Survey of Mathematics

Dictionary

Every definition and theorem in the book, A to Z. Each entry gives the idea in one line and links to where it is taught, with its picture and its proof.

A
A and A-transpose A have the same null space Lemma
ATAx=OA^{\mathsf T}Ax = O exactly when Ax=OAx = O.
Vol. 2, 2.10 Least squares and regression as projection
A closed set contains its limit points Theorem
A set AA is closed if and only if every limit point of AA belongs to AA.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
A connected subset lies on one side of a separation Lemma
If Z=P∪QZ = P \cup Q is a separation and C⊆ZC \subseteq Z is connected, then C⊆PC \subseteq P or C⊆QC \subseteq Q.
Vol. 2, 4.4 Connectedness and path-connectedness
A continuous bijection from a compact space is a homeomorphism Proposition
If KK is compact and f:K→Yf : K \to Y is a continuous bijection onto a metric space, then f−1f^{-1} is continuous, so ff is a homeomorphism.
Vol. 2, 4.5 Continuity between metric spaces
A continuous function with zero integral over every region is zero Lemma
If hh is continuous on an open set and ∭Eh dV=0\iiint_Eh\,dV = 0 for every ball EE inside it, then h=0h = 0 everywhere.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
A convex Lagrangian gives a global minimum Corollary
If x↦L(x,λ)=f(x)−∑λi(gi(x)−ci)x \mapsto L(x, \lambda) = f(x) - \sum\lambda_i(g_i(x) - c_i) is convex and aa satisfies ∇f(a)=∑λi∇gi(a)\nabla f(a) = \sum\lambda_i\nabla g_i(a) and g(a)=cg(a) = c, then aa is an absolute minimum of ff on {g=c}\{g = c\}.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
A field has a limit exactly when its components do Theorem
F(x)→bF(x) \to b as x→ax \to a if and only if Fk(x)→bkF_k(x) \to b_k for every component kk.
Vol. 2, 5.1 Scalar and vector fields, limits and continuity
A field has no zero divisors Lemma
In a field, ab = 0 implies a = 0 or b = 0.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
A function is a bijection from its classes onto its range Theorem
For f:A→Bf: A \to B with a∼ba \sim b iff f(a)=f(b)f(a) = f(b), the rule [a]↦f(a)[a] \mapsto f(a) is a well-defined bijection from A/∼A / {\sim} onto the range f(A)f(A).
Vol. 2, 0.4 Equivalence relations and partitions
A higher-order equation is a first-order system Fact
Put x=(y,y′,…,y(n−1))x = (y, y', \dots, y^{(n-1)}). Then y(n)=f(t,y,…,y(n−1))y^{(n)} = f(t, y, \dots, y^{(n-1)}) is the same as x′=F(t,x)x' = F(t, x) for a vector function FF.
Vol. 2, 7.1 Existence and uniqueness for differential equations
A left inverse is unique and two-sided Theorem
A function has at most one left inverse, and a left inverse is also a right inverse.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
A left inverse of a square matrix is a full inverse Theorem
If AA and BB are n×nn \times n and BA=IBA = I, then AB=IAB = I too, so B=A−1B = A^{-1}.
Vol. 2, 2.6 Systems of equations and elimination
A limit forces the same value along every path Theorem
If F(x)→bF(x) \to b as x→ax \to a and a path r(t)→ar(t) \to a with r(t)≠ar(t) \ne a, then F(r(t))→bF(r(t)) \to b along the path.
Vol. 2, 5.1 Scalar and vector fields, limits and continuity
A linear differential operator is a linear map Fact
L(f+g)=Lf+LgL(f + g) = Lf + Lg and L(cf)=c LfL(cf) = c\,Lf, so the solutions of Ly=0Ly = 0 form the null space of a linear map.
Vol. 2, 7.2 Linear differential equations
A local minimum needs a positive semidefinite Hessian Corollary
If a C2C^2 field has a local minimum at a critical point aa, then every eigenvalue of Hf(a)H_f(a) is at least 00; if it has a local maximum, every eigenvalue is at most 00.
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
A matrix is invertible exactly when its determinant is non-zero Theorem
For a square matrix, det⁡A≠0\det A \ne 0 if and only if AA is invertible, if and only if the rows are independent, if and only if the columns are independent.
Vol. 2, 2.7 Determinants
A non-zero Wronskian proves independence Theorem
If W(f1,…,fn)(t0)≠0W(f_1, \dots, f_n)(t_0) \ne 0 at even one point t0t_0 of JJ, then f1,…,fnf_1, \dots, f_n are linearly independent on JJ.
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
A norm gives a metric Theorem
If ∥⋅∥\lVert \cdot \rVert is a norm on VV, then d(x,y)=∥x−y∥d(x, y) = \lVert x - y \rVert is a metric on VV.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
A passive circuit loses energy Fact
With no source, the stored energy W=12LI2+q22CW = \frac12LI^2 + \frac{q^2}{2C} satisfies W˙=−RI2≤0\dot W = -RI^2 \le 0. With a source, W˙=IE−RI2\dot W = IE - RI^2.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
A polynomial of degree n has at most n roots Theorem
A non-zero polynomial of degree nn has at most nn roots (real or complex).
Vol. 2, 0.6 Complex numbers and polynomials, done properly
A quadratic form is squeezed by the extreme eigenvalues Lemma
If AA is a real symmetric matrix with eigenvalues λmin⁡≤⋯≤λmax⁡\lambda_{\min} \le \dots \le \lambda_{\max}, then λmin⁡∥v∥2≤vTAv≤λmax⁡∥v∥2\lambda_{\min}\lVert v \rVert^2 \le v^{\mathsf T}Av \le \lambda_{\max}\lVert v \rVert^2 for every vv, with equality at the corresponding eigenvectors.
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
A repeated move has as many positions as its order Theorem
If g has finite order k then ⟨g⟩ = {e, g, g², …, g^(k−1)} has exactly k elements, and gᵐ = e exactly when k divides m.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
A stochastic matrix keeps probability vectors Theorem
If PP is stochastic and xx is a probability vector, then PxPx is a probability vector. Also a product of stochastic matrices is stochastic.
Vol. 2, 2.11 Markov chains and PageRank
A strict inequality between continuous fields defines an open set Theorem
 
