Eigenvalues and eigenvectors

At a Glance

Why This Chapter Matters

Eigenvalues and eigenvectors appear in 10 of the last 14 years — a perfect run, placing this atom among the highest-frequency items in Paper 1. Questions split roughly 6:3 between “find eigenvalues and eigenvectors of a given matrix” (pure computation) and “prove a theorem about eigenvalues” (conceptual). The computation questions follow a single repeatable template; the theorem questions each have a one-paragraph proof. The 2024 paper raised the stakes with a 20-mark two-part question that asked for eigenvectors of A−15A^{-15} — demonstrating that the “spectral inheritance” rule (AkA^k has the same eigenvectors as AA, eigenvalues λk\lambda^k) must be memorised explicitly.

Minimum Theory

Characteristic polynomial. For an n×nn\times n matrix AA, the eigenvalues are the roots of the characteristic polynomial p(λ)=det⁡(A−λI)=0p(\lambda)=\det(A-\lambda I)=0. For a 3×33\times 3 matrix this is a cubic; factor by trying integer divisors of the constant term. The algebraic multiplicity of λ\lambda is its multiplicity as a root of pp; the geometric multiplicity is dim⁡ker⁡(A−λI)=n−rank⁡(A−λI)\dim\ker(A-\lambda I)=n-\operatorname{rank}(A-\lambda I). Always: geometric ≤\le algebraic multiplicity. AA is diagonalisable iff for every eigenvalue, geometric = algebraic multiplicity.

Key spectral facts:

Rotation in R2\mathbb R^2. The rotation matrix Tθ=(cos⁡θ−sin⁡θsin⁡θcos⁡θ)T_\theta=\bigl(\begin{smallmatrix}\cos\theta&-\sin\theta\\\sin\theta&\cos\theta\end{smallmatrix}\bigr) has characteristic polynomial λ2−2cos⁡θ λ+1\lambda^2-2\cos\theta\,\lambda+1. Discriminant =4cos⁡2θ−4=−4sin⁡2θ≤0= 4\cos^2\theta-4 = -4\sin^2\theta \le 0; real eigenvalues only when sin⁡θ=0\sin\theta=0 (i.e. θ=0\theta=0 or π\pi). For θ=π/2\theta=\pi/2: p(λ)=λ2+1p(\lambda)=\lambda^2+1, eigenvalues ±i\pm i.

Question Archetypes

Four patterns cover every eigenvalue question in the corpus.

ArchetypeYou are seeing this when…
eigen-computation”find the eigenvalues and eigenvectors” of a given matrix; possibly “hence find eigenvectors of A−kA^{-k}“
eigenvalue-bounda structured matrix (unitary, Hermitian, DFT-type); bound the sum or product of $
eigenvector-independence-proof”prove that eigenvectors for distinct eigenvalues are linearly independent”
no-real-eigenvaluea rotation or anti-symmetric operator; prove it has no real eigenvalue

eigen-computation (6 question(s); 2014, 2015, 2016, 2021, 2024, 2025)

Recognition Cues

Solution Template

  1. Write det⁡(A−λI)\det(A-\lambda I) and expand (for 3×33\times3: cofactor along the most sparse row/column).
  2. Factor the cubic: find one integer root by testing divisors of the constant term; then divide to get a quadratic.
  3. Cross-check: trace =∑λi=\sum\lambda_i and determinant =∏λi=\prod\lambda_i.
  4. For each λ\lambda: row-reduce (A−λI)(A-\lambda I) to echelon form; identify the null space basis. Verify algebraic = geometric multiplicity at any repeated eigenvalue.
  5. If the question asks for A−kA^{-k}: state “eigenvectors of AA and A−kA^{-k} are identical; eigenvalues of A−kA^{-k} are λ−k\lambda^{-k}.” Do not re-compute.

Worked Example(s)

2014 Paper 1, 2014-P1-Q3c-i (8 marks)

A=(−22−321−6−1−20)A=\bigl(\begin{smallmatrix}-2&2&-3\\2&1&-6\\-1&-2&0\end{smallmatrix}\bigr). Find eigenvalues and eigenvectors.

