(4221)P = \frac{1}{5}\begin{pmatrix} 4 & 2 \\ 2 & 1 \end{pmatrix} is the projection onto the same line LL, and R=(0−110)R = \begin{pmatrix} 0 & -1 \\ 1 & 0 \end{pmatrix} is the rotation by 90∘90^\circ counterclockwise. The figure shows QQ acting on one vector, and RR acting on two.

LvQvreflection in LaRabRbrotation by 90 degrees
  • a) Without computing any determinant, give two eigenvalues of QQ and an eigenvector for each, from the geometry of a reflection.
  • b) Confirm a) by multiplying QQ by your two vectors.
  • c) Give the eigenvalues and eigenspaces of PP from the geometry, confirm them by multiplication, and explain why PP is not invertible, in terms of its eigenvalues.
  • d) Explain from the figure why no non-zero vector stays on its line under RR, and confirm that cR(x)c_R(x) has no real root.
  • e) Check that the trace is the sum and the determinant the product of the eigenvalues, for QQ and for PP.
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Answers

  • a) λ=1\lambda = 1 with d=(2,1)d = (2, 1) along LL; λ=−1\lambda = -1 with n=(1,−2)n = (1, -2) perpendicular to LL.
  • b) Qd=dQd = d and Qn=(−1,2)=−nQn = (-1, 2) = -n
  • c) E1(P)=span{(2,1)}E_1(P) = \text{span}\{(2, 1)\}, E0(P)=span{(1,−2)}E_0(P) = \text{span}\{(1, -2)\}; 00 is an eigenvalue, so PP is not invertible.
  • d) cR(x)=x2+1≥1c_R(x) = x^2 + 1 \ge 1: no real eigenvalue.
  • e) QQ: trace 0=1−10 = 1 - 1, det −1=1⋅(−1)-1 = 1 \cdot (-1). PP: trace 1=1+01 = 1 + 0, det 0=1⋅00 = 1 \cdot 0.

a) A reflection leaves every point of its mirror where it is: any vector along LL is sent to itself, so it is an eigenvector with eigenvalue 11. The line y=x2y = \frac{x}{2} is spanned by d=(2,1)d = (2, 1). A vector PERPENDICULAR to the mirror is sent to its opposite: eigenvalue −1-1, with eigenvector n=(1,−2)n = (1, -2), since d⋅n=2−2=0d \cdot n = 2 - 2 = 0. Every other vector, like vv on the figure, is sent to its mirror image, which is on another line: not an eigenvector. So the eigenvalues are 11 and −1-1, and a 2×22 \times 2 has at most two, so the list is complete.

b) Qd=15(3⋅2+4⋅1, 4⋅2−3⋅1)=15(10,5)=(2,1)=dQd = \frac{1}{5}(3 \cdot 2 + 4 \cdot 1,\ 4 \cdot 2 - 3 \cdot 1) = \frac{1}{5}(10, 5) = (2, 1) = d. Qn=15(3−8, 4+6)=15(−5,10)=(−1,2)=−nQn = \frac{1}{5}(3 - 8,\ 4 + 6) = \frac{1}{5}(-5, 10) = (-1, 2) = -n. Both confirmed. The figure of the solution draws them: dd untouched, nn reversed on its own line (drawn there at half length). Notice that the reversed vector is a full eigenvector: the eigenvalue −1-1 is exactly the case the sentence keeps its direction would throw away.

c) Projecting onto LL keeps every vector of LL: eigenvalue 11, E1(P)=span{(2,1)}E_1(P) = \text{span}\{(2, 1)\}. It crushes every vector perpendicular to LL to the zero vector: Pn=0=0⋅nPn = 0 = 0 \cdot n, eigenvalue 00, E0(P)=span{(1,−2)}E_0(P) = \text{span}\{(1, -2)\}. Check: P(2,1)=15(8+2, 4+1)=(2,1)P(2, 1) = \frac{1}{5}(8 + 2,\ 4 + 1) = (2, 1) and P(1,−2)=15(4−4, 2−2)=(0,0)P(1, -2) = \frac{1}{5}(4 - 4,\ 2 - 2) = (0, 0). Since 00 is an eigenvalue, Px=0Px = 0 has a non-zero solution, so PP is NOT invertible: geometrically, two different vectors such as vv and v+nv + n have the same shadow, and no matrix can undo that. Note that the eigenvector for λ=0\lambda = 0 is nn, a non-zero vector; the zero vector PnPn is its image, not the eigenvector.

d) A rotation by 90∘90^\circ turns every non-zero vector a quarter turn: aa and RaRa, bb and RbRb are perpendicular on the figure, so RxRx is never on the line of xx, and no real λ\lambda can satisfy Rx=λxRx = \lambda x with x≠0x \neq 0. Algebraically, xI−R=(x1−1x)xI - R = \begin{pmatrix} x & 1 \\ -1 & x \end{pmatrix}, so cR(x)=x⋅x−(1)(−1)=x2+1c_R(x) = x \cdot x - (1)(-1) = x^2 + 1. For every real xx, x2+1≥1>0x^2 + 1 \ge 1 > 0: no real root, no real eigenvalue, no eigenvector in R2\mathbb{R}^2. In MATH 133 this is the complete answer. The polynomial does have roots in the complex numbers, but eigenvalues here are real numbers attached to vectors of Rn\mathbb{R}^n, and computing with complex ones is outside the course.

e) For QQ: trace 3−35=0\frac{3 - 3}{5} = 0 and 1+(−1)=01 + (-1) = 0; determinant 3⋅(−3)−4⋅425=−2525=−1\frac{3 \cdot (-3) - 4 \cdot 4}{25} = \frac{-25}{25} = -1 and 1⋅(−1)=−11 \cdot (-1) = -1. For PP: trace 4+15=1\frac{4 + 1}{5} = 1 and 1+0=11 + 0 = 1; determinant 4⋅1−2⋅225=0\frac{4 \cdot 1 - 2 \cdot 2}{25} = 0 and 1⋅0=01 \cdot 0 = 0. The determinant −1-1 of the reflection is its reversal of orientation, and the determinant 00 of the projection is its collapse onto a line: the two numbers that the geometry announces are exactly the products of the eigenvalues that the geometry showed.

Qd = dnQn = -neigenvalues 1 and -1Pd = dn, and Pn = 0vPveigenvalues 1 and 0

Exercise 5: A block triangular 4 by 4, and the eigenvectors that do not pad

A matrix of the form A=(BC0D)A = \begin{pmatrix} B & C \\ 0 & D \end{pmatrix}, with square blocks BB and DD, is block upper triangular. Its determinant is det⁡B⋅det⁡D\det B \cdot \det D, and xI−AxI - A has the same shape. So the eigenvalues of a 4×44 \times 4 of this kind cost two 2×22 \times 2 polynomials, not a quartic.