Vol. 2, 5.1 Scalar and vector fields, limits and continuity
A system has zero, one or infinitely many solutions Corollary
No solution if bb is not in the range of AA. Otherwise one solution if the null space is {O}\{O\}, and infinitely many if it is bigger.
Vol. 2, 2.6 Systems of equations and elimination
A vector field is differentiable exactly when its components are Theorem
F=(F1,…,Fm)F = (F_1, \dots, F_m) is differentiable at aa if and only if every FiF_i is, and then F′(a)(y)=(∇F1(a)⋅y,…,∇Fm(a)⋅y)F'(a)(y) = (\nabla F_1(a)\cdot y, \dots, \nabla F_m(a)\cdot y), whose matrix is the Jacobian.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Abel's formula Theorem
If b1,…,bnb_1, \dots, b_n solve y(n)+an−1y(n−1)+⋯=0y^{(n)} + a_{n-1}y^{(n-1)} + \dots = 0, their Wronskian satisfies W′=−an−1WW' = -a_{n-1}W, so W(t)=W(t0)exp⁡ ⁣(−∫t0tan−1)W(t) = W(t_0)\exp\!\big(-\int_{t_0}^{t}a_{n-1}\big).
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Abelian group Definition
A group in which ab = ba for all a and b.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Absolute convergence Definition
∑ak\sum a_k converges absolutely if ∑∣ak∣\sum |a_k| converges.
Vol. 2, 1.6 Series, power series, and uniform convergence
Absolute convergence implies convergence Theorem
If ∑∣ak∣\sum |a_k| converges, then ∑ak\sum a_k converges, and ∣∑ak∣≤∑∣ak∣\left|\sum a_k\right| \le \sum |a_k|.
Vol. 2, 1.6 Series, power series, and uniform convergence
Absolute maximum Definition
A point aa of the domain SS with f(x)≤f(a)f(x) \le f(a) for every x∈Sx \in S (a global maximum).
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
Absolute minimum Definition
A point aa of the domain SS with f(x)≥f(a)f(x) \ge f(a) for every x∈Sx \in S (a global minimum).
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
Absolutely convergent matrix series converge Theorem
If ∑k∥Mk∥\sum_k\lVert M_k\rVert converges as a series of numbers, then ∑kMk\sum_kM_k converges in the space of matrices.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Additivity for overlapping sets Theorem
If ff is finitely additive on a Boolean algebra, then f(A∪B)=f(A)+f(B∖A)f(A \cup B) = f(A) + f(B \setminus A) and f(A∪B)=f(A)+f(B)−f(A∩B)f(A \cup B) = f(A) + f(B) - f(A \cap B) for all A,BA, B in the algebra.
Vol. 2, 10.1 Probability as measure
Additivity of the integral over intervals Theorem
If a<c<ba < c < b and ff is integrable on [a,c][a, c] and on [c,b][c, b], then it is integrable on [a,b][a, b] and ∫abf=∫acf+∫cbf\int_a^b f = \int_a^c f + \int_c^b f.
Vol. 2, 1.5 The Riemann integral: area as a limit
Adjoint Definition
The adjoint A∗A^* is the map with (Ax,y)=(x,A∗y)(Ax, y) = (x, A^*y) for all x,yx, y; for real matrices with the dot product it is the transpose.
Vol. 2, 3.1 Symmetric matrices and the spectral theorem
Algebraic limit laws Theorem
If an→aa_n \to a and bn→bb_n \to b, then an+bn→a+ba_n + b_n \to a + b, c an→cac\,a_n \to ca, anbn→aba_n b_n \to ab, and an/bn→a/ba_n/b_n \to a/b when b≠0b \ne 0.
Vol. 2, 1.2 Sequences and limits, from zero
All bases have the same size Theorem
If VV has a basis with nn elements, every basis of VV has nn elements.
Vol. 2, 2.2 Span, independence, basis, dimension
All norms on R^n are equivalent Theorem
For any norm ∥⋅∥\lVert \cdot \rVert on Rn\mathbb R^n there are constants 0<m≤M0 < m \le M with m∥x∥1≤∥x∥≤M∥x∥1m\lVert x \rVert_1 \le \lVert x \rVert \le M\lVert x \rVert_1 for all xx.
Vol. 2, 4.5 Continuity between metric spaces
Alternating series test Theorem
If bkb_k decreases to 00, then ∑(−1)k+1bk\sum (-1)^{k+1} b_k converges, and the error after nn terms is at most bn+1b_{n+1}.
Vol. 2, 1.6 Series, power series, and uniform convergence
Ampere's law Definition
For the magnetic field of steady currents, the circulation of BB round a closed loop CC is μ0\mu_0 times the current through any surface bounded by CC: ∮CB⋅dℓ=μ0∬SJ⋅n dS\oint_CB\cdot d\ell = \mu_0\iint_SJ\cdot n\,dS, locally ∇×B=μ0J\nabla\times B = \mu_0J.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
An eigenvector has only one eigenvalue Fact
If T(x)=λxT(x) = \lambda x and T(x)=μxT(x) = \mu x with x≠Ox \ne O, then λ=μ\lambda = \mu.
Vol. 2, 2.8 Eigenvalues and eigenvectors
An implication equals its contrapositive Theorem
P⇒QP \Rightarrow Q and ¬Q⇒¬P\neg Q \Rightarrow \neg P are true in exactly the same situations.
Vol. 2, 0.1 How to read a theorem
An IVP is an integral equation Theorem
A continuous function yy solves y′=f(t,y)y' = f(t, y), y(t0)=y0y(t_0) = y_0 on an interval exactly when y(t)=y0+∫t0tf(s,y(s)) dsy(t) = y_0 + \int_{t_0}^{t} f(s, y(s))\,ds for every tt in it.
Vol. 2, 7.1 Existence and uniqueness for differential equations
Analytic function Definition
A function ff is analytic on (x0−r,x0+r)(x_0 - r, x_0 + r) if it equals a power series ∑an(x−x0)n\sum a_n(x - x_0)^n at every point of that interval.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Annihilating operator Definition
A constant-coefficient operator BB with Bf=0Bf = 0: it sends the function ff to zero. Example: D−rD - r annihilates erte^{rt}, (D−r)m(D - r)^m annihilates tm−1ertt^{m-1}e^{rt}.
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Annihilator Definition
For a subspace U of V, the set U⁰ of functionals that are 0 on every vector of U.
Vol. 2, 3.7 Dual spaces and quotient spaces
Approximation property of the supremum Theorem
 
Vol. 2, 1.1 The real numbers and completeness
Archimedean property Definition
 
Vol. 2, 1.1 The real numbers and completeness
Area as a line integral Theorem
For a positively oriented piecewise smooth Jordan curve α(t)=(X(t),Y(t))\alpha(t) = (X(t), Y(t)) bounding SS, and any real cc, area(S)=∫ab[(c−1)YX′+cXY′] dt\text{area}(S) = \int_a^b\big[(c - 1)YX' + cXY'\big]\,dt; with c=1,0,12c = 1, 0, \frac12: area(S)=∮x dy=−∮y dx=12∮(x dy−y dx)\text{area}(S) = \oint x\,dy = -\oint y\,dx = \frac12\oint(x\,dy - y\,dx).
Vol. 2, 6.4 Green's theorem and change of variables
Area under a change of variables Theorem
 
