Linear Algebra and Vector Geometry 201-SN4-RE • CEGEP, Montreal

Revision sheet: eigenvalues and diagonalization (201-SN4-RE)

This sheet does not repeat the definition of an eigenvalue: you have it in your notes. It deals with what decides the mark at the end of 201-SN4-RE (formerly 201-NYC): the diagonalizability criterion applied correctly, the order in which PP and DD are filled in, and the checks that catch a wrong eigenvalue in ten seconds.

It is written for CEGEP students in Science and in the Social Science mathematics profile (201-105). Once you have read it, the corrected exercise set on the same chapter puts every reflex to the test.

Mark this sheet as read or add it to your favourites: a free account, no password, keeps your read sheets and favourites from one visit to the next, tells you which chapter to tackle next and lets you ask for the method or exercise you are missing. Create your space, an email is enough.

The thread of the chapter

An eigenvector is a DIRECTION that the matrix merely stretches. The whole chapter is about finding these directions, and the most expensive mistake is to believe there are always enough of them to diagonalize.

This chapter is part of 201-SN4-RE, Linear Algebra and Vector Geometry

The essentials

What an eigenvalue means, and how to find it

  • • λ\lambda is an EIGENVALUE of AA if there is a NON-ZERO vector v⃗\vec{v} such that Av⃗=λv⃗A\vec{v}=\lambda\vec{v}. That v⃗\vec{v} is an associated EIGENVECTOR.
  • • Geometrically, AA only STRETCHES v⃗\vec{v}, without changing its direction. A negative λ\lambda flips the vector, a zero λ\lambda crushes it onto the origin.
  • • CHARACTERISTIC POLYNOMIAL: the eigenvalues are the roots of det⁡(A−λI)=0\det(A-\lambda I)=0. Subtract λ\lambda along the WHOLE diagonal, then compute the determinant.
  • • For a 2×22\times 2 matrix it reads λ2−tr⁡(A)λ+det⁡(A)=0\lambda^{2}-\operatorname{tr}(A)\lambda+\det(A)=0, where the trace is the sum of the diagonal entries.
  • • Two free checks: the SUM of the eigenvalues is the trace, and their PRODUCT is the determinant.
vAv = 2vdirection preservedwAwdirection changed
With A=(2001)A=\begin{pmatrix} 2 & 0 \\ 0 & 1 \end{pmatrix}: the image of the eigenvector v⃗\vec{v} stays on its line, twice as long; the image of w⃗\vec{w}, which is not one, leaves its line.

These two checks are the best value in the chapter: they take five seconds and catch almost every calculation error in the characteristic polynomial.

Eigenspaces and the diagonalizability criterion

  • • Eλ=ker⁡(A−λI)E_{\lambda}=\ker(A-\lambda I) is the EIGENSPACE: you get it by solving the homogeneous system (A−λI)v⃗=0⃗(A-\lambda I)\vec{v}=\vec{0}. It is always a subspace, of dimension at least 11.
  • • ALGEBRAIC MULTIPLICITY of λ\lambda: its order as a root of the characteristic polynomial. GEOMETRIC MULTIPLICITY: dim⁡Eλ\dim E_{\lambda}.
  • • Always, geometric ≤\leq algebraic, and the inequality can be STRICT: that is exactly what prevents diagonalization.
  • • CRITERION: AA of order nn is diagonalizable if and only if the dimensions of the eigenspaces add up to nn, that is, if the two multiplicities agree for EVERY eigenvalue.
  • • Two easy cases where you conclude without calculation: nn DISTINCT eigenvalues, or a real SYMMETRIC matrix, which is always diagonalizable with orthogonal eigenvectors.
-3-2-1123456-5-4-3-2-1123456Av = 5vAu = 2uvuE₅E₂
For A=(4123)A=\begin{pmatrix} 4 & 1 \\ 2 & 3 \end{pmatrix}: E5E_{5} is the line of (1,1)(1, 1), E2E_{2} the line of (1,−2)(1, -2), and each vector on them is stretched by its eigenvalue. Two lines: diagonalizable.

