Putnam

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Every rule and concept in Putnam, with its definition and a link to the lesson that teaches it. Search by term, by idea, or by lesson title.

Glossary (131)

Absolute versus conditional, and the principal value
∫∣f∣\int |f| convergent implies ∫f\int f convergent.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › Improper Integrals: When They Converge
Bijections before formulas
Pair objects with objects.
Combinatorics & Generating Functions › Counting With Structure
Cauchy's equation and its relatives
f(x+y)=f(x)+f(y)f(x + y) = f(x) + f(y) has only f(x)=cxf(x) = cx on Q\mathbb Q (and on R\mathbb R under any regularity: continuous, monotone, bounded on an interval).
Functional Equations & Recurrences › Solving for Functions
Cayley–Hamilton and minimal polynomials
Every matrix satisfies its own characteristic polynomial: pA(A)=0p_A(A) = 0.
Linear Algebra II: Spectra, Cayley–Hamilton & Finite Fields › Spectral Reasoning
Change variables to match the integrand
With u=x+yu = x + y, v=x−yv = x - y (Jacobian 12\tfrac12), or polar coordinates, or u=xyu = xy, v=y/xv = y/x: choose the substitution that makes the integrand a function of one new variable.
Multivariable Calculus on the Putnam › The Moves That Recur
Choose the extreme, then read off an inequality
Take the object that is largest or smallest in some measure — a minimum label, a closest pair, a point nearest a line.
Extremal Principle and Working Backwards › The Extremal Principle, Worked
Classify states from the end
When a process or game ends in known states, classify every state by working backwards from them: in a game, a position is a loss for the player to move (a P-position) iff every move leads to a win for the opponent (an N-position), and a win iff SOME move l…
Extremal Principle and Working Backwards › Working Backwards, Worked
Closed forms from α+α−1\alpha + \alpha^{-1}
If a0=α+α−1a_0 = \alpha + \alpha^{-1} and an+1=an2−2a_{n+1} = a_n^2 - 2, then an=α2n+α−2na_n = \alpha^{2^n} + \alpha^{-2^n}.
Hard Sequences: Closed Forms, Rates & Periodicity › Sequences the Putnam Actually Sets
Combinatorics and probability
Bijections; PIE; derangements; Catalan and the reflection principle; generating functions and xddxx\tfrac{d}{dx}; Erdős–Szekeres; Mantel/Turán, Hall, Euler; extremal and pigeonhole; games (P/N, Nim, strategy stealing).
Formulas & Methods › Combinatorics, Probability & Geometry
Compactness, and why it is the hypothesis that saves proofs
A closed bounded subset of Rn\mathbb{R}^n is compact; a continuous function on a compact set attains its maximum and minimum, and is uniformly continuous there.
Limits, Continuity & the Big Theorems › Rigor: ε\varepsilon-δ\delta, Uniform Convergence and Compactness
Comparison and limit comparison
If 0≤f≤g0 \le f \le g and ∫g\int g converges, so does ∫f\int f.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › Improper Integrals: When They Converge
Compute, conjecture, prove
Compute the first few cases EXACTLY (fractions, not decimals).
Strategy & Writing a 10 › Small Cases, Then Generalize, Worked
Conditioning and first-step analysis
For expected times and absorption probabilities, condition on the first step: Ei=1+∑jpijEjE_i = 1 + \sum_jp_{ij}E_j — a small linear system.
Probability & Expectation › Expectation Without Distributions
Constant-coefficient linear equations
y′′+py′+qy=0y'' + py' + qy = 0 has solutions erxe^{rx} for the roots rr of r2+pr+q=0r^2 + pr + q = 0 (with xerxxe^{rx} for a double root, and eaxcos⁡bxe^{ax}\cos bx, eaxsin⁡bxe^{ax}\sin bx for r=a±bir = a \pm bi).
Differential Equations on the Putnam › The ODE Toolkit the Exam Assumes
Contradiction with a minimal counterexample
Assume the claim fails; take the SMALLEST failure (smallest nn, shortest sequence, least degree).
Proof Techniques for the Putnam › The Three Forms, at Putnam Level
Convexity and its consequences
A function with f′′≥0f'' \ge 0 lies above its tangent lines and below its chords.
Inequalities & Convexity › The Inequality Toolkit
Coordinates adapted to the integrand
If the integrand depends on xx and yy only through some combinations u(x,y)u(x, y), v(x,y)v(x, y), integrate in u,vu, v: ∬Rf dx dy=∬R′f ∣J∣ du dv\iint_Rf\,dx\,dy = \iint_{R'}f\,|J|\,du\,dv with J=∂(x,y)∂(u,v)J = \dfrac{\partial(x, y)}{\partial(u, v)}.
Multivariable Calculus on the Putnam › Double Integrals by Substitution, Worked
Differentiate the condition, then read off initial values
A condition involving ∫0x\int_0^x or a shifted argument such as f(1−x)f(1 - x) often becomes an ordinary differential equation after one or two differentiations.