Vol. 2, 6.4 Green's theorem and change of variables
Arithmetic respects congruence Theorem
If a≡a′a \equiv a' and b≡b′b \equiv b' (mod nn), then a+b≡a′+b′a + b \equiv a' + b' and ab≡a′b′ab \equiv a'b'; so addition and multiplication of classes are well defined.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Asymptotically stable Definition
 
Vol. 2, 7.6 Phase portraits, stability and linearization
Augmented matrix Definition
The matrix [A∣b][A \mid b]: the coefficient matrix with the right-hand side added as an extra last column.
Vol. 2, 2.6 Systems of equations and elimination
Autonomous system Definition
A system x′=F(x)x' = F(x) whose right-hand side does not depend on the time tt.
Vol. 2, 7.6 Phase portraits, stability and linearization
Axioms 1 to 3 force a multiple of the determinant Theorem
If dd is a determinant function and FF satisfies only Axioms 1 to 3, then F(A)=d(A) F(I)F(A) = d(A)\,F(I) for every AA.
Vol. 2, 2.7 Determinants
B
Backpropagation Definition
Compute the derivative of a scalar output with respect to every input by applying the chain rule backwards through the computational graph, reusing each intermediate result once.
Vol. 2, 3.8 Matrix calculus and backpropagation
Banach fixed point theorem Theorem
A contraction TT of a non-empty complete metric space has exactly one fixed point x∗x^*; from any start x0x_0 the iterates xn+1=Txnx_{n+1} = T x_n converge to x∗x^*, with d(xn,x∗)≤qn1−q d(x1,x0)d(x_n, x^*) \le \dfrac{q^n}{1 - q}\,d(x_1, x_0).
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Basic reproduction number Definition
R0=β/γR_0 = \beta/\gamma: the average number of people infected by one infected person during the whole infectious period, when everyone else is susceptible.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Basic rules of probability Theorem
From the three axioms: P(∅)=0P(\varnothing) = 0; probability is finitely additive; P(Ac)=1−P(A)P(A^c) = 1 - P(A); A⊆BA \subseteq B implies P(A)≤P(B)P(A) \le P(B); every P(A)P(A) lies in [0,1][0, 1]; and P(A∪B)=P(A)+P(B)−P(A∩B)P(A \cup B) = P(A) + P(B) - P(A \cap B).
Vol. 2, 10.1 Probability as measure
Basis Definition
An independent set that spans the whole space: enough vectors to build everything, and none wasted.
Vol. 2, 2.2 Span, independence, basis, dimension
Basis for repeated roots Theorem
The mm functions ert,tert,…,tm−1erte^{rt}, te^{rt}, \dots, t^{m-1}e^{rt} are a basis of the solutions of (D−r)my=0(D - r)^my = 0.
Vol. 2, 7.2 Linear differential equations
Basis of solutions from the roots Theorem
If PA(t)=∏i=1k(t−ri)miP_A(t) = \prod_{i=1}^{k}(t - r_i)^{m_i} with distinct roots rir_i, the n=∑min = \sum m_i functions tjeritt^je^{r_it} (i≤ki \le k, 0≤j<mi0 \le j < m_i) are a basis of the solutions of Ay=0Ay = 0.
Vol. 2, 7.2 Linear differential equations
Bayes' theorem Theorem
 
Vol. 2, 10.1 Probability as measure
Bessel function Definition
Jn(x)=∑k≥0(−1)kk! (k+n)!(x2)2k+nJ_n(x) = \sum_{k \ge 0}\dfrac{(-1)^k}{k!\,(k+n)!}\left(\dfrac x2\right)^{2k+n}, the solution of Bessel's equation x2y′′+xy′+(x2−n2)y=0x^2y'' + xy' + (x^2 - n^2)y = 0 that is finite at x=0x = 0 (for n=0,1,2,…n = 0, 1, 2, \dots).
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Best approximation theorem Theorem
Among all points of SS, the projection ss is the unique closest point to xx: ∥x−s∥≤∥x−t∥\lVert x - s\rVert \le \lVert x - t\rVert for every t∈St \in S.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Bézout's identity Theorem
The gcd of aa and bb is always an integer combination of them: gcd⁡(a,b)=ax+by\gcd(a, b) = ax + by for some integers x,yx, y. In fact it is the smallest positive number of that form.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Bijections and inverses Theorem
f:A→Bf: A \to B is bijective exactly when there is a function g:B→Ag: B \to A that undoes it in both orders; this gg is the inverse f−1f^{-1}.
Vol. 2, 0.3 Sets, functions, and counting infinity
Bijective Definition
ff is bijective if it is both injective and surjective: every element of the codomain is hit by exactly one input.
Vol. 2, 0.3 Sets, functions, and counting infinity
Bolzano–Weierstrass in R^n Theorem
Every closed bounded subset of Rn\mathbb R^n is sequentially compact: each sequence in it has a subsequence converging to a point of it.
Vol. 2, 4.3 Compactness
Bolzano–Weierstrass theorem Theorem
Every bounded sequence has a convergent subsequence.
Vol. 2, 1.2 Sequences and limits, from zero
Boolean algebra of sets Definition
A non-empty family of subsets of a set SS that contains the union A∪BA \cup B and the complement Ac=S∖AA^c = S \setminus A whenever it contains AA and BB.
Vol. 2, 10.1 Probability as measure
Bordered determinant test in two variables Corollary
For f(x,y)f(x, y) with one constraint gg at a regular point: det⁡B>0\det B \gt 0 means a strict local constrained maximum, det⁡B<0\det B \lt 0 a strict local constrained minimum, where BB is the 3×33 \times 3 bordered Hessian.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Bordered Hessian Definition
The (n+m)×(n+m)(n + m) \times (n + m) symmetric matrix B=[0Dg(a)Dg(a)TH]B = \begin{bmatrix}0 & Dg(a)\\ Dg(a)^{\mathsf T} & H\end{bmatrix}, where H=D2f(a)−∑λiD2gi(a)H = D^2f(a) - \sum\lambda_iD^2g_i(a) is the Hessian in xx of the Lagrangian.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Boundary Definition
The boundary of AA is every point whose every ball touches both AA and the complement of AA: the edge of AA.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Bounded Definition
A set is bounded above if it has an upper bound, bounded below if it has a lower bound, and bounded if both.
Vol. 2, 1.1 The real numbers and completeness
Bounded set in a metric space Definition
A set KK is bounded if it fits inside some ball: there are a point pp and a radius RR with K⊆B(p,R)K \subseteq B(p, R).
Vol. 2, 4.3 Compactness
Bounded with discontinuities of content zero is integrable Theorem
If ff is bounded on a rectangle QQ and the set of points where ff is not continuous has content zero, then ff is integrable on QQ.
Vol. 2, 6.3 Multiple integrals
Building a linear map from the images of a basis Corollary
If T(ek)=ukT(e_k) = u_k on a basis, then TT is onto WW exactly when the uku_k span WW, one-to-one exactly when they are independent, and an isomorphism exactly when they are a basis of WW.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Building continuous fields Theorem
Sums, scalar multiples, dot products, norms and compositions of continuous fields are continuous; so are the coordinate functions, linear maps, polynomials, and quotients where the denominator is not zero.
Vol. 2, 5.1 Scalar and vector fields, limits and continuity
Building continuous maps Theorem
Compositions of continuous maps are continuous; sums, multiples, products and quotients (with non-zero denominator) of continuous real functions are continuous; a map into Rm\mathbb R^m is continuous iff each of its mm coordinate functions is; coordinate projections are continuous.
Vol. 2, 4.5 Continuity between metric spaces
C
C[a, b] with the sup metric is complete Theorem
Every Cauchy sequence of continuous functions on [a,b][a, b], in the sup metric, converges uniformly to a continuous function.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Catastrophic cancellation Definition
The loss of most or all correct digits when two nearly equal numbers, each carrying a small rounding error, are subtracted.
Vol. 2, 15.1 Numerical analysis
Cauchy criterion Theorem
A sequence of real numbers converges if and only if it is Cauchy.
Vol. 2, 1.2 Sequences and limits, from zero
Cauchy criterion for series Theorem
 