Here A=(4−31−1100−100420013)A = \begin{pmatrix} 4 & -3 & 1 & -1 \\ 1 & 0 & 0 & -1 \\ 0 & 0 & 4 & 2 \\ 0 & 0 & 1 & 3 \end{pmatrix}, so that B=(4−310)B = \begin{pmatrix} 4 & -3 \\ 1 & 0 \end{pmatrix}, C=(1−10−1)C = \begin{pmatrix} 1 & -1 \\ 0 & -1 \end{pmatrix} and D=(4213)D = \begin{pmatrix} 4 & 2 \\ 1 & 3 \end{pmatrix}. Write an eigenvector as x=(u,w)x = (u, w), with uu the upper half and ww the lower half.

  • a) Explain why cA(x)=cB(x) cD(x)c_A(x) = c_B(x) \, c_D(x), and give cA(x)c_A(x) fully factored.
  • b) For the eigenvalues coming from BB, give an eigenvector of AA, and prove that padding an eigenvector of BB with two zeros always works.
  • c) For λ=5\lambda = 5, show that ww must be a multiple of (2,1)(2, 1), then find uu by solving a 2×22 \times 2 system. Give a basis of E5(A)E_5(A).
  • d) A classmate claims that (0,0,1,−1)(0, 0, 1, -1) is an eigenvector of AA for λ=2\lambda = 2, since (1,−1)(1, -1) is an eigenvector of DD. Test the claim, then find a basis of E2(A)E_2(A).
  • e) Check your four eigenvalues against the trace and the determinant of AA.
Show the solution

Answers

  • a) cA(x)=(x−1)(x−3)(x−2)(x−5)c_A(x) = (x - 1)(x - 3)(x - 2)(x - 5)
  • b) (1,1,0,0)(1, 1, 0, 0) for λ=1\lambda = 1 and (3,1,0,0)(3, 1, 0, 0) for λ=3\lambda = 3
  • c) E5(A)=span{(1,0,2,1)}E_5(A) = \text{span}\{(1, 0, 2, 1)\}
  • d) A(0,0,1,−1)=(2,1,2,−2)A(0, 0, 1, -1) = (2, 1, 2, -2): false. E2(A)=span{(−1,0,1,−1)}E_2(A) = \text{span}\{(-1, 0, 1, -1)\}.
  • e) trace 11=1+3+2+511 = 1 + 3 + 2 + 5, det 30=1⋅3⋅2⋅530 = 1 \cdot 3 \cdot 2 \cdot 5

a) xI−A=(xI−B−C0xI−D)xI - A = \begin{pmatrix} xI - B & -C \\ 0 & xI - D \end{pmatrix} is block upper triangular, with the zero block below the diagonal, so its determinant is the product of the determinants of the diagonal blocks: cA(x)=det⁡(xI−B)det⁡(xI−D)=cB(x) cD(x)c_A(x) = \det(xI - B)\det(xI - D) = c_B(x)\,c_D(x). The block CC plays no part. Now cB(x)=det⁡(x−43−1x)=x(x−4)+3=x2−4x+3=(x−1)(x−3)c_B(x) = \det\begin{pmatrix} x - 4 & 3 \\ -1 & x \end{pmatrix} = x(x - 4) + 3 = x^2 - 4x + 3 = (x - 1)(x - 3) and cD(x)=det⁡(x−4−2−1x−3)=(x−4)(x−3)−2=x2−7x+10=(x−2)(x−5)c_D(x) = \det\begin{pmatrix} x - 4 & -2 \\ -1 & x - 3 \end{pmatrix} = (x - 4)(x - 3) - 2 = x^2 - 7x + 10 = (x - 2)(x - 5). So cA(x)=(x−1)(x−3)(x−2)(x−5)c_A(x) = (x - 1)(x - 3)(x - 2)(x - 5) and the eigenvalues are 11, 33, 22 and 55.

b) The block product gives A(u,w)=(Bu+Cw, Dw)A(u, w) = (Bu + Cw,\ Dw). With w=0w = 0: A(u,0)=(Bu,0)A(u, 0) = (Bu, 0). So if Bu=λuBu = \lambda u with u≠0u \neq 0, then A(u,0)=(λu,0)=λ(u,0)A(u, 0) = (\lambda u, 0) = \lambda(u, 0), and (u,0)(u, 0) is an eigenvector of AA. For λ=1\lambda = 1: I−B=(−33−11)I - B = \begin{pmatrix} -3 & 3 \\ -1 & 1 \end{pmatrix}, R1→−13R1R_1 \to -\frac{1}{3}R_1 then R2→R2+R1R_2 \to R_2 + R_1 leaves u1=u2u_1 = u_2, so u=(1,1)u = (1, 1) and (1,1,0,0)(1, 1, 0, 0) is an eigenvector. For λ=3\lambda = 3: 3I−B=(−13−13)3I - B = \begin{pmatrix} -1 & 3 \\ -1 & 3 \end{pmatrix}, R2→R2−R1R_2 \to R_2 - R_1 leaves u1=3u2u_1 = 3u_2, so (3,1,0,0)(3, 1, 0, 0). Checks: A(1,1,0,0)=(4−3, 1, 0, 0)=(1,1,0,0)A(1, 1, 0, 0) = (4 - 3,\ 1,\ 0,\ 0) = (1, 1, 0, 0) and A(3,1,0,0)=(12−3, 3, 0, 0)=(9,3,0,0)A(3, 1, 0, 0) = (12 - 3,\ 3,\ 0,\ 0) = (9, 3, 0, 0). Padding works here because the zero block kills everything below.

c) x=(u,w)x = (u, w) is an eigenvector for 55 when Bu+Cw=5uBu + Cw = 5u and Dw=5wDw = 5w. If ww were 00, the first equation would say Bu=5uBu = 5u with u≠0u \neq 0, impossible since 55 is not an eigenvalue of BB. So w≠0w \neq 0 and Dw=5wDw = 5w: ww is an eigenvector of DD. From 5I−D=(1−2−12)5I - D = \begin{pmatrix} 1 & -2 \\ -1 & 2 \end{pmatrix} and R2→R2+R1R_2 \to R_2 + R_1: w1=2w2w_1 = 2w_2, so w=t(2,1)w = t(2, 1). Take w=(2,1)w = (2, 1). Then (5I−B)u=Cw=(2−1, 0−1)=(1,−1)(5I - B)u = Cw = (2 - 1,\ 0 - 1) = (1, -1), with 5I−B=(13−15)5I - B = \begin{pmatrix} 1 & 3 \\ -1 & 5 \end{pmatrix}. R2→R2+R1R_2 \to R_2 + R_1 gives 8u2=08u_2 = 0, so u2=0u_2 = 0 and u1=1u_1 = 1. Hence E5(A)=span{(1,0,2,1)}E_5(A) = \text{span}\{(1, 0, 2, 1)\}. Check: A(1,0,2,1)=(4+2−1, 1−1, 8+2, 2+3)=(5,0,10,5)A(1, 0, 2, 1) = (4 + 2 - 1,\ 1 - 1,\ 8 + 2,\ 2 + 3) = (5, 0, 10, 5), five times the vector.

