MATH 133 Linear Algebra and Geometry • McGill University, Montreal

Revision sheet: eigenvalues and eigenvectors (MATH 133)

This sheet is not a summary of section 3.3 of Nicholson: you already have the course notes. It answers one question only, what makes students lose marks on eigenvalues and eigenvectors in MATH 133 at McGill University, and which precise gesture avoids each loss.

The convention is the course's: cA(x)=det⁡(xI−A)c_A(x) = \det(xI - A). Every number below is done by hand, as on the exam, and every eigenvector quoted has been checked by the one multiplication that settles it: AxAx must be a multiple of xx.

The thread of the chapter

Every eigen question is a question about the single 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. When the reduction of λI−A\lambda I - A leaves no free variable, the λ\lambda is wrong, not the vector.

This chapter is part of MATH 133, Linear Algebra and Geometry (McGill)

The essentials

Two questions, two tools, one matrix

  • • 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; the vector x=0x = 0 never is.
  • • The NUMBERS: the eigenvalues are the real roots of cA(x)=det⁡(xI−A)c_A(x) = \det(xI - A), because λ\lambda is an eigenvalue exactly when λI−A\lambda I - A is singular.
  • • The DIRECTIONS: Eλ(A)E_\lambda(A) is the null space of λI−A\lambda I - A. Its basic solutions, one per free variable, are the basic eigenvectors and form a basis of Eλ(A)E_\lambda(A).
  • • A correct eigenvalue ALWAYS leaves at least one free variable in the reduction of λI−A\lambda I - A. No free variable means a wrong λ\lambda.
  • • An eigenvector is a direction that AA keeps on its LINE through the origin: stretched if λ>1\lambda > 1, shrunk if 0<λ<10 < \lambda < 1, reversed if λ<0\lambda < 0, crushed to 00 if λ=0\lambda = 0.
Au = 5uuwAwvAveigenvectors, even flippedturned: no
For A=(1423)A = \begin{pmatrix} 1 & 4 \\ 2 & 3 \end{pmatrix}: uu is stretched by 55 and ww is REVERSED, both stay on their dashed line and both are eigenvectors; vv leaves its line, so it is not one.

Every question of the chapter is one of these two: find λ\lambda (a determinant) or find xx (a row reduction). Writing which one you are doing on the first line of an answer is already half the method mark.

What you get for free once the eigenvalues are known

  • • 00 is an eigenvalue of AA if and only if AA is NOT invertible. A visible dependency between the columns is an eigenvector for 00.
  • • 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, each eigenvalue counted as often as it is a root.
  • • cA(0)=det⁡(−A)=(−1)ndet⁡Ac_A(0) = \det(-A) = (-1)^n \det A, so for a 3×33 \times 3, cA(0)=−det⁡Ac_A(0) = -\det A.
  • • Triangular AA: the eigenvalues are the diagonal entries. Block triangular (BC0D)\begin{pmatrix} B & C \\ 0 & D \end{pmatrix}: cA=cB cDc_A = c_B \, c_D.
  • • Powers, inverse, shifts, multiples and transpose: see the table below, each rule has a one-line proof starting from Ax=λxAx = \lambda x.

The rules in table form

Each row reads from left to right: the assumptions, then the result. A red cell is not an answer, it is the finding that the form settles nothing and the instruction to rewrite it. Every case is followed by a worked example.

Related matrices: which rules exist, and which do not

Read a line as: if Ax=λxAx = \lambda x with x≠0x \neq 0, then the matrix of the first column has the eigenvector and the eigenvalue of the next two. The examples use A=(5−63−4)A = \begin{pmatrix} 5 & -6 \\ 3 & -4 \end{pmatrix}, with eigenvalues 22 and −1-1 and eigenvectors (2,1)(2, 1) and (1,1)(1, 1). The red lines are the rules students invent.

MatrixEigenvectorEigenvalue
AkA^k same xx λk\lambda^k

Example: A3A^3 has eigenvalues 88 and −1-1: A3(2,1)=8(2,1)A^3(2, 1) = 8(2, 1).

A−1A^{-1} same xx 1λ\frac{1}{\lambda}

Example: A−1=12(4−63−5)A^{-1} = \frac{1}{2}\begin{pmatrix} 4 & -6 \\ 3 & -5 \end{pmatrix} and A−1(2,1)=(1,12)A^{-1}(2, 1) = (1, \frac{1}{2}): eigenvalue 12\frac{1}{2}, not −2-2.