Vol. 2, 1.6 Series, power series, and uniform convergence
Cauchy sequence Definition
 
Vol. 2, 1.2 Sequences and limits, from zero
Cauchy sequence in a metric space Definition
 
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Cauchy–Schwarz inequality Theorem
∣(x,y)∣≤∥x∥ ∥y∥|(x, y)| \le \lVert x\rVert\,\lVert y\rVert, with equality exactly when xx and yy are linearly dependent.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Cauchy's mean value theorem Lemma
If g,kg, k are continuous on [0,h][0, h], differentiable on (0,h)(0, h) and k′≠0k' \ne 0 there, then g(h)−g(0)k(h)−k(0)=g′(τ)k′(τ)\dfrac{g(h) - g(0)}{k(h) - k(0)} = \dfrac{g'(\tau)}{k'(\tau)} for some τ∈(0,h)\tau \in (0, h).
Vol. 2, 15.1 Numerical analysis
Cayley–Hamilton theorem Theorem
Every square matrix satisfies its own characteristic polynomial: if p(λ) = det(λI − A), then p(A) = 0.
Vol. 2, 3.6 Cayley–Hamilton, Schur, and the Jordan form
Centre Definition
The origin of x′=Axx' = Ax when AA has purely imaginary eigenvalues ±ib\pm ib, b≠0b \ne 0: every orbit is a closed curve (an ellipse) around it.
Vol. 2, 7.6 Phase portraits, stability and linearization
Centre of mass Definition
For a wire with density φ\varphi, the mass is M=∫Cφ dsM = \int_C \varphi\,ds, and the centre of mass is the point (xˉ,yˉ,zˉ)(\bar x, \bar y, \bar z) with xˉ M=∫Cx φ ds\bar x\,M = \int_C x\,\varphi\,ds, and likewise for yy and zz.
Vol. 2, 6.1 Paths and line integrals
Chain rule Theorem
If gg is differentiable at aa and ff at g(a)g(a), then (f∘g)′(a)=f′(g(a)) g′(a)(f \circ g)'(a) = f'(g(a))\,g'(a).
Vol. 2, 1.4 The derivative as best linear approximation
Change of basis Definition
The matrix CC whose column jj is the new basis vector fjf_j written in old coordinates; it converts new coordinates into old ones.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Change of basis rewrites the matrix of a map Theorem
If AA and BB are the matrices of TT in the old and new bases, then B=C−1ACB = C^{-1}AC. Conversely every C−1ACC^{-1}AC is the matrix of the same map in some basis.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Change of variables in a double integral Theorem
If g:T→Sg: T \to S is one-to-one and C1C^1 with J≠0J \ne 0 (allowed to fail on a set of content zero) and ff is continuous on SS, then ∬Sf dx dy=∬Tf(X(u,v),Y(u,v)) ∣J(u,v)∣ du dv\iint_Sf\,dx\,dy = \iint_Tf(X(u, v), Y(u, v))\,|J(u, v)|\,du\,dv.
Vol. 2, 6.4 Green's theorem and change of variables
Characteristic curve Definition
A curve (x(s),y(s))(x(s), y(s)) along which the PDE a ux+b uy+c u=fa\,u_x + b\,u_y + c\,u = f turns into an ordinary differential equation: x′=ax' = a, y′=by' = b.
Vol. 2, 5.9 Partial differential equations
Characteristic polynomial Definition
The polynomial pA(λ)=det⁡(λI−A)p_A(\lambda) = \det(\lambda I - A). Its roots are exactly the eigenvalues of AA.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Characteristic polynomial of an operator Definition
For A=Dn+an−1Dn−1+⋯+a0A = D^n + a_{n-1}D^{n-1} + \dots + a_0, the polynomial PA(t)=tn+an−1tn−1+⋯+a0P_A(t) = t^n + a_{n-1}t^{n-1} + \dots + a_0. Its roots decide the solutions.
Vol. 2, 7.2 Linear differential equations
Charge density Definition
The function ρ(r)\rho(r) such that the charge in a region EE is Q=∭Eρ dVQ = \iiint_E\rho\,dV.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Chebyshev nodes Definition
The n+1n+1 roots of Tn+1T_{n+1}: xk=cos⁡(2k+1)π2n+2x_k = \cos\dfrac{(2k+1)\pi}{2n+2} for k=0,…,nk = 0, \dots, n. They are the projections onto the xx-axis of equally spaced points on a semicircle, so they crowd toward the ends.
Vol. 2, 15.1 Numerical analysis
Chebyshev polynomial Definition
T0=1T_0 = 1, T1=xT_1 = x, and Tn+1(x)=2x Tn(x)−Tn−1(x)T_{n+1}(x) = 2x\,T_n(x) - T_{n-1}(x). The key property is Tn(cos⁡θ)=cos⁡(nθ)T_n(\cos\theta) = \cos(n\theta).
Vol. 2, 15.1 Numerical analysis
Chebyshev's inequality Theorem
 