d) A(0,0,1,−1)=(1+1, 0+1, 4−2, 1−3)=(2,1,2,−2)A(0, 0, 1, -1) = (1 + 1,\ 0 + 1,\ 4 - 2,\ 1 - 3) = (2, 1, 2, -2), while 2(0,0,1,−1)=(0,0,2,−2)2(0, 0, 1, -1) = (0, 0, 2, -2). The lower half is right, the upper half is not: the block CC sends ww back into the top rows. Padding with zeros works for the UPPER-LEFT block only. The correct computation: w=(1,−1)w = (1, -1) spans E2(D)E_2(D), since 2I−D=(−2−2−1−1)2I - D = \begin{pmatrix} -2 & -2 \\ -1 & -1 \end{pmatrix} gives w1=−w2w_1 = -w_2. Then Cw=(1+1, 0+1)=(2,1)Cw = (1 + 1,\ 0 + 1) = (2, 1) and (2I−B)u=(2,1)(2I - B)u = (2, 1) with 2I−B=(−23−12)2I - B = \begin{pmatrix} -2 & 3 \\ -1 & 2 \end{pmatrix}: R1↔R2R_1 \leftrightarrow R_2, R2→R2−2R1R_2 \to R_2 - 2R_1 gives −u2=0-u_2 = 0, so u2=0u_2 = 0 and −u1=1-u_1 = 1, u=(−1,0)u = (-1, 0). So E2(A)=span{(−1,0,1,−1)}E_2(A) = \text{span}\{(-1, 0, 1, -1)\}, and A(−1,0,1,−1)=(−4+1+1, −1+1, 4−2, 1−3)=(−2,0,2,−2)A(-1, 0, 1, -1) = (-4 + 1 + 1,\ -1 + 1,\ 4 - 2,\ 1 - 3) = (-2, 0, 2, -2) confirms it.

e) trace A=4+0+4+3=11A = 4 + 0 + 4 + 3 = 11 and 1+3+2+5=111 + 3 + 2 + 5 = 11. det⁡A=det⁡B⋅det⁡D=(0+3)(12−2)=3⋅10=30\det A = \det B \cdot \det D = (0 + 3)(12 - 2) = 3 \cdot 10 = 30 and 1⋅3⋅2⋅5=301 \cdot 3 \cdot 2 \cdot 5 = 30. Both agree. A 4×44 \times 4 determinant by cofactors is a long computation; here the block structure hands it over in one line, and the check confirms the four eigenvalues without a single new product.

Part B: problems and reasoning (/50)

Exercise 6: Eigenvalues of related matrices, each with its one-line proof

Once the eigenvalues of AA are known, those of AkA^k, A−1A^{-1}, A+cIA + cI, kAkA and ATA^T follow without a new determinant. On an exam each of these is worth a mark for the answer and a mark for the one line that justifies it, and the justification is always the same move: start from Ax=λxAx = \lambda x and apply the operation to both sides.

Here A=(5−63−4)A = \begin{pmatrix} 5 & -6 \\ 3 & -4 \end{pmatrix}. You may use that cA(x)=(x−2)(x+1)c_A(x) = (x - 2)(x + 1), with E2(A)=span{(2,1)}E_2(A) = \text{span}\{(2, 1)\} and E−1(A)=span{(1,1)}E_{-1}(A) = \text{span}\{(1, 1)\}.

  • a) Check the two eigenvectors, then prove that Ax=λxAx = \lambda x implies Akx=λkxA^k x = \lambda^k x for every k≥1k \ge 1. Give the eigenvalues of A3A^3 with an eigenvector for each.
  • b) Explain why AA is invertible without computing det⁡A\det A. Prove that the eigenvalues of A−1A^{-1} are the reciprocals 1λ\frac{1}{\lambda}, with the same eigenvectors, and confirm with A−1A^{-1} computed.
  • c) Give the eigenvalues of A+4IA + 4I and of 3A3A, with a one-line proof for each.
  • d) Prove that ATA^T has the same characteristic polynomial as AA. Then find E2(AT)E_2(A^T) and compare it with E2(A)E_2(A).
  • e) Prove that if a square matrix BB satisfies B2=BB^2 = B, each of its eigenvalues is 00 or 11, and that if B2=IB^2 = I, each is 11 or −1-1. Which matrices of Exercise 4 illustrate each case?
Show the solution

Answers

  • a) A3A^3 has eigenvalues 88 (eigenvector (2,1)(2, 1)) and −1-1 (eigenvector (1,1)(1, 1)).
  • b) 00 is not an eigenvalue. A−1A^{-1} has eigenvalues 12\frac{1}{2} and −1-1, same eigenvectors.
  • c) A+4IA + 4I: 66 and 33. 3A3A: 66 and −3-3. Same eigenvectors.
  • d) cAT=cAc_{A^T} = c_A; E2(AT)=span{(1,−1)}≠E2(A)E_2(A^T) = \text{span}\{(1, -1)\} \neq E_2(A).
  • e) B2=BB^2 = B gives λ2=λ\lambda^2 = \lambda, so 00 or 11 (projection PP); B2=IB^2 = I gives λ2=1\lambda^2 = 1, so ±1\pm 1 (reflection QQ).

a) A(2,1)=(10−6, 6−4)=(4,2)=2(2,1)A(2, 1) = (10 - 6,\ 6 - 4) = (4, 2) = 2(2, 1) and A(1,1)=(5−6, 3−4)=(−1,−1)=−1⋅(1,1)A(1, 1) = (5 - 6,\ 3 - 4) = (-1, -1) = -1 \cdot (1, 1). Now suppose Ax=λxAx = \lambda x. Then A2x=A(Ax)=A(λx)=λAx=λ2xA^2 x = A(Ax) = A(\lambda x) = \lambda Ax = \lambda^2 x, and by induction, if Akx=λkxA^k x = \lambda^k x then Ak+1x=A(λkx)=λkAx=λk+1xA^{k+1}x = A(\lambda^k x) = \lambda^k Ax = \lambda^{k+1} x. The same xx works, with the eigenvalue raised to the power. So A3A^3 has eigenvalues 23=82^3 = 8, with eigenvector (2,1)(2, 1), and (−1)3=−1(-1)^3 = -1, with eigenvector (1,1)(1, 1). As A3A^3 is 2×22 \times 2 it has at most two eigenvalues, so the list is complete. Computing A3A^3 entry by entry to find this would be nine times the work and is never what the question wants.