A simple eigenvalue never causes trouble: its geometric multiplicity is necessarily 11. Only REPEATED eigenvalues require computing the dimension of the eigenspace.

Diagonalizing, and putting it to use

  • • A=PDP−1A=PDP^{-1}, where the COLUMNS of PP are the eigenvectors and DD is diagonal with the eigenvalues in the SAME ORDER.
  • • Column ii of PP must be an eigenvector associated with the eigenvalue in position ii of DD. The order is free, but it must be the same on both sides.
  • • An=PDnP−1A^{n}=PD^{n}P^{-1}, and DnD^{n} is obtained by raising each diagonal entry to the power nn. That is the whole point of diagonalizing.
  • • A check that avoids computing P−1P^{-1}: AP=PDAP=PD. Two matrix products are enough to validate PP and DD together.
  • • A real symmetric matrix is diagonalized in an ORTHONORMAL basis: eigenvectors associated with different eigenvalues are orthogonal, and you only need to normalize them.
X₀AX₀A²X₀A³X₀E₅
Same matrix: the directions of X0=(1,0)X_{0}=(1, 0), AX0AX_{0}, A2X0A^{2}X_{0}, A3X0A^{3}X_{0} (drawn at the same length) fold onto E5E_{5}: the eigenvalue with the largest absolute value imposes its direction.

For a sequence of vectors Xk+1=AXkX_{k+1}=AX_{k}, the eigenvalue with the largest absolute value ends up dominating: the limiting direction is that of its eigenvector, whatever the initial condition.

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. Mistaking the zero vector for an eigenvector

1 mark for rigour, and the question on the dimension of the eigenspace becomes inconsistent.

What not to write

“A0⃗=λ0⃗A\vec{0}=\lambda\vec{0} for every λ\lambda, so 0⃗\vec{0} is an eigenvector.”

What to write

“An eigenvector is NON-ZERO by definition. Otherwise every real number would be an eigenvalue of every matrix, and the notion would have no content.”

Why: 0⃗\vec{0} does belong to EλE_{\lambda}, which is a subspace, but it is not an EIGENVECTOR. The distinction shows in the write-up: “EλE_{\lambda} contains 0⃗\vec{0}” is true, “0⃗\vec{0} is an eigenvector” is false.

2. Forming the matrix A−λIA-\lambda I wrongly

the whole question, and the eigenvalues found have nothing to do with the matrix.

What not to write

“det⁡(A)−λ=0\det(A)-\lambda=0”, or λ\lambda subtracted from the top-left entry only.

What to write

“det⁡(A−λI)=0\det(A-\lambda I)=0: subtract λ\lambda from ALL the diagonal entries, then compute the determinant of the resulting matrix.”

Why: λI\lambda I is the diagonal matrix of λ\lambdas, not the number λ\lambda: you cannot subtract a number from a matrix. It is the same rule as for any matrix sum, entry by entry.

3. Giving an eigenspace reduced to a single vector

1 mark, and more if the question asked for the dimension of the eigenspace.

What not to write

“E4={(1,1)}E_{4}=\{(1, 1)\}.”

What to write

“E4=span⁡{(1,1)}E_{4}=\operatorname{span}\{(1, 1)\}, that is, the whole LINE: every non-zero multiple of (1,1)(1, 1) is also an eigenvector associated with 44.”

-3-2-1123-3-2-1123(1, 1)E₄
E4E_{4} is the whole LINE directed by (1,1)(1, 1): (2,2)(2, 2) and (−1,−1)(-1, -1), in green, are eigenvectors for 44 as well. Write E4=span⁡{(1,1)}E_{4}=\operatorname{span}\{(1, 1)\}.