Vol. 2, 10.1 Probability as measure
Chebyshev's minimal property Theorem
Among all monic polynomials of degree m≥1m \ge 1, none has a smaller largest absolute value on [−1,1][-1, 1] than 21−m2^{1-m}, and Tm/2m−1T_m/2^{m-1} achieves it.
Vol. 2, 15.1 Numerical analysis
Circulation Definition
The circulation of a field FF around a closed curve CC is ∮CF⋅dr\oint_C F \cdot dr.
Vol. 2, 6.1 Paths and line integrals
Class C^k Definition
A field is of class CkC^k on an open set if all its partial derivatives of order at most kk exist and are continuous there; C∞C^\infty means CkC^k for every kk.
Vol. 2, 5.5 Higher partial derivatives and the equality of mixed partials
Classification of planar linear systems Theorem
 
Vol. 2, 7.4 Systems of equations and the matrix exponential
Classification of the origin by trace and determinant Theorem
 
Vol. 2, 7.6 Phase portraits, stability and linearization
Closed form Definition
A form ω\omega with dω=0d\omega = 0.
Vol. 2, 6.7 Differential forms and the one big theorem
Closed path Definition
A path r:[a,b]→Rnr: [a, b] \to \mathbb R^n with r(a)=r(b)r(a) = r(b): it ends where it starts.
Vol. 2, 6.1 Paths and line integrals
Closed set Definition
A set is closed if its complement is open.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Closed sets and limits of sequences Theorem
A point lies in the closure of AA if and only if some sequence in AA converges to it. Hence AA is closed if and only if the limit of every convergent sequence of points of AA lies in AA.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Closed subsets of compact sets are compact Lemma
If QQ is compact and F⊆QF \subseteq Q is closed, then FF is compact.
Vol. 2, 4.3 Compactness
Closed subsets of complete spaces are complete Theorem
Inside a complete space, a subset with the same distance is complete if and only if it is closed.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Closed surface Definition
A surface without a boundary curve of its own, such as the boundary of a solid region: a sphere, the surface of a cube or a torus. An open surface such as a bowl or a cube without a lid has a boundary curve.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Closed under Definition
A set is closed under an operation when applying it to elements of the set never produces something outside the set.
Vol. 2, 2.1 Vector spaces and subspaces
Closure Definition
The closure of AA is every point whose every ball touches AA: the set AA together with its edge.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Closure of a connected set is connected Lemma
If AA is connected and A⊆B⊆A‾A \subseteq B \subseteq \overline A, then BB is connected.
Vol. 2, 4.4 Connectedness and path-connectedness
Closure properties of countable sets Corollary
Subsets of countable sets are countable; the image of a countable set under any function is countable; a product of two countable sets is countable.
Vol. 2, 0.3 Sets, functions, and counting infinity
Cofactor Definition
The number Ckj=(−1)k+jdet⁡AkjC_{kj} = (-1)^{k+j}\det A_{kj}: the determinant of the minor with a checkerboard sign.
Vol. 2, 2.7 Determinants
Cofactor formula for the inverse Theorem
A (cof⁡A)T=(det⁡A) IA\,(\operatorname{cof}A)^{\mathsf T} = (\det A)\,I, so when det⁡A≠0\det A \ne 0, A−1=1det⁡A(cof⁡A)TA^{-1} = \frac1{\det A}(\operatorname{cof}A)^{\mathsf T}.
Vol. 2, 2.7 Determinants
Cofactor matrix Definition
The matrix whose (i,j)(i, j) entry is the cofactor CijC_{ij}. Its transpose is the adjugate.
Vol. 2, 2.7 Determinants
Column space Definition
The span of the columns of AA. It equals the range of x↦Axx \mapsto Ax.
Vol. 2, 2.6 Systems of equations and elimination
Compact equals complete and totally bounded Theorem
A metric space is compact if and only if it is complete and totally bounded.
Vol. 2, 4.3 Compactness
Compact equals sequentially compact Theorem
In a metric space, a set is compact if and only if it is sequentially compact.
Vol. 2, 4.3 Compactness
Compact set Definition
A set KK is compact if every open cover of KK has a finite subcover.
Vol. 2, 4.3 Compactness
Compact sets are closed and bounded Theorem
In any metric space, every compact set is closed and bounded.
Vol. 2, 4.3 Compactness
Companion matrix Definition
The matrix A(t)A(t) with ones directly above the diagonal and the last row (−a0,−a1,…,−an−1)(-a_0, -a_1, \dots, -a_{n-1}), for which x=(y,y′,…,y(n−1))x = (y, y', \dots, y^{(n-1)}) satisfies x′=A(t)x+(0,…,0,R)x' = A(t)x + (0, \dots, 0, R).
Vol. 2, 7.2 Linear differential equations
Comparing the 1-, 2- and max-norms Theorem
For every x∈Rnx \in \mathbb R^n: ∥x∥∞≤∥x∥2≤∥x∥1≤n ∥x∥2≤n ∥x∥∞\lVert x \rVert_\infty \le \lVert x \rVert_2 \le \lVert x \rVert_1 \le \sqrt n\,\lVert x \rVert_2 \le n\,\lVert x \rVert_\infty.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Comparison test Theorem
If 0≤ak≤bk0 \le a_k \le b_k and ∑bk\sum b_k converges, then ∑ak\sum a_k converges; if ∑ak\sum a_k diverges, so does ∑bk\sum b_k.
Vol. 2, 1.6 Series, power series, and uniform convergence
Complement Definition
AcA^c is everything in the universe UU that is not in AA.
Vol. 2, 0.3 Sets, functions, and counting infinity
Complements of independent events Theorem
If AA and BB are independent, so are AA and BcB^c, AcA^c and BB, and AcA^c and BcB^c.
Vol. 2, 10.1 Probability as measure
Complete metric space Definition
A metric space in which every Cauchy sequence converges to a point of the space.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Completeness axiom Definition
Every non-empty set of real numbers that is bounded above has a supremum in R\mathbb R.
Vol. 2, 1.1 The real numbers and completeness
Complex number Definition
An ordered pair (a,b)(a, b) of real numbers, added by (a,b)+(c,d)=(a+c,b+d)(a,b) + (c,d) = (a+c, b+d) and multiplied by (a,b)(c,d)=(ac−bd, ad+bc)(a,b)(c,d) = (ac - bd,\ ad + bc).
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Complex roots of real polynomials come in conjugate pairs Theorem
If a polynomial with real coefficients has root zz, then zˉ\bar z is also a root.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Composite trapezoidal and Simpson rules Theorem
With NN pieces of width hh: TN=h(12f0+f1+⋯+fN−1+12fN)T_N = h\big(\tfrac12 f_0 + f_1 + \cdots + f_{N-1} + \tfrac12 f_N\big) has error at most (b−a)h212M2\dfrac{(b-a)h^2}{12}M_2, and (for NN even) SN=h3(f0+4f1+2f2+4f3+⋯+4fN−1+fN)S_N = \dfrac h3\big(f_0 + 4f_1 + 2f_2 + 4f_3 + \cdots + 4f_{N-1} + f_N\big) has error at most (b−a)h4180M4\dfrac{(b-a)h^4}{180}M_4.
Vol. 2, 15.1 Numerical analysis
Composition Definition
The map STST that does TT first and then SS: (ST)(x)=S(T(x))(ST)(x) = S(T(x)).
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Composition distributes over addition Proposition
(S+T)R=SR+TR(S + T)R = SR + TR and R(S+T)=RS+RTR(S + T) = RS + RT (the second needs RR linear); scalars pass through too.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Composition is associative Theorem
For any three functions that can be chained, R(ST)=(RS)TR(ST) = (RS)T.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Composition of injections and surjections Proposition
If ff and gg are injective, so is g∘fg \circ f; if both are surjective, so is g∘fg \circ f; hence a composition of bijections is a bijection.
Vol. 2, 0.3 Sets, functions, and counting infinity
Composition of linear maps is linear Theorem
If T:U→VT: U \to V and S:V→WS: V \to W are linear, then ST:U→WST: U \to W is linear.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Computational graph Definition
A diagram of a calculation: nodes are intermediate values, arrows say which values each one is computed from.
Vol. 2, 3.8 Matrix calculus and backpropagation
Computing the inverse by row reducing [A | I] Theorem
Row reduce [A∣I][A \mid I]. If the left block becomes II, the right block is A−1A^{-1}. If the left block cannot become II, AA has no inverse.
Vol. 2, 2.6 Systems of equations and elimination
Condition number Definition
κ(A)=∥A∥ ∥A−1∥=σ1/σn\kappa(A) = \lVert A \rVert\,\lVert A^{-1} \rVert = \sigma_1/\sigma_n: the worst-case factor by which A magnifies relative errors in solving Ax = b.
Vol. 2, 3.5 Matrix norms, conditioning, and why numerics fail
Conditional probability Definition
 