b) AA is invertible exactly when 00 is not an eigenvalue, and its eigenvalues are 22 and −1-1. (Indeed det⁡A=2⋅(−1)=−2\det A = 2 \cdot (-1) = -2, the product of the eigenvalues.) If Ax=λxAx = \lambda x with λ≠0\lambda \neq 0, multiply on the left by A−1A^{-1}: x=λA−1xx = \lambda A^{-1}x, then divide by λ\lambda: A−1x=1λxA^{-1}x = \frac{1}{\lambda}x. So A−1A^{-1} has eigenvalues 12\frac{1}{2} and 1−1=−1\frac{1}{-1} = -1, with the SAME eigenvectors. The division by λ\lambda is exactly where invertibility is used. Confirmation: A−1=1−2(−46−35)=12(4−63−5)A^{-1} = \frac{1}{-2}\begin{pmatrix} -4 & 6 \\ -3 & 5 \end{pmatrix} = \frac{1}{2}\begin{pmatrix} 4 & -6 \\ 3 & -5 \end{pmatrix}, and A−1(2,1)=12(8−6, 6−5)=(1,12)=12(2,1)A^{-1}(2, 1) = \frac{1}{2}(8 - 6,\ 6 - 5) = (1, \frac{1}{2}) = \frac{1}{2}(2, 1), A−1(1,1)=12(−2,−2)=−(1,1)A^{-1}(1, 1) = \frac{1}{2}(-2, -2) = -(1, 1). The trap is to answer −2-2 and 11: the inverse takes RECIPROCALS, never opposites.

c) (A+4I)x=Ax+4x=λx+4x=(λ+4)x(A + 4I)x = Ax + 4x = \lambda x + 4x = (\lambda + 4)x: the eigenvalues shift by 44, to 66 and 33, and the eigenvectors do not move. (3A)x=3(Ax)=3λx(3A)x = 3(Ax) = 3\lambda x: the eigenvalues are multiplied by 33, to 66 and −3-3, same eigenvectors again. Notice that A+4IA + 4I and 3A3A both have 66 as an eigenvalue, but for DIFFERENT eigenvectors, (2,1)(2, 1) and (1,1)(1, 1) respectively: an eigenvalue alone never identifies a matrix, it always comes attached to its vector.

d) xI−AT=(xI−A)TxI - A^T = (xI - A)^T, because IT=II^T = I, and a matrix and its transpose have the same determinant. So cAT(x)=cA(x)=(x−2)(x+1)c_{A^T}(x) = c_A(x) = (x - 2)(x + 1): same eigenvalues 22 and −1-1. The eigenvectors, however, are computed from a different matrix. AT=(53−6−4)A^T = \begin{pmatrix} 5 & 3 \\ -6 & -4 \end{pmatrix} and 2I−AT=(−3−366)2I - A^T = \begin{pmatrix} -3 & -3 \\ 6 & 6 \end{pmatrix}; R2→R2+2R1R_2 \to R_2 + 2R_1 gives a zero row and x1+x2=0x_1 + x_2 = 0, so E2(AT)=span{(1,−1)}E_2(A^T) = \text{span}\{(1, -1)\}. Check: AT(1,−1)=(5−3, −6+4)=(2,−2)A^T(1, -1) = (5 - 3,\ -6 + 4) = (2, -2). This is not the line of (2,1)(2, 1): indeed AT(2,1)=(13,−16)A^T(2, 1) = (13, -16), not a multiple of (2,1)(2, 1). Transposing keeps the eigenvalues and moves the eigenvectors.

e) Let Bx=λxBx = \lambda x with x≠0x \neq 0. Then B2x=λ2xB^2 x = \lambda^2 x by part a). If B2=BB^2 = B, then λ2x=Bx=λx\lambda^2 x = Bx = \lambda x, so (λ2−λ)x=0(\lambda^2 - \lambda)x = 0, and since x≠0x \neq 0 the NUMBER λ2−λ\lambda^2 - \lambda must be 00: λ=0\lambda = 0 or λ=1\lambda = 1. If B2=IB^2 = I, then λ2x=x\lambda^2 x = x, so λ2=1\lambda^2 = 1 and λ=±1\lambda = \pm 1. The step since x≠0x \neq 0 is the reason the definition excludes the zero vector: without it nothing could be concluded. The projection PP of Exercise 4 satisfies P2=PP^2 = P (projecting twice is projecting once) and has eigenvalues 11 and 00; the reflection QQ satisfies Q2=IQ^2 = I (reflecting twice gives back the vector) and has eigenvalues 11 and −1-1. The algebra says which eigenvalues are POSSIBLE; it does not say that both occur, and B=IB = I satisfies both equations with the single eigenvalue 11.

Exercise 7: Zero, the trace and the determinant: finding the missing eigenvalue

Two facts save whole determinants. First, 00 is an eigenvalue of AA exactly when AA is not invertible, and then any non-zero solution of Ax=0Ax = 0 is an eigenvector for it. Second, when cAc_A splits into real linear factors, the trace of AA is the sum of the eigenvalues and det⁡A\det A is their product, each counted as often as it appears in cAc_A.

Together they recover an eigenvalue that is missing, as soon as the others are known. Here N=(3−12−121134)N = \begin{pmatrix} 3 & -1 & 2 \\ -1 & 2 & 1 \\ 1 & 3 & 4 \end{pmatrix} and A=(111−1410−12)A = \begin{pmatrix} 1 & 1 & 1 \\ -1 & 4 & 1 \\ 0 & -1 & 2 \end{pmatrix}.

  • a) Observe the columns of NN. Deduce, without any determinant, that NN is not invertible, that 00 is an eigenvalue, and give an eigenvector for it.
  • b) Show that (1,0,1)(1, 0, 1) is an eigenvector of NN and give its eigenvalue. Then find the third eigenvalue of NN from the trace alone.
  • c) Find a basis of the eigenspace of that third eigenvalue, and check it.
  • d) Starting from cM(x)=(x−λ1)(x−λ2)(x−λ3)c_M(x) = (x - \lambda_1)(x - \lambda_2)(x - \lambda_3) for a 3×33 \times 3 matrix MM, prove that det⁡M=λ1λ2λ3\det M = \lambda_1\lambda_2\lambda_3 and tr M=λ1+λ2+λ3\text{tr}\,M = \lambda_1 + \lambda_2 + \lambda_3. Watch the sign of cM(0)c_M(0).
  • e) For AA, the vectors (1,0,1)(1, 0, 1) and (0,−1,1)(0, -1, 1) are eigenvectors. Find their eigenvalues, deduce the third eigenvalue from the trace, and confirm it with the determinant.
Show the solution