Characteristic polynomial. Expanding det⁡(A−λI)\det(A-\lambda I) along row 1: p(λ)=(λ+3)[−(λ+2)(λ−4)+7]=(λ+3)(λ+3)(λ−5)⋅(−1)p(\lambda) = (\lambda+3)[-(\lambda+2)(\lambda-4)+7] = (\lambda+3)(\lambda+3)(\lambda-5) \cdot (-1) ⇒p(λ)=−(λ+3)2(λ−5).\Rightarrow p(\lambda)=-(\lambda+3)^2(\lambda-5).

Eigenvalues: λ=5\lambda=5 (simple) and λ=−3\lambda=-3 (algebraic multiplicity 2).

Eigenvector for λ=5\lambda=5. Row-reduce A−5IA-5I: pivot equations yield y=−2zy=-2z, x=−zx=-z. Take z=−1z=-1:   v1=(1,2,−1) for λ=5.  \boxed{\;v_1=(1,2,-1)\text{ for }\lambda=5.\;}

Eigenvectors for λ=−3\lambda=-3. (A+3I)(A+3I) row-reduces to a single equation x+2y−3z=0x+2y-3z=0 (rank 1 ⇒ geometric multiplicity 2). Two free variables:   v2=(−2,1,0),v3=(3,0,1) for λ=−3.  \boxed{\;v_2=(-2,1,0),\quad v_3=(3,0,1)\text{ for }\lambda=-3.\;}

Check: trace =5+(−3)+(−3)=−1=−2+1+0=5+(-3)+(-3)=-1=-2+1+0 ✓; det =5⋅9=45=5\cdot9=45: verify directly ✓.


2015 Paper 1, 2015-P1-Q2c (12 marks)

A=(113151311)A=\bigl(\begin{smallmatrix}1&1&3\\1&5&1\\3&1&1\end{smallmatrix}\bigr) (symmetric). Find eigenvalues and eigenvectors.

Characteristic polynomial. Expanding and collecting (note the λ\lambda coefficient cancels — a reliable check): p(λ)=−λ3+7λ2−36=0  ⟹  λ3−7λ2+36=0.p(\lambda) = -\lambda^3+7\lambda^2-36 = 0 \;\Longrightarrow\; \lambda^3-7\lambda^2+36=0.

Trial root λ=−2\lambda=-2: −8−28+36=0-8-28+36=0 ✓. Factor: (λ+2)(λ−3)(λ−6)=0(\lambda+2)(\lambda-3)(\lambda-6)=0.

Eigenvalues: λ=−2,3,6\lambda=-2,3,6 (all distinct; trace =7=7 ✓).

Eigenvectors (each by 2-equation row reduction): v1=(1,0,−1) (λ=−2),v2=(1,−1,1) (λ=3),v3=(1,2,1) (λ=6).v_1=(1,0,-1)\ (\lambda=-2),\quad v_2=(1,-1,1)\ (\lambda=3),\quad v_3=(1,2,1)\ (\lambda=6).

Orthogonality check (AA symmetric, distinct λ\lambda): v1⋅v2=0v_1\cdot v_2=0, v1⋅v3=0v_1\cdot v_3=0, v2⋅v3=0v_2\cdot v_3=0 ✓.


2016 Paper 1, 2016-P1-Q2b-i (8 marks)

A=(110110001)A=\bigl(\begin{smallmatrix}1&1&0\\1&1&0\\0&0&1\end{smallmatrix}\bigr). Find eigenvalues and eigenvectors.

Block structure. AA is block-diagonal: (1111)⊕[1]\bigl(\begin{smallmatrix}1&1\\1&1\end{smallmatrix}\bigr)\oplus[1]. Characteristic polynomial: p(λ)=[(1−λ)2−1]⋅(1−λ)=λ(λ−2)(1−λ).p(\lambda)=[(1-\lambda)^2-1]\cdot(1-\lambda)=\lambda(\lambda-2)(1-\lambda).

Eigenvalues: λ=0,1,2\lambda=0,1,2.

Eigenvectors: λ=0\lambda=0: x+y=0,z=0x+y=0,z=0 → (1,−1,0)(1,-1,0). λ=1\lambda=1: x=y=0,zx=y=0,z free → (0,0,1)(0,0,1). λ=2\lambda=2: x=y,z=0x=y,z=0 → (1,1,0)(1,1,0).