A+cIA + cI same xx λ+c\lambda + c

Example: A+4IA + 4I has eigenvalues 2+4=62 + 4 = 6 and −1+4=3-1 + 4 = 3.

kAkA same xx kλk\lambda

Example: 3A3A has eigenvalues 66 and −3-3.

ATA^T DIFFERENT λ\lambda

Example: ATA^T has eigenvalues 22 and −1-1, but E2(AT)=span{(1,−1)}E_2(A^T) = \text{span}\{(1, -1)\}, not (2,1)(2, 1).

A+BA + B no rule λ+μ\lambda + \mu no such rule

Example: (0100)\begin{pmatrix} 0 & 1 \\ 0 & 0 \end{pmatrix} and (0010)\begin{pmatrix} 0 & 0 \\ 1 & 0 \end{pmatrix} each have only 00, yet their sum has 11 and −1-1.

What to do: Compute cA+Bc_{A+B} from scratch. The rule holds only when B=cIB = cI.

echelon form of AA no rule its diagonal no such rule

Example: (1232)\begin{pmatrix} 1 & 2 \\ 3 & 2 \end{pmatrix} has eigenvalues 44 and −1-1; after R2→R2−3R1R_2 \to R_2 - 3R_1 the diagonal reads 11 and −4-4.

What to do: Form xI−AxI - A first and take its determinant; reduce only λI−A\lambda I - A, and only to find vectors.

Every line in blue is proved in one line from Ax=λxAx = \lambda x: apply the operation to both sides. If you cannot write that line, the rule does not exist, which is exactly what happens with A+BA + B.

The mistakes that cost marks

These are the errors I correct most often in session. Each one costs marks on a paper, even when the reasoning behind it is right.

1. Reading the eigenvalues off a row reduced matrix

the whole question, and every eigenvector computed after it

What not to write

“R2→R2−3R1R_2 \to R_2 - 3R_1 turns (1232)\begin{pmatrix} 1 & 2 \\ 3 & 2 \end{pmatrix} into (120−4)\begin{pmatrix} 1 & 2 \\ 0 & -4 \end{pmatrix}, so the eigenvalues are 11 and −4-4.”

What to write

“cA(x)=det⁡(x−1−2−3x−2)=(x−1)(x−2)−6=x2−3x−4=(x−4)(x+1)c_A(x) = \det\begin{pmatrix} x - 1 & -2 \\ -3 & x - 2 \end{pmatrix} = (x - 1)(x - 2) - 6 = x^2 - 3x - 4 = (x - 4)(x + 1), so the eigenvalues are 44 and −1-1.”

Why: Row operations preserve the null space of AA, not its eigenvalues. The determinant has to be taken of xI−AxI - A BEFORE any reduction; reduction comes afterwards, on λI−A\lambda I - A, to find the vectors.

2. Giving the zero vector when the reduction has no free variable

2 marks, plus the eigenvalue that was actually missed

What not to write

“4I−A4I - A reduces to II, so E4={0}E_4 = \{0\} and the eigenvector is (0,0)(0, 0).”

What to write

“4I−A4I - A reduces to II, so it is invertible and 44 is NOT an eigenvalue: I go back to cA(x)c_A(x) and find the slip.”

Why: λI−A\lambda I - A is singular by construction when λ\lambda is a root of cAc_A, so a reduction with three pivots on a 3×33 \times 3 is an alarm, never an answer. For (12−26)\begin{pmatrix} 1 & 2 \\ -2 & 6 \end{pmatrix}, det⁡(4I−A)=cA(4)=−2≠0\det(4I - A) = c_A(4) = -2 \neq 0, and the true eigenvalues are 22 and 55.

3. Rejecting an eigenvector because its eigenvalue is negative

1 to 2 marks per missed eigenvector, and half the eigenvectors of any reflection

What not to write

“A(1,−1)=(−1,1)A(1, -1) = (-1, 1) points the other way, so (1,−1)(1, -1) is not an eigenvector.”

What to write

“A(1,−1)=(−1,1)=−1⋅(1,−1)A(1, -1) = (-1, 1) = -1 \cdot (1, -1): an eigenvector with eigenvalue −1-1.”

Why: The definition asks for AxAx on the LINE of xx, not in its direction. A reversed vector is the eigenvector of −1-1, the value every reflection has perpendicular to its mirror. The figure of the essentials shows ww reversed and kept.

4. Expanding a 3 by 3 along the wrong row, then fighting a cubic

10 minutes, and usually a sign error inside them

What not to write

“Along the first row: cA(x)=x3−10x2+31x−30c_A(x) = x^3 - 10x^2 + 31x - 30. I cannot factor it.”