Answers

  • a) Column 3 == column 1 ++ column 2, so N(1,1,−1)=0N(1, 1, -1) = 0: λ=0\lambda = 0 with eigenvector (1,1,−1)(1, 1, -1).
  • b) N(1,0,1)=(5,0,5)N(1, 0, 1) = (5, 0, 5): λ=5\lambda = 5. Third eigenvalue 9−0−5=49 - 0 - 5 = 4.
  • c) E4(N)=span{(3,−1,1)}E_4(N) = \text{span}\{(3, -1, 1)\}
  • d) cM(0)=−det⁡M=−λ1λ2λ3c_M(0) = -\det M = -\lambda_1\lambda_2\lambda_3; the x2x^2 coefficient is −tr M=−(λ1+λ2+λ3)-\text{tr}\,M = -(\lambda_1 + \lambda_2 + \lambda_3).
  • e) λ=2\lambda = 2 and λ=3\lambda = 3; the third is 7−5=27 - 5 = 2 again; det⁡A=12=2⋅3⋅2\det A = 12 = 2 \cdot 3 \cdot 2.

a) The third column of NN is the sum of the first two: 2=3+(−1)2 = 3 + (-1), 1=−1+21 = -1 + 2, 4=1+34 = 1 + 3. So 1⋅c1+1⋅c2−1⋅c3=01 \cdot c_1 + 1 \cdot c_2 - 1 \cdot c_3 = 0, which says exactly that N(1,1,−1)=0N(1, 1, -1) = 0. Row by row: 3−1−2=03 - 1 - 2 = 0, −1+2−1=0-1 + 2 - 1 = 0, 1+3−4=01 + 3 - 4 = 0. The columns are dependent, so NN is not invertible; and (1,1,−1)(1, 1, -1) is a NON-ZERO vector with N(1,1,−1)=0=0⋅(1,1,−1)N(1, 1, -1) = 0 = 0 \cdot (1, 1, -1), so 00 is an eigenvalue and (1,1,−1)(1, 1, -1) an eigenvector for it. No determinant was needed: a visible column dependency IS an eigenvector for 00.

b) N(1,0,1)=(3+2, −1+1, 1+4)=(5,0,5)=5(1,0,1)N(1, 0, 1) = (3 + 2,\ -1 + 1,\ 1 + 4) = (5, 0, 5) = 5(1, 0, 1): eigenvalue 55. The trace of NN is 3+2+4=93 + 2 + 4 = 9, and it is the sum of the three eigenvalues, so the third one is 9−0−5=49 - 0 - 5 = 4. The determinant cannot find it here, since det⁡N=0⋅5⋅λ3=0\det N = 0 \cdot 5 \cdot \lambda_3 = 0 whatever λ3\lambda_3 is: when 00 is an eigenvalue, the product is blind and only the trace speaks. Choosing the right identity is half the question.

c) 4I−N=(11−212−1−1−30)4I - N = \begin{pmatrix} 1 & 1 & -2 \\ 1 & 2 & -1 \\ -1 & -3 & 0 \end{pmatrix}. R2→R2−R1R_2 \to R_2 - R_1 gives (0,1,1)(0, 1, 1), R3→R3+R1R_3 \to R_3 + R_1 gives (0,−2,−2)(0, -2, -2), then R3→R3+2R2R_3 \to R_3 + 2R_2 gives a zero row, which is the confirmation that 44 really is an eigenvalue. R1→R1−R2R_1 \to R_1 - R_2 gives (1,0,−3)(1, 0, -3). So x1=3x3x_1 = 3x_3, x2=−x3x_2 = -x_3, and E4(N)=span{(3,−1,1)}E_4(N) = \text{span}\{(3, -1, 1)\}. Check: N(3,−1,1)=(9+1+2, −3−2+1, 3−3+4)=(12,−4,4)=4(3,−1,1)N(3, -1, 1) = (9 + 1 + 2,\ -3 - 2 + 1,\ 3 - 3 + 4) = (12, -4, 4) = 4(3, -1, 1). Had the trace been misread, the reduction would have produced three pivots and warned you.

d) Set x=0x = 0 in both expressions of cMc_M. On one side cM(0)=det⁡(0I−M)=det⁡(−M)=(−1)3det⁡M=−det⁡Mc_M(0) = \det(0I - M) = \det(-M) = (-1)^3 \det M = -\det M. On the other, (0−λ1)(0−λ2)(0−λ3)=−λ1λ2λ3(0 - \lambda_1)(0 - \lambda_2)(0 - \lambda_3) = -\lambda_1\lambda_2\lambda_3. Hence det⁡M=λ1λ2λ3\det M = \lambda_1\lambda_2\lambda_3. The two minus signs cancel only because BOTH sides are handled with Nicholson's det⁡(xI−M)\det(xI - M); mixing conventions gives det⁡M=−λ1λ2λ3\det M = -\lambda_1\lambda_2\lambda_3, a classic lost mark. For the trace, expand det⁡(xI−M)\det(xI - M): every term other than the product of the diagonal entries (x−m11)(x−m22)(x−m33)(x - m_{11})(x - m_{22})(x - m_{33}) misses at least two diagonal positions, so has degree at most 11. The x2x^2 coefficient therefore comes from the diagonal alone and equals −(m11+m22+m33)-(m_{11} + m_{22} + m_{33}). In the factored form it is −(λ1+λ2+λ3)-(\lambda_1 + \lambda_2 + \lambda_3). Comparing: tr M=λ1+λ2+λ3\text{tr}\,M = \lambda_1 + \lambda_2 + \lambda_3.

e) A(1,0,1)=(1+1, −1+1, 0+2)=(2,0,2)A(1, 0, 1) = (1 + 1,\ -1 + 1,\ 0 + 2) = (2, 0, 2): eigenvalue 22. A(0,−1,1)=(−1+1, −4+1, 1+2)=(0,−3,3)A(0, -1, 1) = (-1 + 1,\ -4 + 1,\ 1 + 2) = (0, -3, 3): eigenvalue 33. The trace is 1+4+2=71 + 4 + 2 = 7, so the third eigenvalue is 7−2−3=27 - 2 - 3 = 2: the eigenvalue 22 appears TWICE, and cA(x)=(x−2)2(x−3)c_A(x) = (x - 2)^2(x - 3). The trap is to reject this answer because 22 is already on the list: nothing forces the three eigenvalues to be distinct, and the trace counts each one as often as it is a root. The determinant confirms it: by cofactors along the first row, det⁡A=1(8+1)−1(−2−0)+1(1−0)=9+2+1=12\det A = 1(8 + 1) - 1(-2 - 0) + 1(1 - 0) = 9 + 2 + 1 = 12, and 2⋅3⋅2=122 \cdot 3 \cdot 2 = 12.

Exercise 8: Five statements to correct

Each statement below was written by a student in a MATH 133 tutorial, and each is false. Say what is wrong, give the correct statement, and settle it with the smallest counterexample you can find.