Differential Equations on the Putnam › Equations That Hide an ODE
Direct proofs that name their theorems
A direct proof at this level is a chain of cited results: "by the mean value theorem there is c∈(a,b)c \in (a, b) with…", "since the series converges absolutely we may rearrange…".
Proof Techniques for the Putnam › The Three Forms, at Putnam Level
Dirichlet variants by parts
∫0∞sin⁡2xx2dx=∫0∞1−cos⁡xx2dx=π2\int_0^\infty\frac{\sin^2x}{x^2}dx = \int_0^\infty\frac{1 - \cos x}{x^2}dx = \frac\pi2 — one integration by parts each, landing on ∫0∞sin⁡xxdx\int_0^\infty\frac{\sin x}{x}dx.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › More Named Results
Divisor sums and multiplicative functions
τ\tau, σ\sigma, φ\varphi are multiplicative: compute on prime powers and multiply.
Number Theory › Proof-Level Number Theory
Eigenvalues carry every polynomial fact
If AA has eigenvalues λi\lambda_i then p(A)p(A) has eigenvalues p(λi)p(\lambda_i): det⁡(A2+I)=∏(λi2+1)\det(A^2 + I) = \prod(\lambda_i^2 + 1), tr(Ak)=∑λik\mathrm{tr}(A^k) = \sum\lambda_i^k, det⁡eA=etrA\det e^A = e^{\mathrm{tr}A}.
Linear Algebra II: Spectra, Cayley–Hamilton & Finite Fields › Spectral Reasoning
Fresnel, the reflection formula, and Wallis
∫0∞sin⁡(x2)dx=∫0∞cos⁡(x2)dx=12π2\int_0^\infty\sin(x^2)dx = \int_0^\infty\cos(x^2)dx = \frac12\sqrt{\frac\pi2}; Γ(s)Γ(1−s)=πsin⁡πs\Gamma(s)\Gamma(1 - s) = \frac{\pi}{\sin\pi s}; ∏n≥14n24n2−1=π2\prod_{n\ge1}\frac{4n^2}{4n^2 - 1} = \frac\pi2; ∫01ln⁡x1−xdx=−π26\int_0^1\frac{\ln x}{1 - x}dx = -\frac{\pi^2}{6}.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › More Named Results
Frullani's theorem
∫0∞f(ax)−f(bx)x dx=(f(0)−f(∞))ln⁡ba\displaystyle\int_0^\infty\frac{f(ax) - f(bx)}{x}\,dx = \big(f(0) - f(\infty)\big)\ln\frac ba for continuous ff with finite limits at 00 and ∞\infty.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › The Named Integrals
Gamma and Beta
Γ(s)=∫0∞xs−1e−xdx\Gamma(s) = \displaystyle\int_0^\infty x^{s-1}e^{-x}dx, with Γ(n+1)=n!\Gamma(n+1) = n! and Γ(12)=π\Gamma(\tfrac12) = \sqrt\pi.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › The Named Integrals
Geometric probability and random walks
Probability == favorable measure ÷\div total measure; expectations become integrals.
Probability & Expectation › Expectation Without Distributions
Geometry
Pick's theorem; gcd⁡+1\gcd + 1 lattice points on a segment; Minkowski; Gauss circle count πr2+O(r)\pi r^2 + O(r); complex numbers (rotation, collinearity via real ratios, equilateral criterion a+ωb+ω2c=0a + \omega b + \omega^2c = 0); point-to-line/plane distances; convexity …
Formulas & Methods › Combinatorics, Probability & Geometry
Glasser's master theorem
∫−∞∞f ⁣(x−∑iaix−bi)dx=∫−∞∞f(x) dx\displaystyle\int_{-\infty}^\infty f\!\left(x - \sum_{i}\frac{a_i}{x - b_i}\right)dx = \int_{-\infty}^\infty f(x)\,dx for ai>0a_i > 0.
Integrals II: King's Rule, Queen's Rule, and Glasser › Symmetry Substitutions
Green, Stokes and the divergence theorem as identities
A line integral around a closed curve equals a double integral of a curl; the flux of r/∣r∣3\mathbf r/|\mathbf r|^3 through any surface enclosing the origin is 4π4\pi; the area of a region is 12∮(x dy−y dx)\tfrac12\oint(x\,dy - y\,dx).
Multivariable Calculus on the Putnam › The Moves That Recur
Groups and orders
A group is a set with an associative operation, an identity, and inverses.
Abstract Algebra Basics › The Definitions the Putnam Assumes
Identity plus rank one
det⁡(I+uvT)=1+vTu\det(I + \mathbf u\mathbf v^{\mathsf T}) = 1 + \mathbf v^{\mathsf T}\mathbf u (the matrix determinant lemma).