What to write

“Row 2 of xI−AxI - A is (0, x−5, 0)(0,\ x - 5,\ 0), so 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).”

Why: A row or a column of xI−AxI - A with two zeros gives the polynomial ALREADY FACTORED. Scan for it before writing any cofactor: here A=(41−2050111)A = \begin{pmatrix} 4 & 1 & -2 \\ 0 & 5 & 0 \\ 1 & 1 & 1 \end{pmatrix}, and the first factor (x−5)(x - 5) comes out for free.

5. Giving one vector where the eigenspace needs two

1 mark, and the whole next chapter if the count is wrong

What not to write

“For λ=1\lambda = 1 the solutions are (−t,s,t)(-t, s, t), so the eigenvector is (−1,1,1)(-1, 1, 1).”

What to write

“Two free variables, so two basic eigenvectors: E1=span{(0,1,0),(−1,0,1)}E_1 = \text{span}\{(0, 1, 0), (-1, 0, 1)\}.”

Why: The question asks for a BASIS of the eigenspace: one basic eigenvector per free variable, obtained by setting one parameter to 11 and the others to 00. (−1,1,1)(-1, 1, 1) is an eigenvector, but alone it spans a line inside a plane. Worked in full in the example below.

6. Assuming A and its transpose share their eigenvectors

2 marks

What not to write

“ATA^T has the same characteristic polynomial, so E2(AT)=span{(2,1)}E_2(A^T) = \text{span}\{(2, 1)\} as for AA.”

What to write

“Same eigenvalues, but 2I−AT=(−3−366)2I - A^T = \begin{pmatrix} -3 & -3 \\ 6 & 6 \end{pmatrix} gives E2(AT)=span{(1,−1)}E_2(A^T) = \text{span}\{(1, -1)\}.”

2-1A2-1transpose
Same eigenvalues 22 and −1-1, four different lines: the eigenlines of AA on the left, those of ATA^T on the right. Transposing keeps the numbers and moves the directions.

Why: det⁡(xI−AT)=det⁡((xI−A)T)=det⁡(xI−A)\det(xI - A^T) = \det\left((xI - A)^T\right) = \det(xI - A) proves the eigenvalues agree and nothing more: the null spaces of λI−A\lambda I - A and λI−AT\lambda I - A^T are different. Here A=(5−63−4)A = \begin{pmatrix} 5 & -6 \\ 3 & -4 \end{pmatrix} and AT(2,1)=(13,−16)A^T(2, 1) = (13, -16).

7. Taking opposites instead of reciprocals for the inverse

1 mark for the answer and 1 for the missing proof

What not to write

“AA has eigenvalues 22 and −1-1, so A−1A^{-1} has −2-2 and 11.”

What to write

“From Ax=λxAx = \lambda x and λ≠0\lambda \neq 0: A−1x=1λxA^{-1}x = \frac{1}{\lambda}x, so A−1A^{-1} has 12\frac{1}{2} and −1-1, with the same eigenvectors.”

Why: Undoing a stretch by 22 is a stretch by 12\frac{1}{2}, not by −2-2. The proof is one line, multiply by A−1A^{-1} and divide by λ\lambda, and the division is where invertibility, that is λ≠0\lambda \neq 0, is used.

8. Mixing the two sign conventions for the characteristic polynomial

1 mark, and a wrong missing eigenvalue whenever the determinant is used to find one

What not to write

“cA(0)=det⁡Ac_A(0) = \det A, and cA(0)=(−λ1)(−λ2)(−λ3)c_A(0) = (-\lambda_1)(-\lambda_2)(-\lambda_3), so det⁡A=−λ1λ2λ3\det A = -\lambda_1\lambda_2\lambda_3.”

What to write

“cA(0)=det⁡(−A)=(−1)3det⁡A=−det⁡Ac_A(0) = \det(-A) = (-1)^3\det A = -\det A, and also cA(0)=−λ1λ2λ3c_A(0) = -\lambda_1\lambda_2\lambda_3, so det⁡A=λ1λ2λ3\det A = \lambda_1\lambda_2\lambda_3.”

Why: det⁡(A−xI)=(−1)ndet⁡(xI−A)\det(A - xI) = (-1)^n\det(xI - A): the two conventions agree for a 2×22 \times 2 and are OPPOSITE for a 3×33 \times 3. The roots never change, the coefficients do. Pick Nicholson's det⁡(xI−A)\det(xI - A) and keep it for the whole answer.