  • a) An eigenvector keeps its direction, so (1,−1)(1, -1) is not an eigenvector of (1232)\begin{pmatrix} 1 & 2 \\ 3 & 2 \end{pmatrix}, since its image (−1,1)(-1, 1) points the other way.
  • b) To find the eigenvalues, row reduce AA to an echelon form and read the diagonal.
  • c) AA and ATA^T have the same eigenvectors, since they have the same characteristic polynomial.
  • d) The eigenvalues of A+BA + B are the sums of an eigenvalue of AA and an eigenvalue of BB.
  • e) A matrix whose only eigenvalue is 00 is the zero matrix.
Show the solution

Answers

  • a) False: it is an eigenvector with λ=−1\lambda = -1; an eigenvector stays on its LINE.
  • b) False: row operations change the eigenvalues (44 and −1-1 become a diagonal 11, −4-4).
  • c) False: same eigenvalues, different eigenvectors (E2E_2 is (2,1)(2, 1) for AA, (1,−1)(1, -1) for ATA^T in Exercise 6).
  • d) False: (0100)\begin{pmatrix} 0 & 1 \\ 0 & 0 \end{pmatrix} and (0010)\begin{pmatrix} 0 & 0 \\ 1 & 0 \end{pmatrix} have only 00, their sum has 11 and −1-1.
  • e) False: (0100)\begin{pmatrix} 0 & 1 \\ 0 & 0 \end{pmatrix} has c(x)=x2c(x) = x^2 and is not zero.

a) FALSE. A(1,−1)=(1−2, 3−2)=(−1,1)=−1⋅(1,−1)A(1, -1) = (1 - 2,\ 3 - 2) = (-1, 1) = -1 \cdot (1, -1), so (1,−1)(1, -1) is an eigenvector with eigenvalue −1-1. The definition Ax=λxAx = \lambda x puts no sign on λ\lambda: a negative eigenvalue reverses the vector and keeps it on the same line through the origin. Correct statement: a non-zero xx is an eigenvector when AxAx lies on the line spanned by xx, whether stretched, shrunk, reversed or sent to 00. This error deletes every eigenvector of every reflection for the value −1-1.

b) FALSE. Row operations preserve the null space of AA, not its eigenvalues. For A=(1232)A = \begin{pmatrix} 1 & 2 \\ 3 & 2 \end{pmatrix}, whose eigenvalues are 44 and −1-1 by Exercise 1, the single operation R2→R2−3R1R_2 \to R_2 - 3R_1 gives (120−4)\begin{pmatrix} 1 & 2 \\ 0 & -4 \end{pmatrix}, whose diagonal reads 11 and −4-4: both wrong. The eigenvalues depend on AA as a whole, and xI−AxI - A must be formed BEFORE anything is reduced. Correct statement: the eigenvalues can be read off the diagonal only when AA itself is triangular; row reduction is used afterwards, on λI−A\lambda I - A, to find the eigenvectors.

c) FALSE. The characteristic polynomials are equal, so the EIGENVALUES agree, but the eigenvectors come from the null spaces of λI−A\lambda I - A and λI−AT\lambda I - A^T, which are different matrices. In Exercise 6, A=(5−63−4)A = \begin{pmatrix} 5 & -6 \\ 3 & -4 \end{pmatrix} has E2(A)=span{(2,1)}E_2(A) = \text{span}\{(2, 1)\} while E2(AT)=span{(1,−1)}E_2(A^T) = \text{span}\{(1, -1)\}, and AT(2,1)=(13,−16)A^T(2, 1) = (13, -16) is not a multiple of (2,1)(2, 1). Correct statement: AA and ATA^T have the same eigenvalues; their eigenvectors must be computed separately.

d) FALSE. Take A=(0100)A = \begin{pmatrix} 0 & 1 \\ 0 & 0 \end{pmatrix} and B=(0010)B = \begin{pmatrix} 0 & 0 \\ 1 & 0 \end{pmatrix}. Each is triangular with zeros on the diagonal, so each has the single eigenvalue 00, and every sum of an eigenvalue of AA and one of BB is 00. But A+B=(0110)A + B = \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix} has c(x)=x2−1c(x) = x^2 - 1, with eigenvalues 11 and −1-1, eigenvectors (1,1)(1, 1) and (1,−1)(1, -1). The reasoning (A+B)x=λx+μx(A + B)x = \lambda x + \mu x would need the SAME xx to be an eigenvector of both. Correct statement: the rule holds for A+cIA + cI, since every vector is an eigenvector of cIcI, and the eigenvalues then shift by cc.

e) FALSE. A=(0100)A = \begin{pmatrix} 0 & 1 \\ 0 & 0 \end{pmatrix} has cA(x)=det⁡(x−10x)=x2c_A(x) = \det\begin{pmatrix} x & -1 \\ 0 & x \end{pmatrix} = x^2, so its only eigenvalue is 00, and yet A≠0A \neq 0: it sends (0,1)(0, 1) to (1,0)(1, 0). What the eigenvalues do force is the trace and the determinant, both 00 here, and the fact that AA is not invertible. Correct statement: a matrix whose only eigenvalue is 00 is singular, with trace 00; it need not be the zero matrix, and the eigenvalues alone never determine a matrix.

Exercise 9: A stretched rubber sample: which printed fibres keep their line

A materials lab stretches a square sample of rubber sheet on which straight fibres have been printed through one corner, taken as the origin. The deformation is homogeneous: a point at position pp moves to FpFp, with F=(4−211)F = \begin{pmatrix} 4 & -2 \\ 1 & 1 \end{pmatrix}, lengths in units of the printed grid. A fibre printed along a direction vv ends up along FvFv, and the engineers want to know which fibres come out on their ORIGINAL line, and how much each is stretched.

The figure shows the unit square of the grid and its image.

sample(1, 0)(0, 1)F(4, 1)(-2, 1)(2, 2)(0, 0)
  • a) Find the eigenvalues of FF and the directions of the fibres that stay on their line, with the stretch factor of each.
  • b) Where does the fibre printed along the bottom edge, direction (1,0)(1, 0), go? Is any fibre of the sample reversed?
  • c) By what factor is the area of the sample multiplied? A sample of 33 by 33 grid units covers what area after stretching? Relate the factor to the eigenvalues.
  • d) When the sample is released it returns to its original shape through F−1F^{-1}. Which fibres keep their line on the way back, with what factors? And if the lab adds a uniform stretch of 1.51.5 in every direction, applying 1.5F1.5F instead of FF?
  • e) A second sample is skewed by S=(11201)S = \begin{pmatrix} 1 & \frac{1}{2} \\ 0 & 1 \end{pmatrix}. Find cSc_S, the eigenvalue and its eigenspace. Which fibres keep their line, and are any of them stretched?
Show the solution