Linear Algebra I: Determinants & Structured Matrices › Determinants the Putnam Way
Inclusion–exclusion and extremal arguments
∣A1∪⋯∪An∣=∑∣Ai∣−∑∣Ai∩Aj∣+⋯|A_1\cup\cdots\cup A_n| = \sum|A_i| - \sum|A_i\cap A_j| + \cdots.
Combinatorics & Generating Functions › Counting With Structure
Induction that is actually strong
When P(n+1)P(n + 1) depends on several earlier cases, assume P(k)P(k) for ALL k≤nk \le n.
Proof Techniques for the Putnam › The Three Forms, at Putnam Level
Inequalities and convexity
AM–GM, Cauchy–Schwarz (sums and integrals), Jensen, rearrangement, power means; Hermite–Hadamard f(a+b2)≤1b−a∫abf≤f(a)+f(b)2f(\tfrac{a+b}{2}) \le \tfrac{1}{b-a}\int_a^bf \le \tfrac{f(a) + f(b)}{2} for convex ff; tangent-line trick; MVT-derived bounds (ex≥1+xe^x \ge 1 + x, $ x ≤ x…
Formulas & Methods › Analysis
Integer polynomials and interpolation
For P∈Z[x]P \in \mathbb Z[x]: a−b∣P(a)−P(b)a - b \mid P(a) - P(b).
Polynomials › Working With Roots You Never Find
IVT, MVT, Rolle, and Taylor with remainder
Continuous ff on [a,b][a,b] takes every value between f(a)f(a) and f(b)f(b).
Limits, Continuity & the Big Theorems › The Theorems That Do the Work
Jump to the other root
For an equation that is quadratic in each variable, fix all but one variable, say xx; if x=ax = a is a root of the quadratic x2−px+q=0x^2 - px + q = 0, so is a′=p−a=qaa' = p - a = \tfrac qa.
Extremal Principle and Working Backwards › Vieta Jumping, Worked
King's rule
∫abf(x) dx=∫abf(a+b−x) dx\displaystyle\int_a^b f(x)\,dx = \int_a^b f(a + b - x)\,dx — reflect the interval onto itself.
Integrals II: King's Rule, Queen's Rule, and Glasser › Symmetry Substitutions
Know the solution without solving
Phase line: for y′=g(y)y' = g(y), a solution never crosses an equilibrium (g(c)=0g(c) = 0), and between equilibria it is monotone.
Differential Equations on the Putnam › Comparison, Phase Lines and Blow-Up
Lagrange multipliers, then check the boundary
To extremize ff on g=cg = c: solve ∇f=λ∇g\nabla f = \lambda\nabla g together with g=cg = c.
Multivariable Calculus on the Putnam › The Moves That Recur
Limits that are derivatives, integrals, or exponentials in disguise
n(21/n−1)→ln⁡2n(2^{1/n} - 1) \to \ln 2 (a derivative); 1n∑f(kn)→∫01f\tfrac1n\sum f(\tfrac kn) \to \int_0^1 f (an integral); (1+an)n→ea(1 + \tfrac an)^n \to e^a (an exponential); (n!)1/nn→1e\tfrac{(n!)^{1/n}}{n} \to \tfrac1e (a log of a Riemann sum).
Limits, Continuity & the Big Theorems › The Theorems That Do the Work
Limits, series, integrals
Limits as derivatives (n(a1/n−1)→ln⁡an(a^{1/n} - 1) \to \ln a), as Riemann sums (1n∑f(kn)→∫01f\tfrac1n\sum f(\tfrac kn) \to \int_0^1f), as exponentials ((1+an)n→ea(1 + \tfrac an)^n \to e^a); Stolz–Cesàro; Taylor with Lagrange remainder; the three series (∑xn\sum x^n, ∑xnn\sum\tfrac{x^n}{n},…
Formulas & Methods › Analysis
Linear algebra
Matrix determinant lemma det⁡(I+uvT)=1+vTu\det(I + \mathbf u\mathbf v^{\mathsf T}) = 1 + \mathbf v^{\mathsf T}\mathbf u and det⁡(aI+bJ)=an−1(a+nb)\det(aI + bJ) = a^{n-1}(a + nb); Vandermonde ∏i<j(xj−xi)\prod_{i<j}(x_j - x_i); circulant eigenvalues by DFT; tridiagonal Toeplitz eigenvalues $a + 2b\…
Formulas & Methods › Algebra
Linearity and indicators
E[∑Xi]=∑E[Xi]E[\sum X_i] = \sum E[X_i] with NO independence assumption.