9. Inventing complex eigenvectors for a rotation

1 mark for the conclusion, and time lost outside the course

What not to write

“cR(x)=x2+1c_R(x) = x^2 + 1, so the eigenvalues of the rotation by 90∘90^\circ are ±i\pm i and I look for the eigenvectors.”

What to write

“cR(x)=x2+1≥1c_R(x) = x^2 + 1 \ge 1 has no real root: the rotation has no real eigenvalue and no eigenvector in R2\mathbb{R}^2, since a quarter turn moves every line.”

Why: In MATH 133 eigenvalues are real numbers attached to vectors of Rn\mathbb{R}^n. The expected answer is that observation, backed by the geometry of the decision tree figure below: no line through the origin survives a quarter turn.

Which method to choose

Where the eigenvalues come from, by the FORM of the matrix

Look at the shape of the matrix, or at what the statement already gives you, before writing any determinant

reflection1 and -1projection1 and 0rotation 90no real one
The reflection keeps LL (11) and reverses its perpendicular (−1-1); the projection keeps LL (11) and crushes the perpendicular to the dot (00); the quarter turn keeps no line at all.
  • If the matrix is triangular → the eigenvalues are the diagonal entries, no computation

    Example: (270−3)\begin{pmatrix} 2 & 7 \\ 0 & -3 \end{pmatrix} has eigenvalues 22 and −3-3

  • If the matrix is block triangular (BC0D)\begin{pmatrix} B & C \\ 0 & D \end{pmatrix} → cA=cB cDc_A = c_B \, c_D, two small polynomials instead of one big one

    Example: a 4×44 \times 4 with cB=(x−1)(x−3)c_B = (x - 1)(x - 3) and cD=(x−2)(x−5)c_D = (x - 2)(x - 5)

  • If a row or column of xI−AxI - A holds two zeros → expand along it: the polynomial comes out already factored

    Example: row (0, x−5, 0)(0,\ x - 5,\ 0) gives the factor (x−5)(x - 5) at once

  • If a general 2×22 \times 2 → cA(x)=x2−(tr A)x+det⁡Ac_A(x) = x^2 - (\text{tr}\,A)x + \det A

    Example: (12−26)\begin{pmatrix} 1 & 2 \\ -2 & 6 \end{pmatrix}: x2−7x+10=(x−2)(x−5)x^2 - 7x + 10 = (x - 2)(x - 5)

  • If the matrix is described geometrically → read the lines the map sends onto themselves

    Example: reflection 11 and −1-1, projection 11 and 00, rotation by 90∘90^\circ none

  • If some eigenvectors or eigenvalues are already given → multiply to get their eigenvalues, then the trace (or the determinant) for the last one

    Example: eigenvalues 00 and 55, trace 99: the third is 9−0−5=49 - 0 - 5 = 4

If no branch applies, expand det⁡(xI−A)\det(xI - A) along the row with the most zeros and test the divisors of the constant term: on an exam without a calculator the roots are always small integers. If none of them works, the polynomial is wrong.

How the answer is expected to be written

A marker ticks steps. Here they are in order, with the concluding sentence expected word for word.

Finding a basis of an eigenspace

When to use it: Any question that says find the eigenvectors, find the eigenspaces, or give a basis of Eλ(A)E_\lambda(A)

  1. 1 Write the eigenvalue you are using and form λI−A\lambda I - A explicitly, entries written out: subtract AA from λI\lambda I, so the off-diagonal entries change sign.
  2. 2 Row reduce, naming each operation (R2→R2−2R1R_2 \to R_2 - 2R_1). Check that at least one zero row appears; if not, stop and recheck the eigenvalue.
  3. 3 Write the general solution with one parameter per free variable, then split it into one vector per parameter: these are the basic eigenvectors.
  4. 4 Check each basic eigenvector by computing AxAx and comparing with λx\lambda x, entry by entry.
  5. 5 Conclude with the span, never with a single vector unless there is a single free variable.

Concluding sentence

“For λ=1\lambda = 1, the reduced form of I−AI - A gives x1=−x3x_1 = -x_3 with x2x_2 and x3x_3 free, so E1(A)=span{(0,1,0),(−1,0,1)}E_1(A) = \text{span}\{(0, 1, 0), (-1, 0, 1)\}.”

The trap: Reducing AA instead of λI−A\lambda I - A, or reducing λI−A\lambda I - A with a sign error on the diagonal. The multiplication check of step 4 catches both in ten seconds.