Answers

  • a) cF(x)=(x−2)(x−3)c_F(x) = (x - 2)(x - 3): fibres along (1,1)(1, 1) stretched by 22, along (2,1)(2, 1) stretched by 33.
  • b) (1,0)↦(4,1)(1, 0) \mapsto (4, 1): turned. No fibre is reversed, both eigenvalues are positive.
  • c) Factor det⁡F=6=2⋅3\det F = 6 = 2 \cdot 3; the 33 by 33 sample covers 5454 square units.
  • d) F−1F^{-1}: same fibres, factors 12\frac{1}{2} and 13\frac{1}{3}. 1.5F1.5F: same fibres, factors 33 and 4.54.5.
  • e) cS(x)=(x−1)2c_S(x) = (x - 1)^2; E1(S)=span{(1,0)}E_1(S) = \text{span}\{(1, 0)\}: only horizontal fibres keep their line, unstretched.

a) A fibre along vv stays on its line exactly when Fv=λvFv = \lambda v: the fibres that keep their line ARE the eigenvectors, and the stretch factors are the eigenvalues. xI−F=(x−42−1x−1)xI - F = \begin{pmatrix} x - 4 & 2 \\ -1 & x - 1 \end{pmatrix}, so cF(x)=(x−4)(x−1)+2=x2−5x+6=(x−2)(x−3)c_F(x) = (x - 4)(x - 1) + 2 = x^2 - 5x + 6 = (x - 2)(x - 3). For λ=2\lambda = 2: 2I−F=(−22−11)2I - F = \begin{pmatrix} -2 & 2 \\ -1 & 1 \end{pmatrix}, R1→−12R1R_1 \to -\frac{1}{2}R_1 then R2→R2+R1R_2 \to R_2 + R_1 leaves x1=x2x_1 = x_2, so the direction (1,1)(1, 1): the diagonal fibre doubles in length. For λ=3\lambda = 3: 3I−F=(−12−12)3I - F = \begin{pmatrix} -1 & 2 \\ -1 & 2 \end{pmatrix}, R2→R2−R1R_2 \to R_2 - R_1 leaves x1=2x2x_1 = 2x_2, so the direction (2,1)(2, 1), tripled. Check: F(1,1)=(2,2)F(1, 1) = (2, 2) and F(2,1)=(6,3)F(2, 1) = (6, 3). The figure of the solution draws both: the fibres that end at (1,1)(1, 1) and at (1,12)(1, \frac{1}{2}) in the square end at (2,2)(2, 2) and (3,32)(3, \frac{3}{2}), on the same lines.

b) F(1,0)=(4,1)F(1, 0) = (4, 1), the first column of FF. It is not a multiple of (1,0)(1, 0), since its second entry is 1≠01 \neq 0: that fibre is turned upward, as the figure of the solution shows. A reversed fibre would need a NEGATIVE eigenvalue; both eigenvalues are positive, so no fibre of the sample comes out pointing backwards. Almost every fibre turns: only the two eigen-directions escape, which is why they are the ones an engineer measures.

c) A linear map multiplies every area by ∣det⁡F∣|\det F|, and det⁡F=4⋅1−(−2)⋅1=6\det F = 4 \cdot 1 - (-2) \cdot 1 = 6. So the 33 by 33 sample, of area 99 square units, covers 9×6=549 \times 6 = 54 square units after stretching. The factor is the product of the eigenvalues, 2×3=62 \times 3 = 6, and the picture explains why: a small parallelogram built on the two eigen-directions has one side doubled and the other tripled, so its area is multiplied by 66, and the whole sample is tiled by such parallelograms.

d) FF is invertible since 00 is not an eigenvalue. If Fv=λvFv = \lambda v then F−1v=1λvF^{-1}v = \frac{1}{\lambda}v: on release the same two fibres stay on their lines, the diagonal one shrinking by a factor 12\frac{1}{2} and the other by 13\frac{1}{3}. Check: F−1=16(12−14)F^{-1} = \frac{1}{6}\begin{pmatrix} 1 & 2 \\ -1 & 4 \end{pmatrix} and F−1(1,1)=16(3,3)=12(1,1)F^{-1}(1, 1) = \frac{1}{6}(3, 3) = \frac{1}{2}(1, 1). With the extra uniform stretch, (1.5F)v=1.5λv(1.5F)v = 1.5\lambda v: same fibres again, with factors 1.5×2=31.5 \times 2 = 3 and 1.5×3=4.51.5 \times 3 = 4.5. A uniform stretch multiplies every eigenvalue and moves no eigenvector.

e) xI−S=(x−1−120x−1)xI - S = \begin{pmatrix} x - 1 & -\frac{1}{2} \\ 0 & x - 1 \end{pmatrix}, triangular, so cS(x)=(x−1)2c_S(x) = (x - 1)^2: the only eigenvalue is 11, a double root. 1I−S=(0−1200)1I - S = \begin{pmatrix} 0 & -\frac{1}{2} \\ 0 & 0 \end{pmatrix} gives x2=0x_2 = 0 with x1x_1 free, so E1(S)=span{(1,0)}E_1(S) = \text{span}\{(1, 0)\}, a single line. Only the horizontal fibres keep their line, and since the eigenvalue is 11 they are not even stretched; every other fibre is tilted, for instance S(0,1)=(12,1)S(0, 1) = (\frac{1}{2}, 1). The double root did not produce two directions here: the number of basic eigenvectors is whatever the reduction of λI−A\lambda I - A gives, and nothing else. The area is unchanged, det⁡S=1=1⋅1\det S = 1 = 1 \cdot 1, which is what a skew does.

fibre (1, 1): times 2fibre (2, 1): times 3fibre (1, 0): turnedopen dots: fibre ends before stretching

Exercise 10: A final exam question: the matrix whose eigenvectors are (1, t, t squared)

This is the shape of a long final exam question: one matrix, five moves, each using a different tool of the chapter. Here A=(0100016−116)A = \begin{pmatrix} 0 & 1 & 0 \\ 0 & 0 & 1 \\ 6 & -11 & 6 \end{pmatrix}, a matrix whose first two rows simply shift the entries of a vector and whose last row carries all the information.

  • a) Compute cA(x)c_A(x) by cofactor expansion along the first row of xI−AxI - A.
  • b) Factor cAc_A by testing the divisors of its constant term, and give the eigenvalues.
  • c) Show that for every number tt, A(1,t,t2)=(t, t2, 6t2−11t+6)A(1, t, t^2) = (t,\ t^2,\ 6t^2 - 11t + 6). Deduce that (1,t,t2)(1, t, t^2) is an eigenvector exactly when cA(t)=0c_A(t) = 0, and give a basis of each eigenspace.
  • d) Without any new determinant: is AA invertible? Give the eigenvalues of A−1A^{-1}, of A2A^2 and of A−2IA - 2I, and say whether A−2IA - 2I is invertible.
  • e) A matrix BB has the same first two rows as AA and last row (a,b,c)(a, b, c). Find aa, bb and cc so that the eigenvalues of BB are 11, 22 and 44: find cc from the trace and aa from the determinant first, then bb.
Show the solution