Why: If Av⃗=λv⃗A\vec{v}=\lambda\vec{v}, then A(kv⃗)=λ(kv⃗)A(k\vec{v})=\lambda(k\vec{v}) for every kk: the property survives multiplication. An eigenvector is never unique, only its DIRECTION is.

4. Assuming the geometric multiplicity equals the algebraic one

the whole question, with an invented matrix PP whose columns are dependent.

What not to write

“λ=2\lambda=2 is a double root, so dim⁡E2=2\dim E_{2}=2 and the matrix is diagonalizable.”

What to write

“You have to COMPUTE dim⁡E2\dim E_{2}. For A=(2102)A=\begin{pmatrix} 2 & 1 \\ 0 & 2 \end{pmatrix}, the system (A−2I)v⃗=0⃗(A-2I)\vec{v}=\vec{0} gives y=0y=0: E2=span⁡{(1,0)}E_{2}=\operatorname{span}\{(1, 0)\}, of dimension 11. The matrix is NOT diagonalizable.”

v₁2v₁v₂Av₂only one eigendirection
The only direction this matrix preserves is the horizontal one: v2⃗\vec{v_{2}} tips toward it instead of staying on its line. One double eigenvalue, a single eigendirection.

Why: The inequality geometric ≤\leq algebraic can be strict, and precisely that case makes a matrix non-diagonalizable. A repeated eigenvalue always forces you to solve the system.

5. Filling PP and DD in different orders

the whole question, and the computation of AnA^{n} that follows gives nonsense.

What not to write

“P=(111−1)P=\begin{pmatrix} 1 & 1 \\ 1 & -1 \end{pmatrix} with v1⃗\vec{v_{1}}, associated with 44, in the first column, and D=(2004)D=\begin{pmatrix} 2 & 0 \\ 0 & 4 \end{pmatrix}.”

What to write

“Column ii of PP must be an eigenvector for the eigenvalue in position ii of DD: here D=(4002)D=\begin{pmatrix} 4 & 0 \\ 0 & 2 \end{pmatrix}. The check AP=PDAP=PD confirms it at once.”

Why: The equality AP=PDAP=PD is read column by column: Avi⃗=λivi⃗A\vec{v_{i}}=\lambda_{i}\vec{v_{i}}. If the indices do not match, the equality fails for every column.

6. Reversing the order of PP and P−1P^{-1} in the power

the whole power question, and the matrix obtained does not even have the right eigenvalues.

What not to write

“An=P−1DnPA^{n}=P^{-1}D^{n}P.”

What to write

“A=PDP−1A=PDP^{-1}, so An=PDnP−1A^{n}=PD^{n}P^{-1}, in the SAME order as AA. The inner P−1PP^{-1}P cancel and only the two outer factors remain.”

Why: The calculation A2=(PDP−1)(PDP−1)=PD(P−1P)DP−1=PD2P−1A^{2}=(PDP^{-1})(PDP^{-1})=PD(P^{-1}P)DP^{-1}=PD^{2}P^{-1} shows the order. Writing out this telescoping once is enough never to get it wrong again.

7. Concluding that there is no eigenvalue when the discriminant is negative

2 marks, and the geometric interpretation, often the next question, is lost.

What not to write

“The characteristic polynomial has a negative discriminant, so this matrix has no eigenvalues.”

What to write

“It has no REAL eigenvalue: no direction of the plane is preserved, which is the case for a rotation. Over C\mathbb{C}, it has two conjugate eigenvalues, and it is diagonalizable there.”

vAvwAwuAu
The rotation through 60∘60^{\circ} turns every vector through the same angle (image dashed): no arrow stays on its original line, so there is no real eigenvalue. Lengths, on the other hand, are preserved.

Why: The phrase “no eigenvalue” is wrong: you must say over which set. The geometric reading, on the other hand, is immediate and earns marks: a rotation through a non-zero angle leaves no line invariant.

8. Finding only the zero vector as a solution of the eigenvector system

the whole question, plus the time lost looking for the error somewhere other than where it is.