Marking: Typically 1 mark for the matrix lambda I minus A written correctly, 1 for the reduction with named operations, 1 for the basis, and the check is what protects the other three.

Check before you hand in

Five minutes of checking recover more marks than one more problem started in a hurry.

The typical problem, taken apart

A 3 by 3 with a repeated eigenvalue, from the polynomial to the eigenspaces

Let A=(403111102)A = \begin{pmatrix} 4 & 0 & 3 \\ 1 & 1 & 1 \\ 1 & 0 & 2 \end{pmatrix}. Find the characteristic polynomial, the eigenvalues, and a basis of each eigenspace.

No calculator. Every step must be justified as on a MATH 133 final.

Step 1

xI−A=(x−40−3−1x−1−1−10x−2)xI - A = \begin{pmatrix} x - 4 & 0 & -3 \\ -1 & x - 1 & -1 \\ -1 & 0 & x - 2 \end{pmatrix}. Its second COLUMN is (0, x−1, 0)(0,\ x - 1,\ 0): expand along it. The entry is in position (2,2)(2, 2), sign ++.

Why

Scanning for zeros is the first mark of the question. A column works exactly like a row, and this one reduces a 3×33 \times 3 determinant to a single 2×22 \times 2.

Step 2

cA(x)=(x−1)det⁡(x−4−3−1x−2)=(x−1)[(x−4)(x−2)−3]=(x−1)(x2−6x+5)=(x−1)2(x−5)c_A(x) = (x - 1)\det\begin{pmatrix} x - 4 & -3 \\ -1 & x - 2 \end{pmatrix} = (x - 1)\left[(x - 4)(x - 2) - 3\right] = (x - 1)(x^2 - 6x + 5) = (x - 1)^2(x - 5).

Why

The product of the off-diagonal entries is (−3)(−1)=3(-3)(-1) = 3, and it is SUBTRACTED. The quadratic factors because 1+5=61 + 5 = 6 and 1⋅5=51 \cdot 5 = 5, and it happens to share the root 11 with the factor already out: the eigenvalue 11 is a double root.

Step 3

λ=5\lambda = 5: 5I−A=(10−3−14−1−103)5I - A = \begin{pmatrix} 1 & 0 & -3 \\ -1 & 4 & -1 \\ -1 & 0 & 3 \end{pmatrix}. R2→R2+R1R_2 \to R_2 + R_1 gives (0,4,−4)(0, 4, -4), R3→R3+R1R_3 \to R_3 + R_1 gives a zero row, R2→14R2R_2 \to \frac{1}{4}R_2 gives (0,1,−1)(0, 1, -1). So x1=3x3x_1 = 3x_3, x2=x3x_2 = x_3: E5=span{(3,1,1)}E_5 = \text{span}\{(3, 1, 1)\}.

Why

The zero row is the confirmation that 55 is right. One free variable, one basic eigenvector. Each operation is named because that is where the method marks are.

Step 4

λ=1\lambda = 1: I−A=(−30−3−10−1−10−1)I - A = \begin{pmatrix} -3 & 0 & -3 \\ -1 & 0 & -1 \\ -1 & 0 & -1 \end{pmatrix}. R1→−13R1R_1 \to -\frac{1}{3}R_1 gives (1,0,1)(1, 0, 1), then R2→R2+R1R_2 \to R_2 + R_1 and R3→R3+R1R_3 \to R_3 + R_1 give two zero rows. So x1=−x3x_1 = -x_3 with x2=sx_2 = s and x3=tx_3 = t free: x=s(0,1,0)+t(−1,0,1)x = s(0, 1, 0) + t(-1, 0, 1), and E1=span{(0,1,0),(−1,0,1)}E_1 = \text{span}\{(0, 1, 0), (-1, 0, 1)\}.

Why

Two free variables give TWO basic eigenvectors, one per parameter. The column of x2x_2 is entirely zero, so x2x_2 is free even though no equation mentions it: forgetting it is the classic way to lose (0,1,0)(0, 1, 0).

Step 5

Checks: A(3,1,1)=(15,5,5)A(3, 1, 1) = (15, 5, 5), A(0,1,0)=(0,1,0)A(0, 1, 0) = (0, 1, 0), A(−1,0,1)=(−1,0,1)A(-1, 0, 1) = (-1, 0, 1). Trace 4+1+2=7=1+1+54 + 1 + 2 = 7 = 1 + 1 + 5 and det⁡A=1⋅(8−3)=5=1⋅1⋅5\det A = 1 \cdot (8 - 3) = 5 = 1 \cdot 1 \cdot 5.