Probability & Expectation › Expectation Without Distributions
Log-trig integrals and the tangent bridge
∫0π/2ln⁡cos⁡x dx=−π2ln⁡2\int_0^{\pi/2}\ln\cos x\,dx = -\frac\pi2\ln 2, hence ∫0∞ln⁡(1+x2)1+x2dx=πln⁡2\int_0^\infty\frac{\ln(1 + x^2)}{1 + x^2}dx = \pi\ln 2 (substitute x=tan⁡θx = \tan\theta) and ∫0π/2ln⁡tan⁡x dx=0\int_0^{\pi/2}\ln\tan x\,dx = 0.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › More Named Results
Maps of finite order and periodic sequences
x↦11−xx \mapsto \tfrac{1}{1-x} has order 33; x↦1+x1−xx \mapsto \tfrac{1+x}{1-x} has order 44; x↦x+1x−1x \mapsto \tfrac{x+1}{x-1} is an involution.
Hard Sequences: Closed Forms, Rates & Periodicity › Sequences the Putnam Actually Sets
Matrices over finite fields: count
∣GLn(Fq)∣=(qn−1)(qn−q)⋯(qn−qn−1)|GL_n(\mathbb F_q)| = (q^n - 1)(q^n - q)\cdots(q^n - q^{n-1}) — pick columns one at a time, each outside the span of the previous.
Linear Algebra II: Spectra, Cayley–Hamilton & Finite Fields › Spectral Reasoning
Monovariants
A quantity that always DEcreases (or increases) and is bounded proves that a process terminates, and — if it is an integer — how many steps at most.
Invariance and Symmetry › Finding the Invariant
Orders, primitive roots, and CRT
The order of aa mod nn divides every kk with ak≡1a^k \equiv 1, hence divides φ(n)\varphi(n).
Number Theory › Proof-Level Number Theory
Pair, cancel, mirror
A symmetry of the problem — swapping players, swapping heads and tails, reflecting through a point, x↦a+b−xx \mapsto a + b - x — maps outcomes to outcomes.
Invariance and Symmetry › Symmetry Arguments, Worked
Parity, sums mod kk, and colorings
For a process (a game, an operation repeated on a board or a set), compute a quantity after each move: the parity of a count, a sum modulo kk, a weighted sum, a determinant, a product of signs.
Invariance and Symmetry › Finding the Invariant
Periodicity, involutions, and iteration
Compose the function with itself; find the order.
Functional Equations & Recurrences › Solving for Functions
Pick the extreme object
Among finitely many objects, choose the one maximizing or minimizing something — the largest number, the point farthest from a line, the longest chain, the polynomial of least degree.
Extremal Principle and Working Backwards › The Extremal Principle
Pointwise versus uniform convergence
Pointwise: for each xx, fn(x)→f(x)f_n(x) \to f(x).
Limits, Continuity & the Big Theorems › Rigor: ε\varepsilon-δ\delta, Uniform Convergence and Compactness
Polynomials, number theory, abstract algebra
Vieta and Newton; roots of unity filter; auxiliary polynomial with known roots for values at integers; Chebyshev; Eisenstein; a−b∣P(a)−P(b)a - b \mid P(a) - P(b).
Formulas & Methods › Algebra
Proof: (n!)1/nn→1e\frac{(n!)^{1/n}}{n} \to \frac1e
A limit that looks like it needs Stirling and does not.
Limits, Continuity & the Big Theorems › Proofs & Why It Matters
Proof: Γ(12)=π\Gamma(\tfrac12) = \sqrt\pi and the Gaussian integral
Two famous constants, one computation.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › Proofs & Why It Matters
Proof: ∫0∞e−txsin⁡x dx=11+t2\int_0^\infty e^{-tx}\sin x\,dx = \frac{1}{1+t^2}
The Laplace transform that powers the Dirichlet integral.
Integrals I: Feynman's Trick › Proofs & Why It Matters
Proof: ∫0∞sin⁡2xx2dx=π2\int_0^\infty\frac{\sin^2x}{x^2}dx = \frac\pi2
Parts onto Dirichlet.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › Proofs & Why It Matters
Proof: tr⁡Ak=0\operatorname{tr}A^k = 0 for k=1,…,nk = 1, \ldots, n forces AA nilpotent
If an n×nn\times n complex matrix has tr⁡Ak=0\operatorname{tr}A^k = 0 for all 1≤k≤n1 \le k \le n, then every eigenvalue is 00.
Linear Algebra II: Spectra, Cayley–Hamilton & Finite Fields › Proofs & Why It Matters
Proof: ∑d∣nφ(d)=n\sum_{d\mid n}\varphi(d) = n
A one-line counting proof of a multiplicative identity.
Number Theory › Proofs & Why It Matters
Proof: ζ(2)=π26\zeta(2) = \frac{\pi^2}{6} via a double integral
The Basel problem, by a route the Putnam would accept.
Sequences & Series › Proofs & Why It Matters
Proof: a polynomial over a field has at most deg⁡\deg roots
The property that separates fields from rings like Z/8\mathbb Z/8.
Abstract Algebra Basics › Proofs & Why It Matters
Proof: an increasing involution is the identity
If ff is strictly increasing and f(f(x))=xf(f(x)) = x for all xx, then f(x)=xf(x) = x.