What not to write

“I solve (A−λI)v⃗=0⃗(A-\lambda I)\vec{v}=\vec{0} and get v⃗=0⃗\vec{v}=\vec{0}: there is no eigenvector for this λ\lambda.”

What to write

“If λ\lambda really is an eigenvalue, then det⁡(A−λI)=0\det(A-\lambda I)=0, so the homogeneous system NECESSARILY has infinitely many solutions. Finding only 0⃗\vec{0} proves a calculation error, most often in λ\lambda.”

Why: The eigenvalue was chosen precisely to make the matrix A−λIA-\lambda I singular. A pivot must therefore disappear: if none does, the characteristic polynomial is wrong.

Which method to choose

Is this matrix diagonalizable?

Look at the characteristic polynomial and the shape of the matrix. Three branches out of five answer without computing a single eigenspace.

yesyes, symmetricno
Eigendirections in order 22: two lines (distinct eigenvalues), two perpendicular lines (symmetric), or a single one for a double eigenvalue: one is missing, no diagonalization.
  • If nn DISTINCT real eigenvalues for a matrix of order nn → YES, diagonalizable, with no further check

    Example: λ=4\lambda=4 and λ=2\lambda=2 for a matrix of order 22

  • If a real SYMMETRIC matrix → YES, diagonalizable, and even in an orthonormal basis

    This is true even with repeated eigenvalues, and it spares you any dimension calculation.

  • If a REPEATED eigenvalue, non-symmetric matrix → you must COMPUTE dim⁡Eλ\dim E_{\lambda} and compare it with the algebraic multiplicity

    Example: (2102)\begin{pmatrix} 2 & 1 \\ 0 & 2 \end{pmatrix} has dim⁡E2=1\dim E_{2}=1 for a multiplicity of 22, so no

  • If a NEGATIVE discriminant for a real matrix of order 22 → not diagonalizable over R\mathbb{R}, for lack of a real eigenvalue; diagonalizable over C\mathbb{C}

    Geometrically, it is a rotation, possibly combined with a scaling.

  • If an already TRIANGULAR matrix → the eigenvalues are the diagonal entries, with no calculation; the multiplicities still have to be dealt with

A triple root λ\lambda in order 33? There is only one eigenspace, EλE_{\lambda}: the matrix is diagonalizable if and only if dim⁡Eλ=3\dim E_{\lambda}=3, that is, if A=λIA=\lambda I, with no calculation.

How to compute this expression once AA is diagonalized

Once A=PDP−1A=PDP^{-1} is written, most questions come down to a calculation on DD, which is diagonal and therefore immediate.

  • If you are asked for AnA^{n} → PDnP−1PD^{n}P^{-1}, with DnD^{n} obtained by raising each diagonal entry to the power nn

    Example: D=diag⁡(4,2)D=\operatorname{diag}(4, 2) gives D3=diag⁡(64,8)D^{3}=\operatorname{diag}(64, 8)

  • If you are asked for det⁡(A)\det(A) or tr⁡(A)\operatorname{tr}(A) → the product of the eigenvalues for the determinant, their sum for the trace

    It also works as a check on the eigenvalues found, in the other direction.

  • If you are asked for the eigenvalues of A−1A^{-1}, of AkA^{k} or of A+cIA+cI → 1λ\frac{1}{\lambda}, λk\lambda^{k}, λ+c\lambda+c, with the SAME eigenvectors

    No new calculation: this is the most frequent theory question at the end of the chapter.

  • If you are asked for the behaviour of a sequence Xk+1=AXkX_{k+1}=AX_{k} → decompose X0X_{0} in the eigenbasis, then multiply each component by λk\lambda^{k}

    The eigenvalue with the largest absolute value dominates and sets the limiting direction.

  • If you are asked whether AA is invertible → check whether 00 is an eigenvalue: AA is invertible if and only if no eigenvalue is zero

Never compute P−1P^{-1} unless you have to: the check AP=PDAP=PD validates the diagonalization without it, and many questions do not need it.