2021 Paper 1, 2021-P1-Q4a-ii (10 marks)

A=(0−ii0)A=\bigl(\begin{smallmatrix}0&-i\\i&0\end{smallmatrix}\bigr) over C\mathbb C. Find eigenvalues and eigenvectors.

Characteristic polynomial. det⁡(A−λI)=λ2−(−i)(i)=λ2−1\det(A-\lambda I)=\lambda^2-(-i)(i)=\lambda^2-1 (since −i⋅i=−i2=1-i\cdot i=-i^2=1). Eigenvalues: λ=±1\lambda=\pm1 (real, as expected for a Hermitian matrix — this is the Pauli matrix σy\sigma_y).

Eigenvectors. For λ=1\lambda=1: −v1−iv2=0⇒v1=−iv2-v_1-iv_2=0\Rightarrow v_1=-iv_2; take v2=1v_2=1: v1=(1,i)Tv_1=(1,i)^T. For λ=−1\lambda=-1: v1−iv2=0v_1-iv_2=0; v2=(i,1)Tv_2=(i,1)^T.

Verify: A(1,i)T=(−i⋅i, i⋅1)T=(1,i)TA(1,i)^T=(-i\cdot i,\,i\cdot 1)^T=(1,i)^T ✓. Orthogonality: (1,−i)⋅(i,1)T=i−i=0(1,-i)\cdot(i,1)^T=i-i=0 ✓.


2024 Paper 1, 2024-P1-Q4a (20 marks)

A=(324202423)A=\bigl(\begin{smallmatrix}3&2&4\\2&0&2\\4&2&3\end{smallmatrix}\bigr). Find eigenvalues and eigenvectors of AA; hence find those of A−15A^{-15}.

Characteristic polynomial. Expanding det⁡(A−λI)\det(A-\lambda I): λ3−6λ2−15λ−8=0  ⟹  (λ+1)2(λ−8)=0.\lambda^3-6\lambda^2-15\lambda-8=0 \;\Longrightarrow\; (\lambda+1)^2(\lambda-8)=0.

Eigenvalues: λ=8\lambda=8 (simple), λ=−1\lambda=-1 (algebraic multiplicity 2). Trace =6=8−1−1=6=8-1-1 ✓; det =8=8⋅1⋅1=8=8\cdot1\cdot1 ✓.

Eigenvectors. For λ=8\lambda=8: row-reduce A−8IA-8I; get v1=2v2v_1=2v_2, v3=2v2v_3=2v_2 → (2,1,2)T(2,1,2)^T. For λ=−1\lambda=-1: all rows of A+IA+I collapse to 2v1+v2+2v3=02v_1+v_2+2v_3=0 (rank 1, geometric multiplicity 2); basis (1,−2,0)T(1,-2,0)^T and (0,−2,1)T(0,-2,1)^T.

Eigenvalues of A−15A^{-15}. Eigenvectors are unchanged. Eigenvalues become λ−15\lambda^{-15}: 8−15=2−458^{-15}=2^{-45} for (2,1,2)T(2,1,2)^T and (−1)−15=−1(-1)^{-15}=-1 for (1,−2,0)T(1,-2,0)^T and (0,−2,1)T(0,-2,1)^T.

  Same eigenvectors as A;eigenvalues 2−45 and −1 (mult. 2).  \boxed{\;\text{Same eigenvectors as }A;\quad \text{eigenvalues }2^{-45}\text{ and }-1\ (\text{mult. }2).\;}


2025 Paper 1, 2025-P1-Q4c-i (12 marks)

A=(12021−62−23)A=\bigl(\begin{smallmatrix}1&2&0\\2&1&-6\\2&-2&3\end{smallmatrix}\bigr). Find eigenvalues and eigenvectors.

Characteristic polynomial. Expanding along row 1 (third entry is 0 — one cofactor vanishes): p(λ)=−λ3+5λ2+9λ−45=0  ⟹  λ3−5λ2−9λ+45=0.p(\lambda) = -\lambda^3+5\lambda^2+9\lambda-45 = 0 \;\Longrightarrow\; \lambda^3-5\lambda^2-9\lambda+45=0.