Vol. 2, 10.1 Probability as measure
Conditional probability is a probability measure Theorem
 
Vol. 2, 10.1 Probability as measure
Congruent mod n Definition
a≡b(modn)a \equiv b \pmod n means nn divides a−ba - b: aa and bb leave the same remainder on division by nn.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Conjugate Definition
The conjugate of z=a+biz = a + bi is zˉ=a−bi\bar z = a - bi, its mirror image in the real axis.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Connected means no proper clopen subset Proposition
A space AA is connected if and only if the only subsets that are both open and closed in AA are ∅\varnothing and AA.
Vol. 2, 4.4 Connectedness and path-connectedness
Connected set Definition
A set (a metric space) is connected if it has no separation: it cannot be written as two disjoint non-empty open pieces.
Vol. 2, 4.4 Connectedness and path-connectedness
Connected subsets of the line are the intervals Theorem
A subset of R\mathbb R is connected if and only if it is an interval.
Vol. 2, 4.4 Connectedness and path-connectedness
Consequences of Lagrange's theorem Corollary
In a finite group G: the order of every element divides |G|, so g^|G| = e; a group of prime order p is cyclic; and, for the group of invertible classes mod n, a^φ(n) ≡ 1 (Euler), in particular a^(p−1) ≡ 1 for prime p (Fermat).
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Consequences of the group axioms Theorem
In any group: the identity is unique; each element has exactly one inverse; (ab)⁻¹ = b⁻¹a⁻¹; ab = ac implies b = c (and ba = ca implies b = c); and ax = b has the unique solution x = a⁻¹b.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Consequences of the product rule Corollary
det⁡(A−1)=1/det⁡A\det(A^{-1}) = 1/\det A, det⁡(Ak)=(det⁡A)k\det(A^k) = (\det A)^k, det⁡(AB)=det⁡(BA)\det(AB) = \det(BA), and det⁡(cA)=cndet⁡A\det(cA) = c^n\det A for an n×nn \times n matrix.
Vol. 2, 2.7 Determinants
Constant-coefficient operator Definition
An operator A=Dn+an−1Dn−1+⋯+a0A = D^n + a_{n-1}D^{n-1} + \dots + a_0 with numbers aka_k as coefficients. It equals PA(D)P_A(D) for the polynomial PA(t)=tn+an−1tn−1+⋯+a0P_A(t) = t^n + a_{n-1}t^{n-1} + \dots + a_0.
Vol. 2, 7.2 Linear differential equations
Constant-coefficient operators multiply like polynomials Theorem
If A=PA(D)A = P_A(D) and B=PB(D)B = P_B(D) then AB=(PAPB)(D)AB = (P_AP_B)(D). In particular AB=BAAB = BA.
Vol. 2, 7.2 Linear differential equations
Constrained extremum Definition
A point aa with g(a)=cg(a) = c such that f(x)≤f(a)f(x) \le f(a) (a maximum) or f(x)≥f(a)f(x) \ge f(a) (a minimum) for all nearby xx that also satisfy g(x)=cg(x) = c.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Content zero Definition
 
Vol. 2, 6.3 Multiple integrals
Continuity equation Definition
If a conserved quantity has density uu and flux density jj, then ∂tu+∇⋅j=0\partial_tu + \nabla\cdot j = 0. For charge: ∂tρ+∇⋅J=0\partial_t\rho + \nabla\cdot J = 0.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Continuity of probability Theorem
If events grow, A1⊆A2⊆⋯A_1 \subseteq A_2 \subseteq \cdots, then P(An)→P(⋃An)P(A_n) \to P(\bigcup A_n). If events shrink, A1⊇A2⊇⋯A_1 \supseteq A_2 \supseteq \cdots, then P(An)→P(⋂An)P(A_n) \to P(\bigcap A_n).
Vol. 2, 10.1 Probability as measure
Continuous function Definition
ff is continuous at aa if lim⁡x→af(x)=f(a)\lim_{x \to a} f(x) = f(a): small changes of input near aa give small changes of output.
Vol. 2, 1.3 Limits and continuity with epsilon and delta
Continuous functions are integrable Theorem
If ff is continuous on [a,b][a, b], then ff is integrable on [a,b][a, b].
Vol. 2, 1.5 The Riemann integral: area as a limit
Continuous functions on a rectangle are integrable Theorem
If ff is continuous on a closed rectangle QQ, then ff is integrable on QQ.
Vol. 2, 6.3 Multiple integrals
Continuous image of a compact set is compact Theorem
If KK is compact and f:K→Yf : K \to Y is continuous, then f(K)f(K) is compact.
Vol. 2, 4.3 Compactness
Continuous map between metric spaces Definition
 