Functional Equations & Recurrences › Proofs & Why It Matters
Proof: blow-up for y′≥y2y' \ge y^2
If yy is differentiable with y′≥y2y' \ge y^2 and y(0)=c>0y(0) = c > 0, then yy cannot exist on [0,1/c][0, 1/c].
Differential Equations on the Putnam › Proofs & Why It Matters
Proof: Cauchy–Schwarz by a quadratic
For real vectors a,b\mathbf a, \mathbf b: (a⋅b)2≤∣a∣2∣b∣2(\mathbf a\cdot\mathbf b)^2 \le |\mathbf a|^2|\mathbf b|^2.
Inequalities & Convexity › Proofs & Why It Matters
Proof: Cauchy's equation on Q\mathbb Q
If f(x+y)=f(x)+f(y)f(x + y) = f(x) + f(y) for all rationals, then f(x)=cxf(x) = cx with c=f(1)c = f(1).
Functional Equations & Recurrences › Proofs & Why It Matters
Proof: Cayley–Hamilton via the adjugate
Every square matrix satisfies its own characteristic polynomial: pA(A)=0p_A(A) = 0.
Linear Algebra II: Spectra, Cayley–Hamilton & Finite Fields › Proofs & Why It Matters
Proof: Erdős–Szekeres
Any sequence of n2+1n^2 + 1 distinct reals has a monotone subsequence of length n+1n + 1.
Combinatorics & Generating Functions › Proofs & Why It Matters
Proof: Frullani's theorem
Assume ff continuous with f(0)f(0), f(∞)f(\infty) finite and 0<a<b0 < a < b.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › Proofs & Why It Matters
Proof: Glasser's theorem in the simplest case
Show ∫−∞∞f ⁣(x−1x)dx=∫−∞∞f(u) du\displaystyle\int_{-\infty}^\infty f\!\left(x - \tfrac1x\right)dx = \int_{-\infty}^\infty f(u)\,du.
Integrals II: King's Rule, Queen's Rule, and Glasser › Proofs & Why It Matters
Proof: Grönwall's inequality
If u′(x)≤βu(x)u'(x) \le \beta u(x) on [0,T][0, T] with u(0)=u0u(0) = u_0, then u(x)≤u0eβxu(x) \le u_0e^{\beta x}.
Differential Equations on the Putnam › Proofs & Why It Matters
Proof: Jensen's inequality
For convex ff and weights wi≥0w_i \ge 0 summing to 11: f(∑wixi)≤∑wif(xi)f(\sum w_ix_i) \le \sum w_if(x_i).
Inequalities & Convexity › Proofs & Why It Matters
Proof: Lagrange's theorem
For a subgroup HH of a finite group GG, ∣H∣|H| divides ∣G∣|G|.
Abstract Algebra Basics › Proofs & Why It Matters
Proof: lifting the exponent (odd prime case)
For odd prime pp with p∣a−bp \mid a - b and p∤abp \nmid ab: vp(an−bn)=vp(a−b)+vp(n)v_p(a^n - b^n) = v_p(a - b) + v_p(n).
Number Theory › Proofs & Why It Matters
Proof: linearity of expectation
E[X+Y]=E[X]+E[Y]E[X + Y] = E[X] + E[Y] for ANY random variables with finite expectations.
Probability & Expectation › Proofs & Why It Matters
Proof: Newton's identity for p2p_2 and the general pattern
p2=e12−2e2p_2 = e_1^2 - 2e_2, and in general pk−e1pk−1+e2pk−2−⋯+(−1)kkek=0p_k - e_1p_{k-1} + e_2p_{k-2} - \cdots + (-1)^kke_k = 0.
Polynomials › Proofs & Why It Matters
Proof: Stolz–Cesàro
If bnb_n is strictly increasing to ∞\infty and an+1−anbn+1−bn→L\tfrac{a_{n+1} - a_n}{b_{n+1} - b_n} \to L, then anbn→L\tfrac{a_n}{b_n} \to L.
Sequences & Series › Proofs & Why It Matters
Proof: Stolz–Cesàro
If bnb_n is strictly increasing with bn→∞b_n \to \infty and an+1−anbn+1−bn→L\tfrac{a_{n+1} - a_n}{b_{n+1} - b_n} \to L, then anbn→L\tfrac{a_n}{b_n} \to L.
Hard Sequences: Closed Forms, Rates & Periodicity › Proofs & Why It Matters
Proof: the Catalan reflection
Lattice paths from (0,0)(0,0) to (n,n)(n,n) never rising above y=xy = x number 1n+1(2nn)\tfrac{1}{n+1}\binom{2n}{n}.
Combinatorics & Generating Functions › Proofs & Why It Matters
Proof: the coupon collector expectation
Collecting all nn equally likely coupons takes nHnnH_n draws on average.