Answers

  • a) cA(x)=x3−6x2+11x−6c_A(x) = x^3 - 6x^2 + 11x - 6
  • b) cA(x)=(x−1)(x−2)(x−3)c_A(x) = (x - 1)(x - 2)(x - 3): eigenvalues 11, 22, 33
  • c) E1=span{(1,1,1)}E_1 = \text{span}\{(1, 1, 1)\}, E2=span{(1,2,4)}E_2 = \text{span}\{(1, 2, 4)\}, E3=span{(1,3,9)}E_3 = \text{span}\{(1, 3, 9)\}
  • d) Invertible. A−1A^{-1}: 11, 12\frac{1}{2}, 13\frac{1}{3}. A2A^2: 11, 44, 99. A−2IA - 2I: −1-1, 00, 11, not invertible.
  • e) c=7c = 7, a=8a = 8, b=−14b = -14: last row (8,−14,7)(8, -14, 7)

a) xI−A=(x−100x−1−611x−6)xI - A = \begin{pmatrix} x & -1 & 0 \\ 0 & x & -1 \\ -6 & 11 & x - 6 \end{pmatrix}. The first row has a zero in position (1,3)(1, 3), so two cofactors survive. Entry (1,1)(1, 1), sign ++: xdet⁡(x−111x−6)=x[x(x−6)+11]=x3−6x2+11xx \det\begin{pmatrix} x & -1 \\ 11 & x - 6 \end{pmatrix} = x\left[x(x - 6) + 11\right] = x^3 - 6x^2 + 11x. Entry (1,2)(1, 2) is −1-1, sign (−1)1+2=−1(-1)^{1+2} = -1: −(−1)det⁡(0−1−6x−6)=0⋅(x−6)−(−1)(−6)=−6-(-1)\det\begin{pmatrix} 0 & -1 \\ -6 & x - 6 \end{pmatrix} = 0 \cdot (x - 6) - (-1)(-6) = -6. So cA(x)=x3−6x2+11x−6c_A(x) = x^3 - 6x^2 + 11x - 6. The product −(−1)-(-1) is where the sign is usually lost: the entry is negative AND the position is negative, and both must be written.

b) A rational root of a monic polynomial with integer coefficients divides the constant term, so the candidates are ±1,±2,±3,±6\pm 1, \pm 2, \pm 3, \pm 6. cA(1)=1−6+11−6=0c_A(1) = 1 - 6 + 11 - 6 = 0, so (x−1)(x - 1) is a factor, and dividing gives cA(x)=(x−1)(x2−5x+6)=(x−1)(x−2)(x−3)c_A(x) = (x - 1)(x^2 - 5x + 6) = (x - 1)(x - 2)(x - 3). The eigenvalues are 11, 22 and 33. On an exam without a calculator, a characteristic cubic is always built to have small integer roots; if none of the divisors works, the polynomial is wrong, not the method.

c) A(1,t,t2)=(0+t+0, 0+0+t2, 6−11t+6t2)=(t, t2, 6t2−11t+6)A(1, t, t^2) = (0 + t + 0,\ 0 + 0 + t^2,\ 6 - 11t + 6t^2) = (t,\ t^2,\ 6t^2 - 11t + 6). For this to equal t(1,t,t2)=(t,t2,t3)t(1, t, t^2) = (t, t^2, t^3), the first two entries already agree, and the third requires 6t2−11t+6=t36t^2 - 11t + 6 = t^3, that is t3−6t2+11t−6=0t^3 - 6t^2 + 11t - 6 = 0, that is cA(t)=0c_A(t) = 0. The vector (1,t,t2)(1, t, t^2) is never zero, because of its first entry. So for each eigenvalue λ\lambda, the vector (1,λ,λ2)(1, \lambda, \lambda^2) is an eigenvector. Moreover, in (λI−A)x=0(\lambda I - A)x = 0 the first two rows read λx1=x2\lambda x_1 = x_2 and λx2=x3\lambda x_2 = x_3, so every solution is x1(1,λ,λ2)x_1(1, \lambda, \lambda^2): each eigenspace is a line. E1=span{(1,1,1)}E_1 = \text{span}\{(1, 1, 1)\}, E2=span{(1,2,4)}E_2 = \text{span}\{(1, 2, 4)\}, E3=span{(1,3,9)}E_3 = \text{span}\{(1, 3, 9)\}. Check one: A(1,3,9)=(3, 9, 6−33+54)=(3,9,27)=3(1,3,9)A(1, 3, 9) = (3,\ 9,\ 6 - 33 + 54) = (3, 9, 27) = 3(1, 3, 9).

d) 00 is not an eigenvalue, so AA is invertible; indeed det⁡A=1⋅2⋅3=6\det A = 1 \cdot 2 \cdot 3 = 6. The eigenvalues of A−1A^{-1} are the reciprocals 11, 12\frac{1}{2} and 13\frac{1}{3}, those of A2A^2 the squares 11, 44 and 99, and those of A−2IA - 2I the shifts 1−2=−11 - 2 = -1, 2−2=02 - 2 = 0 and 3−2=13 - 2 = 1, each with the same eigenvectors as AA. Since 00 is an eigenvalue of A−2IA - 2I, that matrix is NOT invertible, and (1,2,4)(1, 2, 4) is in its null space: (A−2I)(1,2,4)=(2−2, 4−4, 8−8)=0(A - 2I)(1, 2, 4) = (2 - 2,\ 4 - 4,\ 8 - 8) = 0. Being an eigenvalue of AA and making A−λIA - \lambda I singular are the same statement, read in two directions.

e) The computation of a), with the last row (a,b,c)(a, b, c), gives cB(x)=x3−cx2−bx−ac_B(x) = x^3 - cx^2 - bx - a. The trace of BB is 0+0+c=c0 + 0 + c = c, and it must equal 1+2+4=71 + 2 + 4 = 7, so c=7c = 7. The determinant of BB, by the first row, is −1⋅det⁡(01ac)=−(0−a)=a-1 \cdot \det\begin{pmatrix} 0 & 1 \\ a & c \end{pmatrix} = -(0 - a) = a, and it must equal 1⋅2⋅4=81 \cdot 2 \cdot 4 = 8, so a=8a = 8. Finally (x−1)(x−2)(x−4)=x3−7x2+14x−8(x - 1)(x - 2)(x - 4) = x^3 - 7x^2 + 14x - 8, and matching the xx coefficient, −b=14-b = 14, so b=−14b = -14. The last row is (8,−14,7)(8, -14, 7). Check: cB(1)=1−7+14−8=0c_B(1) = 1 - 7 + 14 - 8 = 0, and (1,4,16)(1, 4, 16) should be an eigenvector for 44: B(1,4,16)=(4, 16, 8−56+112)=(4,16,64)=4(1,4,16)B(1, 4, 16) = (4,\ 16,\ 8 - 56 + 112) = (4, 16, 64) = 4(1, 4, 16). Trace and determinant gave two of the three unknowns before any polynomial was expanded.

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