Group: λ2(λ−5)−9(λ−5)=(λ−5)(λ2−9)=(λ−5)(λ−3)(λ+3)=0\lambda^2(\lambda-5)-9(\lambda-5)=(\lambda-5)(\lambda^2-9)=(\lambda-5)(\lambda-3)(\lambda+3)=0.

Eigenvalues: λ=3,5,−3\lambda=3,5,-3.

Eigenvectors. For λ=3\lambda=3: y=xy=x, z=0z=0 → (1,1,0)T(1,1,0)^T. For λ=5\lambda=5: y=2xy=2x, z=−xz=-x → (1,2,−1)T(1,2,-1)^T. For λ=−3\lambda=-3: y=−2xy=-2x, z=−xz=-x → (1,−2,−1)T(1,-2,-1)^T.

Common Traps


eigenvalue-bound (1 question(s); 2013)

Recognition Cues

Solution Template

  1. Compute A∗AA^*A entry-by-entry (dot products of rows of A‾\overline A with columns of AA); use 1+ω+ω2=01+\omega+\omega^2=0 and ∣ω∣=1|\omega|=1 to collapse each entry to zero (off-diagonal) or nn (diagonal).
  2. Conclude A∗A=cIA^*A = cI (scalar matrix); singular values of AA are all c\sqrt c.
  3. For A2A^2: (A2)∗(A2)=A∗∗A∗AA=A∗(cI)A=c A∗A=c2I(A^2)^*(A^2) = A^{**}A^*AA = A^*(cI)A = c\,A^*A = c^2 I, so singular values of A2A^2 are all cc.
  4. A2A^2 is normal (A∗A=AA∗⇒(A2)∗A2=A2(A2)∗A^*A = AA^* \Rightarrow (A^2)^*A^2 = A^2(A^2)^*). For normal matrices the spectral theorem gives ∣λi∣=σi|\lambda_i| = \sigma_i. Therefore each ∣λi(A2)∣=c|\lambda_i(A^2)| = c, and the sum is nc≤Knc \le K.

Worked Example(s)

2013 Paper 1, 2013-P1-Q2b-i (8 marks)

A=(1111ω2ω1ωω2)A=\bigl(\begin{smallmatrix}1&1&1\\1&\omega^2&\omega\\1&\omega&\omega^2\end{smallmatrix}\bigr), ω≠1\omega\ne1, ω3=1\omega^3=1. Show ∣λ1∣+∣λ2∣+∣λ3∣≤9|\lambda_1|+|\lambda_2|+|\lambda_3|\le 9.

Compute A∗AA^*A. Note AA is symmetric so A∗=A‾A^* = \overline A. The (i,j)(i,j)-entry of A‾⋅A\overline A \cdot A is the inner product of row ii of A‾\overline A with column jj of AA. All off-diagonal entries involve 1+ω+ω2=01+\omega+\omega^2=0 or 1+ω3+ω3=31+\omega^3+\omega^3=3 — using ω3=1\omega^3=1, off-diagonal entries vanish and diagonal entries equal 3: A∗A=3I.A^*A = 3I.

Singular values of A2A^2. (A2)∗(A2)=A∗(A∗A)A=A∗(3I)A=3A∗A=9I(A^2)^*(A^2) = A^*(A^*A)A = A^*(3I)A = 3A^*A = 9I. So singular values of A2A^2 are all 33.

Spectral theorem. A2A^2 is normal (the same calculation shows AA∗=3IAA^*=3I as well, so A∗A=AA∗A^*A=AA^*, and thus (A2)∗A2=A2(A2)∗=9I(A^2)^*A^2=A^2(A^2)^*=9I). For a normal matrix, ∣λi∣=σi|\lambda_i|=\sigma_i, so ∣λi(A2)∣=3|\lambda_i(A^2)|=3 for all ii. ∣λ1∣+∣λ2∣+∣λ3∣=9≤9. ■|\lambda_1|+|\lambda_2|+|\lambda_3|=9\le 9.\ \blacksquare

The bound is attained exactly (not strict).