Probability & Expectation › Proofs & Why It Matters
Proof: the Leibniz rule
If ff and ∂af\partial_af are continuous on [c,d]×[a0,a1][c,d]\times[a_0, a_1], then dda∫cdf(x,a) dx=∫cd∂af(x,a) dx\dfrac{d}{da}\int_c^d f(x,a)\,dx = \int_c^d\partial_af(x,a)\,dx.
Integrals I: Feynman's Trick › Proofs & Why It Matters
Proof: the log-sine integral
Show ∫0π/2ln⁡(sin⁡x) dx=−π2ln⁡2\displaystyle\int_0^{\pi/2}\ln(\sin x)\,dx = -\frac\pi2\ln 2 using only King and Queen.
Integrals II: King's Rule, Queen's Rule, and Glasser › Proofs & Why It Matters
Proof: the matrix determinant lemma
det⁡(I+uvT)=1+vTu\det(I + \mathbf u\mathbf v^{\mathsf T}) = 1 + \mathbf v^{\mathsf T}\mathbf u, and more generally det⁡(A+uvT)=det⁡A (1+vTA−1u)\det(A + \mathbf u\mathbf v^{\mathsf T}) = \det A\,(1 + \mathbf v^{\mathsf T}A^{-1}\mathbf u) for invertible AA.
Linear Algebra I: Determinants & Structured Matrices › Proofs & Why It Matters
Proof: the mean value theorem from Rolle
Rolle: if ff is continuous on [a,b][a,b], differentiable on (a,b)(a,b), and f(a)=f(b)f(a) = f(b), then f′(c)=0f'(c) = 0 for some cc.
Limits, Continuity & the Big Theorems › Proofs & Why It Matters
Proof: the roots-of-unity filter
For P(x)=∑akxkP(x) = \sum a_kx^k and ω=e2πi/n\omega = e^{2\pi i/n}: ∑n∣kak=1n∑j=0n−1P(ωj)\sum_{n\mid k}a_k = \tfrac1n\sum_{j=0}^{n-1}P(\omega^j).
Polynomials › Proofs & Why It Matters
Proof: the spectral theorem for real symmetric matrices
A real symmetric matrix has real eigenvalues and an orthonormal basis of eigenvectors.
Linear Algebra II: Spectra, Cayley–Hamilton & Finite Fields › Proofs & Why It Matters
Proof: the tridiagonal recurrence and its eigenvalues
For TnT_n with aa on the diagonal and b,cb, c on the off-diagonals, det⁡Tn=adet⁡Tn−1−bcdet⁡Tn−2\det T_n = a\det T_{n-1} - bc\det T_{n-2}; the eigenvalues of the symmetric case (b=cb = c) are a+2bcos⁡kπn+1a + 2b\cos\frac{k\pi}{n+1}, k=1,…,nk = 1, \ldots, n.
Linear Algebra I: Determinants & Structured Matrices › Proofs & Why It Matters
Proof: the Vandermonde determinant
det⁡[xi j−1]i,j=1n=∏1≤i<j≤n(xj−xi)\det\big[x_i^{\,j-1}\big]_{i,j=1}^n = \prod_{1\le i<j\le n}(x_j - x_i).
Linear Algebra I: Determinants & Structured Matrices › Proofs & Why It Matters
Prove more, so that the step closes
If the step P(n)⇒P(n+1)P(n) \Rightarrow P(n+1) will not go through, look for a STRONGER statement Q(n)Q(n) — one that implies P(n)P(n) — whose own step does go through.
Proof Techniques for the Putnam › Strengthening the Induction Hypothesis
Queen's rule and Jack's rule
∫02af=2∫0af\displaystyle\int_0^{2a} f = 2\int_0^a f if f(2a−x)=f(x)f(2a - x) = f(x), and =0= 0 if f(2a−x)=−f(x)f(2a - x) = -f(x).
Integrals II: King's Rule, Queen's Rule, and Glasser › Symmetry Substitutions
Recurrences and generating functions
Set up ana_n by the first choice; solve by characteristic equation or by the generating function A(x)=∑anxnA(x) = \sum a_nx^n, which turns the recurrence into algebra.
Combinatorics & Generating Functions › Counting With Structure
Recurring Putnam groups
Symmetric groups SnS_n (permutations, cycle structure, parity), matrix groups GLn(Fq)GL_n(\mathbb F_q), units mod nn, dihedral groups, and "the set of all maps satisfying …" that turns out to be a group.
Abstract Algebra Basics › The Definitions the Putnam Assumes
Rings, fields, and polynomials over them
A field has division by nonzero elements; Fp=Z/p\mathbb F_p = \mathbb Z/p and its extensions Fpk\mathbb F_{p^k} are the finite ones.
Abstract Algebra Basics › The Definitions the Putnam Assumes
Roots of unity and the filter
∑k=0n−1ωjk=n\sum_{k=0}^{n-1}\omega^{jk} = n if n∣jn \mid j, else 00.