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.

Diagonalizing a matrix of order two

When to use it: The question asks you to diagonalize AA, or to find PP and DD such that A=PDP−1A=PDP^{-1}.

  1. 1 Write A−λIA-\lambda I in full, then expand det⁡(A−λI)\det(A-\lambda I) to get the characteristic polynomial.
  2. 2 Solve, give the eigenvalues, and check them with the trace and the determinant before going further.
  3. 3 For each eigenvalue, solve the homogeneous system (A−λI)v⃗=0⃗(A-\lambda I)\vec{v}=\vec{0} and give EλE_{\lambda} in the form span⁡{… }\operatorname{span}\{\dots\}.
  4. 4 Justify diagonalizability: distinct eigenvalues, or dimensions adding up to the order.
  5. 5 Write PP with the eigenvectors AS COLUMNS and DD with the eigenvalues in the SAME order, then check AP=PDAP=PD.

Concluding sentence

“The eigenvalues are 44 and 22, which are distinct, so AA is diagonalizable: with P=(111−1)P=\begin{pmatrix} 1 & 1 \\ 1 & -1 \end{pmatrix} and D=(4002)D=\begin{pmatrix} 4 & 0 \\ 0 & 2 \end{pmatrix}, we have A=PDP−1A=PDP^{-1}.”

The trap: Forgetting to justify diagonalizability and jumping straight to PP and DD. The marking scheme always puts half a mark on this sentence, and it is the only one that mentions the criterion.

Marking: 1 mark for the characteristic polynomial, 1 mark for the eigenspaces, 0.5 mark for the justification, 0.5 mark for PP, DD and the check.

Computing a power by diagonalization

When to use it: The question asks for AnA^{n}, or the state of a system after nn steps of an evolution Xk+1=AXkX_{k+1}=AX_{k}.

  1. 1 Diagonalize AA and restate A=PDP−1A=PDP^{-1} with PP and DD written out.
  2. 2 Write the telescoping An=PDnP−1A^{n}=PD^{n}P^{-1}, justified by the cancellation of the inner P−1PP^{-1}P.
  3. 3 Compute DnD^{n} by raising each diagonal entry to the power nn, and say so.
  4. 4 Compute P−1P^{-1}, then carry out the two products in the order PP, then DnD^{n}, then P−1P^{-1}.
  5. 5 Check on a small value of nn, for example n=2n=2, against the direct product A×AA\times A.

Concluding sentence

“Since A=PDP−1A=PDP^{-1}, we have An=PDnP−1A^{n}=PD^{n}P^{-1}, hence A3=(36282836)A^{3}=\begin{pmatrix} 36 & 28 \\ 28 & 36 \end{pmatrix}.”

The trap: Raising PP to the power nn along with DD. Only the diagonal matrix is raised to the power: PP and P−1P^{-1} stay unchanged, since they perform the change of basis.

Marking: 0.5 mark for writing An=PDnP−1A^{n}=PD^{n}P^{-1}, 0.5 mark for DnD^{n}, 1 mark for P−1P^{-1}, 1 mark for the final product.

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

Diagonalizing a symmetric matrix, then computing its cube

Let A=(3113)A=\begin{pmatrix} 3 & 1 \\ 1 & 3 \end{pmatrix}.

1) Find the eigenvalues and the eigenspaces of AA.

2) Write PP and DD such that A=PDP−1A=PDP^{-1}, and check.

3) Deduce A3A^{3}.

-112345-112345(3, 1)(1, 3)
The data: AA sends the unit square (in blue) onto the parallelogram built on its columns (3,1)(3, 1) and (1,3)(1, 3). Question 1 asks which directions this change merely stretches.