Common Traps


eigenvector-independence-proof (1 question(s); 2017)

Recognition Cues

Solution Template

Proof by induction on the number of eigenvectors kk:

  1. Base case (k=1k=1): a single non-zero vector is trivially independent.
  2. Inductive step: assume any k−1k-1 eigenvectors for distinct eigenvalues are independent. Suppose ∑i=1kcivi=0\sum_{i=1}^k c_i v_i = \mathbf0.
  3. Apply AA: ∑ciλivi=0\sum c_i\lambda_i v_i = \mathbf0. Subtract λk\lambda_k times the original relation: ∑i=1k−1ci(λi−λk)vi=0\sum_{i=1}^{k-1}c_i(\lambda_i-\lambda_k)v_i=\mathbf0.
  4. By hypothesis, ci(λi−λk)=0c_i(\lambda_i-\lambda_k)=0 for i<ki<k. Since λi≠λk\lambda_i\ne\lambda_k, we get ci=0c_i=0 for i<ki<k. Then ckvk=0c_kv_k=\mathbf0 and vk≠0v_k\ne\mathbf0 gives ck=0c_k=0.

Worked Example(s)

2017 Paper 1, 2017-P1-Q3b (10 marks)

Prove distinct non-zero eigenvectors of a matrix are linearly independent.

Setup. The correct statement: eigenvectors v1,…,vkv_1,\ldots,v_k belonging to distinct eigenvalues λ1,…,λk\lambda_1,\ldots,\lambda_k are linearly independent. State this clearly — the problem’s wording is slightly imprecise.

Suppose c1v1+⋯+ckvk=0c_1v_1+\cdots+c_kv_k=\mathbf0. (1)\qquad(1)

Apply AA: c1λ1v1+⋯+ckλkvk=0.(2)c_1\lambda_1v_1+\cdots+c_k\lambda_kv_k=\mathbf0.\qquad(2)

Subtract λk×\lambda_k\times(1) from (2): ∑i=1k−1ci(λi−λk)vi=0.\sum_{i=1}^{k-1}c_i(\lambda_i-\lambda_k)v_i=\mathbf0.

By the inductive hypothesis (applied to v1,…,vk−1v_1,\ldots,v_{k-1} for k−1k-1 distinct eigenvalues): each ci(λi−λk)=0c_i(\lambda_i-\lambda_k)=0. Since λi≠λk\lambda_i\ne\lambda_k, we get ci=0c_i=0 for all i<ki<k. Then (1) gives ckvk=0c_kv_k=\mathbf0, and vk≠0v_k\ne\mathbf0 forces ck=0c_k=0.

  All ci=0; hence v1,…,vk are linearly independent. ■  \boxed{\;\text{All }c_i=0\text{; hence }v_1,\ldots,v_k\text{ are linearly independent.}\ \blacksquare\;}

Common Traps


no-real-eigenvalue (1 question(s); 2022)

Recognition Cues

Solution Template

  1. Write the standard rotation matrix Tθ=(cos⁡θ−sin⁡θsin⁡θcos⁡θ)T_\theta = \bigl(\begin{smallmatrix}\cos\theta&-\sin\theta\\\sin\theta&\cos\theta\end{smallmatrix}\bigr).
  2. Compute the characteristic polynomial p(λ)=λ2−2cos⁡θ λ+1p(\lambda)=\lambda^2-2\cos\theta\,\lambda+1.
  3. Discriminant =4cos⁡2θ−4=−4sin⁡2θ= 4\cos^2\theta-4=-4\sin^2\theta. Real eigenvalues iff sin⁡θ=0\sin\theta=0 (i.e. θ=0\theta=0 or π\pi).
  4. For θ=π/2\theta=\pi/2: p(λ)=λ2+1=0p(\lambda)=\lambda^2+1=0, roots λ=±i\lambda=\pm i. No real solutions.
  5. Geometric conclusion: a 90°90° rotation maps every vector to a perpendicular direction; no non-zero vector can be parallel to its image, so no real eigenvector exists.

Worked Example(s)

2022 Paper 1, 2022-P1-Q4a (15 marks)

Rotation T:R2→R2T:\mathbb R^2\to\mathbb R^2 by angle θ\theta; find the linear map; show Tπ/2T_{\pi/2} has no real eigenvalue.