Vol. 2, 4.5 Continuity between metric spaces
Continuous maps pull open sets back to open sets Lemma
If f:X→Yf : X \to Y is continuous and WW is open in YY, then f−1(W)={x:f(x)∈W}f^{-1}(W) = \{x : f(x) \in W\} is open in XX.
Vol. 2, 4.4 Connectedness and path-connectedness
Continuous maps send convergent sequences to convergent sequences Lemma
If ff is continuous at aa and xn→ax_n \to a, then f(xn)→f(a)f(x_n) \to f(a).
Vol. 2, 4.3 Compactness
Continuous on a closed interval implies uniformly continuous Theorem
A continuous function on [a,b][a, b] is uniformly continuous there.
Vol. 2, 1.3 Limits and continuity with epsilon and delta
Continuous on a compact set implies uniformly continuous Theorem
A continuous map from a compact metric space to any metric space is uniformly continuous: one δ\delta works for the whole set.
Vol. 2, 4.3 Compactness
Continuous partial derivatives imply differentiable Theorem
If ff is continuously differentiable at aa, then ff is differentiable at aa, with Ta(v)=∇f(a)⋅vT_a(v) = \nabla f(a)\cdot v.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Continuously differentiable field Definition
A scalar field is continuously differentiable at aa if its partial derivatives exist in some ball around aa and are continuous at aa.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Contraction Definition
A map T:X→XT : X \to X that brings every pair of points closer together by a fixed factor q<1q < 1: d(Tx,Ty)≤q d(x,y)d(Tx, Ty) \le q\,d(x, y).
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Contrapositive Definition
The contrapositive of P⇒QP \Rightarrow Q is ¬Q⇒¬P\neg Q \Rightarrow \neg P; it always has the same truth value as the original.
Vol. 2, 0.1 How to read a theorem
Convergence for a diagonalizable chain with a simple eigenvalue 1 Theorem
Let PP be stochastic and diagonalizable. If 11 is an eigenvalue with a one-dimensional eigenspace and every other eigenvalue has size less than 1, then Pkx0P^kx_0 approaches the same stationary distribution π\pi from every starting probability vector x0x_0.
Vol. 2, 2.11 Markov chains and PageRank
Convergence in R^n is coordinatewise Theorem
A sequence of vectors converges in Rn\mathbb R^n (for any of the 1-, 2- or max-distances) if and only if each coordinate converges as a sequence of real numbers.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Convergence in the sup metric is uniform convergence Theorem
For continuous fnf_n and ff on [a,b][a, b]: d∞(fn,f)→0d_\infty(f_n, f) \to 0 if and only if fn→ff_n \to f uniformly on [a,b][a, b].
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Convergence of power series (Abel's lemma) Lemma
If ∑ckx0k\sum c_k x_0^k converges, then ∑ckxk\sum c_k x^k converges absolutely for every ∣x∣<∣x0∣|x| < |x_0|.
Vol. 2, 1.6 Series, power series, and uniform convergence
Convergent sequence Definition
 
Vol. 2, 1.2 Sequences and limits, from zero
Convergent sequence in a metric space Definition
 