Step 1

tr⁡(A)=3+3=6\operatorname{tr}(A)=3+3=6 and det⁡(A)=9−1=8\det(A)=9-1=8, so the characteristic polynomial is λ2−6λ+8=0\lambda^{2}-6\lambda+8=0.

Why

The trace-determinant form avoids writing A−λIA-\lambda I in full in order 22, and it gives right away the two checks used in the next step.

Step 2

Δ=36−32=4\Delta=36-32=4, so λ1=6+22=4\lambda_{1}=\dfrac{6+2}{2}=4 and λ2=6−22=2\lambda_{2}=\dfrac{6-2}{2}=2. Check: 4+2=64+2=6 and 4×2=84\times 2=8.

Why

The check takes five seconds and catches any sign error in the polynomial. Two DISTINCT eigenvalues are already enough to guarantee diagonalizability.

Step 3

E4E_{4}: (A−4I)v⃗=0⃗(A-4I)\vec{v}=\vec{0} gives (−111−1)v⃗=0⃗\begin{pmatrix} -1 & 1 \\ 1 & -1 \end{pmatrix}\vec{v}=\vec{0}, that is −x+y=0-x+y=0, so E4=span⁡{(1,1)}E_{4}=\operatorname{span}\{(1, 1)\}.

Why

The two rows are opposite: a pivot has indeed disappeared, which confirms that 44 is a genuine eigenvalue. The subspace is a LINE, not an isolated vector.

Step 4

E2E_{2}: (A−2I)v⃗=0⃗(A-2I)\vec{v}=\vec{0} gives (1111)v⃗=0⃗\begin{pmatrix} 1 & 1 \\ 1 & 1 \end{pmatrix}\vec{v}=\vec{0}, that is x+y=0x+y=0, so E2=span⁡{(1,−1)}E_{2}=\operatorname{span}\{(1, -1)\}.

Why

The two eigenvectors are orthogonal, which was guaranteed in advance: AA is symmetric. It is a free check on both subspaces at once.

Step 5

AA has two distinct eigenvalues in order 22, so it is diagonalizable: P=(111−1)P=\begin{pmatrix} 1 & 1 \\ 1 & -1 \end{pmatrix} and D=(4002)D=\begin{pmatrix} 4 & 0 \\ 0 & 2 \end{pmatrix}.

Why

The order is free but it must be the SAME on both sides: v1⃗\vec{v_{1}} in the first column of PP forces 44 in the first position of DD.

Step 6

Check: AP=(424−2)AP=\begin{pmatrix} 4 & 2 \\ 4 & -2 \end{pmatrix} and PD=(424−2)PD=\begin{pmatrix} 4 & 2 \\ 4 & -2 \end{pmatrix}: the two agree.

Why

Two products, no inversion: it is the cheapest check, and it tests the order along with the eigenvectors.

Step 7

det⁡(P)=−2\det(P)=-2, so P−1=1−2(−1−1−11)=(121212−12)P^{-1}=\dfrac{1}{-2}\begin{pmatrix} -1 & -1 \\ -1 & 1 \end{pmatrix}=\begin{pmatrix} \frac{1}{2} & \frac{1}{2} \\ \frac{1}{2} & -\frac{1}{2} \end{pmatrix}.

Why

Apply the order-two recipe: swap the diagonal entries, change the sign of the off-diagonal ones, divide by the determinant. Here PP is symmetric, so P−1P^{-1} is too.

Step 8

A3=PD3P−1A^{3}=PD^{3}P^{-1} with D3=(64008)D^{3}=\begin{pmatrix} 64 & 0 \\ 0 & 8 \end{pmatrix}, which gives A3=(36282836)A^{3}=\begin{pmatrix} 36 & 28 \\ 28 & 36 \end{pmatrix}.

Why

Only DD is raised to the power; PP and P−1P^{-1} stay as they are. Direct check: A2=(106610)A^{2}=\begin{pmatrix} 10 & 6 \\ 6 & 10 \end{pmatrix}, then A2AA^{2}A gives the same result.