Why

Three multiplications and two sums confirm every number on the page. The repeated eigenvalue is counted twice in the trace and in the product, which is what makes both checks close.

The conclusion, written out

“cA(x)=(x−1)2(x−5)c_A(x) = (x - 1)^2(x - 5). The eigenvalues are 11 (double root) and 55, with E1(A)=span{(0,1,0),(−1,0,1)}E_1(A) = \text{span}\{(0, 1, 0), (-1, 0, 1)\} and E5(A)=span{(3,1,1)}E_5(A) = \text{span}\{(3, 1, 1)\}.”

The classic mistake on this problem: Expanding along the first row, which gives (x−4)(x−1)(x−2)−3(x−1)(x - 4)(x - 1)(x - 2) - 3(x - 1) and then an expanded cubic, x3−7x2+11x−5x^3 - 7x^2 + 11x - 5, to be factored by trial; or solving I−AI - A with only x1x_1 and x3x_3 in mind and reporting the single eigenvector (−1,0,1)(-1, 0, 1) for λ=1\lambda = 1.

Learn by heart

  • • Ax=λxAx = \lambda x with x≠0x \neq 0. λ=0\lambda = 0 is allowed and means AA is not invertible.
  • • cA(x)=det⁡(xI−A)c_A(x) = \det(xI - A); eigenvalues are its real roots; Eλ(A)E_\lambda(A) is the null space of λI−A\lambda I - A.
  • • A correct λ\lambda ALWAYS leaves a free variable in λI−A\lambda I - A. One basic eigenvector per free variable.
  • • Expand xI−AxI - A along the row or column with the most zeros. Triangular: the diagonal. Block triangular: cB cDc_B \, c_D.
  • • AkA^k: λk\lambda^k. A−1A^{-1}: 1λ\frac{1}{\lambda}. A+cIA + cI: λ+c\lambda + c. kAkA: kλk\lambda. Same eigenvectors. ATA^T: same λ\lambda, different vectors.
  • • tr A=\text{tr}\,A = sum of the eigenvalues, det⁡A=\det A = their product, repeated ones counted twice.
  • • Reflection: 11 and −1-1. Projection: 11 and 00. Rotation by 90∘90^\circ: no real eigenvalue.
  • • NEVER read eigenvalues off a row reduced matrix.

Frequently asked questions

How do I find the eigenvalues and eigenvectors of a 3 by 3 matrix by hand?

Form the matrix x times the identity minus A and look for a row or column with two zeros: expanding along it gives the characteristic polynomial already factored. Its roots are the eigenvalues. Then, for each eigenvalue, row reduce lambda times the identity minus A and read one basic eigenvector per free variable. Check each one by multiplying it by A.

Why can't I read the eigenvalues off the row echelon form?

Because row operations change the eigenvalues. They preserve the null space of a matrix, not its characteristic polynomial. The matrix with rows 1, 2 and 3, 2 has eigenvalues 4 and minus 1, but one row operation turns its diagonal into 1 and minus 4. The eigenvalues can be read off the diagonal only when the original matrix is already triangular.

Can zero be an eigenvalue?

Yes. Zero is an eigenvalue exactly when the matrix is not invertible, because then some non-zero vector is sent to the zero vector. What can never happen is the zero VECTOR being an eigenvector: it would satisfy the equation for every number at once, so the definition excludes it. Two different zeros, two different statements.

Does every matrix have real eigenvalues?

No. The rotation of the plane by ninety degrees moves every line through the origin, so no non-zero vector stays on its line, and its characteristic polynomial x squared plus one has no real root. In MATH 133 the expected answer is exactly that: the matrix has no real eigenvalue and no eigenvector in the plane. Complex eigenvalues are not part of the course.

How do I find a missing eigenvalue with the trace and the determinant?

The trace, the sum of the diagonal entries, equals the sum of the eigenvalues, and the determinant equals their product, each eigenvalue counted as often as it is a root. If two eigenvalues of a 3 by 3 are known, the third is the trace minus the other two. When zero is one of them the determinant is zero and tells you nothing, so use the trace.

Practise it

Corrected exercises: Eigenvalues and eigenvectors, MATH 133 at McGill

A method is proved on a paper, not on a sheet. The set for the same chapter takes each of these traps into a problem, with the solution written out step by step.

  • 10 corrected exercises
  • 100 points
  • 150 minutes
Do the exercises
Previous sheet Linear transformations Next sheet Diagonalization

See also

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