Linear map. The rotation by θ\theta counter-clockwise acts as: Tθ(x,y)=(xcos⁡θ−ysin⁡θ, xsin⁡θ+ycos⁡θ),Tθ=(cos⁡θ−sin⁡θsin⁡θcos⁡θ).T_\theta(x,y) = (x\cos\theta-y\sin\theta,\ x\sin\theta+y\cos\theta),\qquad T_\theta=\begin{pmatrix}\cos\theta & -\sin\theta\\\sin\theta & \cos\theta\end{pmatrix}.

Linearity: matrix multiplication is linear. Verify: Tθ(1,0)T=(cos⁡θ,sin⁡θ)TT_\theta(1,0)^T=(\cos\theta,\sin\theta)^T ✓.

No real eigenvalue at θ=π/2\theta=\pi/2. Tπ/2=(0−110),p(λ)=λ2+1.T_{\pi/2}=\begin{pmatrix}0&-1\\1&0\end{pmatrix},\qquad p(\lambda)=\lambda^2+1. λ2=−1\lambda^2=-1 has no real solutions.   Tπ/2 has eigenvalues ±i; no real eigenvalue. ■  \boxed{\;T_{\pi/2}\text{ has eigenvalues }\pm i;\text{ no real eigenvalue.}\ \blacksquare\;}

Common Traps


Marks-Aware Writing

8-mark questions (2013-Q2b-i, 2014-Q3c-i, 2016-Q2b-i): Three steps — characteristic polynomial, eigenvalues (with trace/det check), eigenvectors. Write the row-reduction briefly; one sentence per pivot. No lengthy justification.

10–12-mark questions (2021-Q4a-ii, 2025-Q4c-i, 2017-Q3b): For computation: same three steps but show the cubic factorisation explicitly. For proofs: write the induction setup in one sentence, then the two displayed equations and the conclusion.

15-mark questions (2022-Q4a): Two parts — state the matrix (with linearity verified), then the characteristic polynomial and conclusion. Geometric interpretation earns the last method mark.

20-mark questions (2024-Q4a): Full computation for AA, then a short bridge paragraph stating the spectral-inheritance rule, then a table of λ−15\lambda^{-15} values and corresponding eigenvectors. The bridge paragraph is worth 4–6 marks; do not skip it.

Practice Set

YearPaper/QMarksArchetypeOne-line hint
2023P1-Q3a20eigen-computationVerify Cayley–Hamilton: show p(A)=Op(A)=O directly; then use p(A)=0p(A)=0 as a recurrence to express An=An−2+A2−IA^n=A^{n-2}+A^2-I; compute A40A^{40} by grouping even powers
2013P1-Q1b10eigenvalue-boundBoth AA∗AA^* and A∗AA^*A are Hermitian (so real eigenvalues); trace equals ∑iσi2\sum_i\sigma_i^2 for both, which is the same (Frobenius norm ∥A∥F2\|A\|_F^2)
2013P1-Q2c-i8eigenvector-independence-proofHermitian + distinct eigenvalues ⇒ orthogonal eigenvectors ⇒ linearly independent ⇒ det⁡C≠0\det C\ne 0
2021P1-Q3c-i8eigenvector-independence-proofSymmetric: take v2T(Av1)v_2^T(Av_1) two ways; Hermitian symmetry gives λ1(v2Tv1)=λ2(v2Tv1)\lambda_1(v_2^Tv_1)=\lambda_2(v_2^Tv_1); λ1≠λ2\lambda_1\ne\lambda_2 forces v2Tv1=0v_2^Tv_1=0
2017P1-Q1a10eigen-computation2×22\times2 diagonalisation: eigenvalues 1,41,4; eigenvectors (−2,1),(1,1)(-2,1),(1,1); P−1AP=diag(1,4)P^{-1}AP=\text{diag}(1,4)
2016P1-Q1a-ii4eigen-computationShow A3=OA^3=O (nilpotent index 3); then A14=A3⋅4+2=OA^{14}=A^{3\cdot4+2}=O; answer is 3A−2I3A-2I
2016P1-Q2b-ii8no-real-eigenvalueHermitian real eigenvalue proof: form x∗Axx^*Ax; use A∗=AA^*=A to show λ∥x∥2\lambda\|x\|^2 is real

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