The conclusion, written out

AA has eigenvalues 44 and 22, with E4=span⁡{(1,1)}E_{4}=\operatorname{span}\{(1, 1)\} and E2=span⁡{(1,−1)}E_{2}=\operatorname{span}\{(1, -1)\}; it diagonalizes as A=PDP−1A=PDP^{-1} and A3=(36282836)A^{3}=\begin{pmatrix} 36 & 28 \\ 28 & 36 \end{pmatrix}.

The classic mistake on this problem: Writing D=(2004)D=\begin{pmatrix} 2 & 0 \\ 0 & 4 \end{pmatrix} while keeping (1,1)(1, 1) in the first column of PP. The check AP=PDAP=PD then fails on both columns, but only if you do it.

Learn by heart

  • • Av⃗=λv⃗A\vec{v}=\lambda\vec{v} with v⃗≠0⃗\vec{v}\neq\vec{0}: the zero vector is never an eigenvector.
  • • Eigenvalues: roots of det⁡(A−λI)=0\det(A-\lambda I)=0, with λ\lambda subtracted along the WHOLE diagonal.
  • • In order 22: λ2−tr⁡(A)λ+det⁡(A)=0\lambda^{2}-\operatorname{tr}(A)\lambda+\det(A)=0. Sum == trace, product == determinant.
  • • Eλ=ker⁡(A−λI)E_{\lambda}=\ker(A-\lambda I) is a SUBSPACE, so at least a line, never a single vector.
  • • Geometric ≤\leq algebraic, and equality for EVERY eigenvalue is the diagonalizability criterion.
  • • nn distinct eigenvalues, or a real symmetric matrix: diagonalizable with no further check.
  • • A=PDP−1A=PDP^{-1}: column ii of PP and position ii of DD must match.
  • • An=PDnP−1A^{n}=PD^{n}P^{-1}, and only DD is raised to the power.
  • • Check with AP=PDAP=PD, which avoids computing P−1P^{-1}.
  • • Negative discriminant: no REAL eigenvalue, so no direction preserved, as for a rotation.

Frequently asked questions

How do I find the eigenvalues of a two by two matrix?

Write the characteristic polynomial as lambda squared, minus the trace times lambda, plus the determinant, set equal to zero. The trace is the sum of the two diagonal entries. Then solve this quadratic equation, and check that the sum of the roots equals the trace and their product the determinant.

Why is the zero vector not an eigenvector?

Because the definition explicitly excludes it. If it were allowed, any number would be an eigenvalue of any matrix, since a matrix always sends the zero vector to itself. The notion would lose all content. The zero vector still belongs to the eigenspace, which is a subspace.

When is a matrix not diagonalizable?

When it has a repeated eigenvalue whose eigenspace has a dimension strictly smaller than its multiplicity. In other words, there are not enough eigendirections to form a basis. Over the real numbers, this is also the case for a matrix whose characteristic polynomial has a negative discriminant, such as a rotation.

What is diagonalization used for in practice?

It turns a hard calculation into an immediate one. Raising a matrix to a high power becomes a simple calculation on the diagonal entries, which lets you study an evolution after a large number of steps, for example two coupled populations, without doing the multiplications one by one.

How do I check a diagonalization without computing the inverse?

Compare two products: the original matrix times the change-of-basis matrix, and the change-of-basis matrix times the diagonal matrix. They must be identical. This check tests the eigenvectors, the eigenvalues and the order in which they are placed all at once, and it costs only two products.

Is a symmetric matrix always diagonalizable?

Yes, as long as it is real. It is a result of the course, valid even when an eigenvalue is repeated. Moreover, eigenvectors associated with different eigenvalues are automatically perpendicular to each other, which lets you choose an orthonormal basis of eigenvectors.

Practise it

Corrected exercises: Eigenvalues and diagonalization, 201-SN4-RE

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.

  • 16 corrected exercises
  • 160 points
  • 225 minutes
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