Polynomials › Working With Roots You Never Find
Sentences graders reward
"We proceed by strong induction on nn." "Suppose for contradiction that no such xx exists; let n0n_0 be the least…" "By the intermediate value theorem applied to the continuous function gg on [0,1][0, 1]…" "The case n=1n = 1 holds since…"
Proof Techniques for the Putnam › The Three Forms, at Putnam Level
Separable and first-order linear equations
Separable: y′=f(x)g(y)⇒∫dyg(y)=∫f(x)dxy' = f(x)g(y) \Rightarrow \int\tfrac{dy}{g(y)} = \int f(x)dx.
Differential Equations on the Putnam › The ODE Toolkit the Exam Assumes
Small cases, then generalize
Compute n=1,2,3n = 1, 2, 3.
Strategy & Writing a 10 › How to Take the Exam
Stolz–Cesàro and Riemann sums
If bn↑∞b_n \uparrow \infty and an+1−anbn+1−bn→L\dfrac{a_{n+1} - a_n}{b_{n+1} - b_n} \to L, then anbn→L\dfrac{a_n}{b_n} \to L.
Sequences & Series › Summing and Testing
Symmetrize before integrating
Over a region symmetric under x↔yx \leftrightarrow y, ∬f(x,y)=∬f(y,x)\iint f(x, y) = \iint f(y, x); average the two.
Multivariable Calculus on the Putnam › The Moves That Recur
Symmetry that solves the problem
If the problem is invariant under a transformation (swapping variables, x→1−xx \to 1 - x, rotation of a configuration), the answer or the extremal configuration is often invariant too — or the transformation pairs up terms that cancel.
Invariance and Symmetry › Finding the Invariant
Tangency, then compare the candidates
At an extremum of ff on the curve (or surface) g=cg = c, at a point where ∇g≠0\nabla g \ne 0: ∇f=λ∇g\nabla f = \lambda\nabla g for some λ\lambda.
Multivariable Calculus on the Putnam › Constrained Extrema, Worked
Telescoping and partial fractions
Write the term as g(n)−g(n+1)g(n) - g(n+1) (or a lagged version) and watch everything cancel except the ends.
Sequences & Series › Summing and Testing
Termination by a monovariant
If every move strictly increases (or decreases) a quantity MM, and MM can take only finitely many values — or values in a set with no infinite decreasing chain, such as the nonnegative integers — then the process stops.
Invariance and Symmetry › Monovariants, Worked
The core four
AM–GM: ∑ain≥∏ain\tfrac{\sum a_i}{n} \ge \sqrt[n]{\prod a_i}.
Inequalities & Convexity › The Inequality Toolkit
The first move in each pool
Linear algebra: row operations before any formula.
Everything the Putnam Tests › One Problem From Each Pool
The invariant method
Find a quantity II with I(after)=I(before)I(\text{after}) = I(\text{before}) for EVERY allowed move.
Invariance and Symmetry › Invariants, Worked
The map of this course
Topics 2–4 are the integrals.
Everything the Putnam Tests › The Syllabus, Honestly
The method in one line
Embed the integral in a family I(a)=∫f(x,a) dxI(a) = \int f(x, a)\,dx, differentiate in the parameter, integrate back, and fix the constant from a value of aa where I(a)I(a) is known.
Integrals I: Feynman's Trick › Differentiating Under the Integral
The named integrals
Feynman: I′(a)=∫∂afI'(a) = \int\partial_af; Dirichlet ∫0∞sin⁡xx=π2\int_0^\infty\tfrac{\sin x}{x} = \tfrac\pi2 and ∫0∞sin⁡2xx2=π2\int_0^\infty\tfrac{\sin^2x}{x^2} = \tfrac\pi2; Gaussian ∫e−x2=π\int e^{-x^2} = \sqrt\pi and ∫0∞e−x2cos⁡2bx=π2e−b2\int_0^\infty e^{-x^2}\cos 2bx = \tfrac{\sqrt\pi}{2}e^{-b^2}; King $\…
Formulas & Methods › Analysis
The six pools
ANALYSIS · LINEAR ALGEBRA · ALGEBRA & POLYNOMIALS · NUMBER THEORY · COMBINATORICS & PROBABILITY · GEOMETRY.
Everything the Putnam Tests › The Syllabus, Honestly
The squaring and reciprocal tricks
For an+1=an+1ana_{n+1} = a_n + \tfrac{1}{a_n}, square: an+12=an2+2+an−2a_{n+1}^2 = a_n^2 + 2 + a_n^{-2}, so an2≈2na_n^2 \approx 2n.
Hard Sequences: Closed Forms, Rates & Periodicity › Sequences the Putnam Actually Sets
The substitution playbook
Plug in 00, 11, −x-x, 1x\tfrac1x, 1−x1 - x, y=xy = x; use the equation to build a second equation, then eliminate.
