The math optional, made finite. Daily Practice

Eigenvalues and eigenvectors

At a Glance

Why This Chapter Matters

Eigenvalues and eigenvectors appear in 9 of the last 13 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 A15A^{-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(AλI)=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 dimker(AλI)=nrank(AλI)\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=(cosθsinθsinθcosθ)T_\theta=\bigl(\begin{smallmatrix}\cos\theta&-\sin\theta\\\sin\theta&\cos\theta\end{smallmatrix}\bigr) has characteristic polynomial λ22cosθλ+1\lambda^2-2\cos\theta\,\lambda+1. Discriminant =4cos2θ4=4sin2θ0= 4\cos^2\theta-4 = -4\sin^2\theta \le 0; real eigenvalues only when sinθ=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 AkA^{-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(AλI)\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 (AλI)(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 AkA^{-k}: state “eigenvectors of AA and AkA^{-k} are identical; eigenvalues of AkA^{-k} are λk\lambda^{-k}.” Do not re-compute.

Worked Example(s)

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

A=(223216120)A=\bigl(\begin{smallmatrix}-2&2&-3\\2&1&-6\\-1&-2&0\end{smallmatrix}\bigr). Find eigenvalues and eigenvectors.

Characteristic polynomial. Expanding det(AλI)\det(A-\lambda I) along row 1: p(λ)=(λ+3)[(λ+2)(λ4)+7]=(λ+3)(λ+3)(λ5)(1)p(\lambda) = (\lambda+3)[-(\lambda+2)(\lambda-4)+7] = (\lambda+3)(\lambda+3)(\lambda-5) \cdot (-1) p(λ)=(λ+3)2(λ5).\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 A5IA-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+2y3z=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 =59=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+7λ236=0    λ37λ2+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: 828+36=0-8-28+36=0 ✓. Factor: (λ+2)(λ3)(λ6)=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): v1v2=0v_1\cdot v_2=0, v1v3=0v_1\cdot v_3=0, v2v3=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)=[(1λ)21](1λ)=λ(λ2)(1λ).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=(0ii0)A=\bigl(\begin{smallmatrix}0&-i\\i&0\end{smallmatrix}\bigr) over C\mathbb C. Find eigenvalues and eigenvectors.

Characteristic polynomial. det(AλI)=λ2(i)(i)=λ21\det(A-\lambda I)=\lambda^2-(-i)(i)=\lambda^2-1 (since ii=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: v1iv2=0v1=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: v1iv2=0v_1-iv_2=0; v2=(i,1)Tv_2=(i,1)^T.

Verify: A(1,i)T=(ii,i1)T=(1,i)TA(1,i)^T=(-i\cdot i,\,i\cdot 1)^T=(1,i)^T ✓. Orthogonality: (1,i)(i,1)T=ii=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 A15A^{-15}.

Characteristic polynomial. Expanding det(AλI)\det(A-\lambda I): λ36λ215λ8=0    (λ+1)2(λ8)=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=811=6=8-1-1 ✓; det =8=811=8=8\cdot1\cdot1 ✓.

Eigenvectors. For λ=8\lambda=8: row-reduce A8IA-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 A15A^{-15}. Eigenvectors are unchanged. Eigenvalues become λ15\lambda^{-15}: 815=2458^{-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 245 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=(120216223)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+9λ45=0    λ35λ29λ+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(λ5)9(λ5)=(λ5)(λ29)=(λ5)(λ3)(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 AAA^*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 AA=cIA^*A = cI (scalar matrix); singular values of AA are all c\sqrt c.
  3. For A2A^2: (A2)(A2)=AAAA=A(cI)A=cAA=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 (AA=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 ncKnc \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), ω1\omega\ne1, ω3=1\omega^3=1. Show λ1+λ2+λ39|\lambda_1|+|\lambda_2|+|\lambda_3|\le 9.

Compute AAA^*A. Note AA is symmetric so A=AA^* = \overline A. The (i,j)(i,j)-entry of AA\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: AA=3I.A^*A = 3I.

Singular values of A2A^2. (A2)(A2)=A(AA)A=A(3I)A=3AA=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 AA=AAA^*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=99. |\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 k1k-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=1k1ci(λiλk)vi=0\sum_{i=1}^{k-1}c_i(\lambda_i-\lambda_k)v_i=\mathbf0.
  4. By hypothesis, ci(λiλk)=0c_i(\lambda_i-\lambda_k)=0 for i<ki<k. Since λiλk\lambda_i\ne\lambda_k, we get ci=0c_i=0 for i<ki<k. Then ckvk=0c_kv_k=\mathbf0 and vk0v_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=1k1ci(λiλk)vi=0.\sum_{i=1}^{k-1}c_i(\lambda_i-\lambda_k)v_i=\mathbf0.

By the inductive hypothesis (applied to v1,,vk1v_1,\ldots,v_{k-1} for k1k-1 distinct eigenvalues): each ci(λiλk)=0c_i(\lambda_i-\lambda_k)=0. Since λiλk\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 vk0v_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=(cosθsinθsinθcosθ)T_\theta = \bigl(\begin{smallmatrix}\cos\theta&-\sin\theta\\\sin\theta&\cos\theta\end{smallmatrix}\bigr).
  2. Compute the characteristic polynomial p(λ)=λ22cosθλ+1p(\lambda)=\lambda^2-2\cos\theta\,\lambda+1.
  3. Discriminant =4cos2θ4=4sin2θ= 4\cos^2\theta-4=-4\sin^2\theta. Real eigenvalues iff sinθ=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:R2R2T:\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)=(xcosθysinθ, xsinθ+ycosθ),Tθ=(cosθsinθsinθcosθ).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=(cosθ,sinθ)TT_\theta(1,0)^T=(\cos\theta,\sin\theta)^T ✓.

No real eigenvalue at θ=π/2\theta=\pi/2. Tπ/2=(0110),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 λ15\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=An2+A2IA^n=A^{n-2}+A^2-I; compute A40A^{40} by grouping even powers
2013P1-Q1b10eigenvalue-boundBoth AAAA^* and AAA^*A are Hermitian (so real eigenvalues); trace equals iσi2\sum_i\sigma_i^2 for both, which is the same (Frobenius norm AF2\|A\|_F^2)
2013P1-Q2c-i8eigenvector-independence-proofHermitian + distinct eigenvalues ⇒ orthogonal eigenvectors ⇒ linearly independent ⇒ detC0\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); λ1λ2\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); P1AP=diag(1,4)P^{-1}AP=\text{diag}(1,4)
2016P1-Q1a-ii4eigen-computationShow A3=OA^3=O (nilpotent index 3); then A14=A34+2=OA^{14}=A^{3\cdot4+2}=O; answer is 3A2I3A-2I
2016P1-Q2b-ii8no-real-eigenvalueHermitian real eigenvalue proof: form xAxx^*Ax; use A=AA^*=A to show λx2\lambda\|x\|^2 is real

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