Functional Equations & Recurrences › Solving for Functions
The three series to know by sight
∑n≥0xn=11−x\displaystyle\sum_{n\ge0}x^n = \frac{1}{1-x}, ∑n≥1xnn=−ln⁡(1−x)\quad\sum_{n\ge1}\frac{x^n}{n} = -\ln(1-x), ∑n≥0xnn!=ex\quad\sum_{n\ge0}\frac{x^n}{n!} = e^x — and everything you get by differentiating or integrating them.
Sequences & Series › Summing and Testing
The universal problem-solving loop
Read twice.
Formulas & Methods › Combinatorics, Probability & Geometry
The words of the question are a contract
"Find all" means: every answer you list works, AND nothing else does.
Everything the Putnam Tests › Reading the Problem: What the Question Commits You To
Triage in the first ten minutes
Read all six problems.
Strategy & Writing a 10 › How to Take the Exam
Two kinds of improper, and the rule for both
An integral is improper at an infinite endpoint or at a point where the integrand blows up.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › Improper Integrals: When They Converge
Two ways to say "there exists"
Either CONSTRUCT the object, or TRAP it: the intermediate value theorem (a continuous function that is ≤0\le 0 at one point and ≥0\ge 0 at another vanishes between them), the pigeonhole principle (n+1n + 1 objects in nn boxes), or averaging (some term is at…
Proof Techniques for the Putnam › Existence: Construct It or Trap It
Uniqueness by integrating factor, and Grönwall
If f′=ff' = f then (fe−x)′=0(fe^{-x})' = 0, so f=Cexf = Ce^x.
Differential Equations on the Putnam › The ODE Toolkit the Exam Assumes
Valuations: Legendre, Kummer, LTE
vp(n!)=∑k≥1⌊n/pk⌋v_p(n!) = \sum_{k\ge1}\lfloor n/p^k\rfloor; vp(nk)v_p\binom{n}{k} is the number of carries adding k+(n−k)k + (n-k) in base pp; vp(an−bn)=vp(a−b)+vp(n)v_p(a^n - b^n) = v_p(a - b) + v_p(n) for odd p∣a−bp \mid a - b.
Number Theory › Proof-Level Number Theory
Vandermonde, circulant, tridiagonal
Vandermonde: det⁡[xij−1]=∏i<j(xj−xi)\det[x_i^{j-1}] = \prod_{i<j}(x_j - x_i).
Linear Algebra I: Determinants & Structured Matrices › Determinants the Putnam Way
Vieta and Newton's identities
For xn−e1xn−1+e2xn−2−⋯x^n - e_1x^{n-1} + e_2x^{n-2} - \cdots, the eke_k are the elementary symmetric functions of the roots, and the power sums obey pk=e1pk−1−e2pk−2+⋯±kekp_k = e_1p_{k-1} - e_2p_{k-2} + \cdots \pm ke_k.
Polynomials › Working With Roots You Never Find
Vieta jumping
For an equation quadratic in each variable, take a solution with minimal x+yx + y; Vieta gives a second root, producing a smaller solution unless the minimal one is a fixed base case.
Extremal Principle and Working Backwards › The Extremal Principle
Weierstrass substitution and series expansion
t=tan⁡x2t = \tan\tfrac x2 rationalizes any ∫R(sin⁡x,cos⁡x) dx\int R(\sin x, \cos x)\,dx.
Integrals III: Frullani, Beta, Gamma, Weierstrass & Series › The Named Integrals
Well-ordering as a proof engine
To prove a statement about objects measured by a nonnegative integer (a number, a degree, a sum ∣x∣+∣y∣+∣z∣|x| + |y| + |z|), assume a counterexample exists and take one with the SMALLEST measure.
Proof Techniques for the Putnam › Minimal Counterexamples, Worked
What a 10 looks like
A complete argument with every nontrivial step justified, edge cases handled, and the conclusion stated.
Strategy & Writing a 10 › How to Take the Exam
What a grader checks
A 10-point solution states what it proves, names every theorem it uses at the moment it uses it, checks that theorem's hypotheses, justifies every interchange of limits, handles every case (including boundary points and small nn), and ends with the conclus…
Strategy & Writing a 10 › A 10 and a 2: Writing It Up
What an ε\varepsilon-δ\delta proof must contain
Given ε>0\varepsilon > 0, EXHIBIT a δ>0\delta > 0 (or an NN) and show the required inequality for every point within δ\delta (or every index past NN).
Limits, Continuity & the Big Theorems › Rigor: ε\varepsilon-δ\delta, Uniform Convergence and Compactness
What the exam is
Twelve problems, two three-hour sessions of six, each scored 00–1010.
Everything the Putnam Tests › The Syllabus, Honestly
Working backwards
Start from what you want and ask what would suffice.
Extremal Principle and Working Backwards › The Extremal Principle