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Convergent sequences are bounded Theorem
If an→La_n \to L, some single number bounds every ∣an∣|a_n|.
Vol. 2, 1.2 Sequences and limits, from zero
Convergent sequences are Cauchy Theorem
If xn→xx_n \to x in a metric space, then (xn)(x_n) is Cauchy.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Converse Definition
The converse of P⇒QP \Rightarrow Q is Q⇒PQ \Rightarrow P; it is a different statement and can be false when the original is true.
Vol. 2, 0.1 How to read a theorem
Convex function Definition
A function ff on a convex set with f(tx+(1−t)y)≤tf(x)+(1−t)f(y)f\big(tx + (1 - t)y\big) \le tf(x) + (1 - t)f(y) for all x,yx, y and t∈[0,1]t \in [0, 1]: the graph lies below every chord.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Convex set Definition
A set SS is convex if for any two points p,qp, q in SS, the whole segment (1−t)p+tq(1 - t)p + tq, 0≤t≤10 \le t \le 1, lies in SS.
Vol. 2, 6.2 Gradient fields and potentials
Coordinates Definition
The unique numbers (c1,…,cn)(c_1, \dots, c_n) with x=∑cieix = \sum c_i e_i for a chosen, ordered basis.
Vol. 2, 2.2 Span, independence, basis, dimension
Coordinates change by C Theorem
[x]E=C [x]F[x]_{\mathcal E} = C\,[x]_{\mathcal F}, and CC is invertible with C−1=mE→F(I)C^{-1} = m_{\mathcal E \to \mathcal F}(I).
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Coordinates in an orthogonal basis Theorem
In an orthogonal basis, the coordinate of xx on eie_i is (x,ei)/(ei,ei)(x, e_i)/(e_i, e_i); in an orthonormal basis it is (x,ei)(x, e_i) itself.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Coset Definition
For a subspace U and a vector v, the coset v + U is the set of all v + u with u in U: the subspace U moved by v.
Vol. 2, 3.7 Dual spaces and quotient spaces
Cosets are the classes modulo a subspace Theorem
Define v ∼ w when v − w ∈ U. This is an equivalence relation whose class of v is exactly the coset v + U. So v + U = w + U iff v − w ∈ U, and any two cosets are equal or disjoint.
Vol. 2, 3.7 Dual spaces and quotient spaces
Countable Definition
A set is countable if its elements can be put in a list, first, second, third, with every element appearing exactly once; finite sets count too.
Vol. 2, 0.3 Sets, functions, and counting infinity
Cramer's rule Definition
For an invertible AA, the solution of Ax=bAx = b has xj=det⁡Aj(b)/det⁡Ax_j = \det A_j(b)/\det A, where Aj(b)A_j(b) is AA with column jj replaced by bb.
Vol. 2, 2.7 Determinants
Cramer's rule is correct Theorem
If det⁡A≠0\det A \ne 0 then the unique solution of Ax=bAx = b is xj=det⁡Aj(b)/det⁡Ax_j = \det A_j(b)/\det A.
Vol. 2, 2.7 Determinants
Critical point Definition
A point aa where a differentiable scalar field has ∇f(a)=O\nabla f(a) = O; Apostol calls it a stationary point.
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
Cross product Definition
For a=(a1,a2,a3)a = (a_1, a_2, a_3) and b=(b1,b2,b3)b = (b_1, b_2, b_3) in R3\mathbb R^3, a×b=(a2b3−a3b2, a3b1−a1b3, a1b2−a2b1)a \times b = (a_2b_3 - a_3b_2,\ a_3b_1 - a_1b_3,\ a_1b_2 - a_2b_1): a vector perpendicular to both, whose length is the area of the parallelogram with sides aa and bb.
Vol. 2, 6.5 Surfaces, area and flux
Curl Definition
For F=(P,Q,R)F = (P, Q, R), curl⁡F=∇×F=(Ry−Qz, Pz−Rx, Qx−Py)\operatorname{curl}F = \nabla\times F = (R_y - Q_z,\ P_z - R_x,\ Q_x - P_y): a vector field that records how much, and about which axis, FF spins at each point.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Curl is circulation per unit area Proposition
For a C1C^1 field FF, a point pp and a unit vector nn, the circulation of FF around the circle of radius ε\varepsilon about pp in the plane perpendicular to nn (counterclockwise from the tip of nn), divided by its area πε2\pi\varepsilon^2, tends to (curl⁡F)(p)⋅n(\operatorname{curl}F)(p)\cdot n as ε→0\varepsilon\to0.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Current density Definition
The vector field JJ such that the current (charge per unit time) through a surface SS is ∬SJ⋅n dS\iint_SJ\cdot n\,dS.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
D
d is gradient, curl and divergence Theorem
In R3\mathbb R^3: df=fx dx+fy dy+fz dzdf = f_x\,dx + f_y\,dy + f_z\,dz (gradient); d(P dx+Q dy+R dz)=(Ry−Qz) dy∧dz+(Pz−Rx) dz∧dx+(Qx−Py) dx∧dyd(P\,dx + Q\,dy + R\,dz) = (R_y - Q_z)\,dy\wedge dz + (P_z - R_x)\,dz\wedge dx + (Q_x - P_y)\,dx\wedge dy (curl); d(A dy∧dz+B dz∧dx+C dx∧dy)=(Ax+By+Cz) dx∧dy∧dzd(A\,dy\wedge dz + B\,dz\wedge dx + C\,dx\wedge dy) = (A_x + B_y + C_z)\,dx\wedge dy\wedge dz (divergence).
Vol. 2, 6.7 Differential forms and the one big theorem
d squared is zero Theorem
For every C2C^2 form ω\omega, d(dω)=0d(d\omega) = 0. For ω=f\omega = f a function in R3\mathbb R^3 this is curl⁡∇f=0\operatorname{curl}\nabla f = 0, and for a 1-form it is div⁡curl⁡F=0\operatorname{div}\operatorname{curl}F = 0.
Vol. 2, 6.7 Differential forms and the one big theorem
d'Alembert's solution of the wave equation Theorem
If FF is twice differentiable and GG is differentiable, then u(x,t)=12[F(x+ct)+F(x−ct)]+12c∫x−ctx+ctG(s) dsu(x, t) = \tfrac12\big[F(x + ct) + F(x - ct)\big] + \dfrac1{2c}\displaystyle\int_{x - ct}^{x + ct}G(s)\,ds solves utt=c2uxxu_{tt} = c^2u_{xx} with u(x,0)=F(x)u(x, 0) = F(x) and ut(x,0)=G(x)u_t(x, 0) = G(x); conversely every C2C^2 solution on R2\mathbb R^2 has this form.
Vol. 2, 5.9 Partial differential equations
Darboux sums are integrals of step functions Theorem
The sup of the lower sums equals the sup of the integrals of step functions below ff, and likewise for upper sums, so Apostol's integral and the Darboux integral agree.
Vol. 2, 1.5 The Riemann integral: area as a limit
De Moivre's formula Corollary
(cos⁡θ+isin⁡θ)n=cos⁡nθ+isin⁡nθ(\cos\theta + i\sin\theta)^n = \cos n\theta + i\sin n\theta for every integer nn.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
De Morgan's laws for sets Theorem
(A∪B)c=Ac∩Bc(A \cup B)^c = A^c \cap B^c and (A∩B)c=Ac∪Bc(A \cap B)^c = A^c \cup B^c.
Vol. 2, 0.3 Sets, functions, and counting infinity
Degree Definition
The degree of a non-zero polynomial is the largest nn with an≠0a_n \ne 0.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Derivative Definition
f′(a)=lim⁡h→0f(a+h)−f(a)hf'(a) = \lim_{h \to 0} \frac{f(a + h) - f(a)}{h}, when the limit exists: the slope of the best straight-line fit to f at a.
Vol. 2, 1.4 The derivative as best linear approximation
Derivative of a complex exponential Fact
For a complex number r=α+iβr = \alpha + i\beta, ert=eαt(cos⁡βt+isin⁡βt)e^{rt} = e^{\alpha t}(\cos\beta t + i\sin\beta t) satisfies D(ert)=rertD(e^{rt}) = re^{rt}.
Vol. 2, 7.2 Linear differential equations
Derivative test for a contraction Theorem
If gg is differentiable on an interval II and ∣g′(x)∣≤q<1\lvert g'(x) \rvert \le q < 1 for every x∈Ix \in I, then ∣g(x)−g(y)∣≤q∣x−y∣\lvert g(x) - g(y) \rvert \le q\lvert x - y \rvert for all x,y∈Ix, y \in I.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Derivative test for a Lipschitz condition Theorem
If f(t,x)f(t, x) is differentiable in the real variable xx on a region where ∣∂f/∂x∣≤L\lvert \partial f/\partial x \rvert \le L and the region contains the segment between any two positions at the same time, then ff satisfies a Lipschitz condition with constant LL.
Vol. 2, 7.1 Existence and uniqueness for differential equations
Descent lemma Lemma
If ∇f\nabla f is LL-Lipschitz, then f(y)≤f(x)+∇f(x)⋅(y−x)+L2∥y−x∥2f(y) \le f(x) + \nabla f(x)\cdot(y - x) + \frac L2\lVert y - x\rVert^2; consequently the step y=x−η∇f(x)y = x - \eta\nabla f(x) with η≤1L\eta \le \frac1L gives f(y)≤f(x)−η2∥∇f(x)∥2f(y) \le f(x) - \frac\eta2\lVert\nabla f(x)\rVert^2.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Determinant Definition
The unique function of the rows of a square matrix satisfying the four axioms. Written det⁡A\det A or ∣A∣|A|. For a 2×22 \times 2 matrix it is ad−bcad - bc.
Vol. 2, 2.7 Determinants
Determinant by row reduction Theorem
If row operations turn AA into an upper triangular UU using pp swaps and scalings by c1,…,cqc_1, \dots, c_q, then det⁡A=(−1)p(c1⋯cq)−1u11⋯unn\det A = (-1)^p(c_1\cdots c_q)^{-1}u_{11}\cdots u_{nn}.
Vol. 2, 2.7 Determinants
Determinant function Definition
A number-valued function d(A1,…,An)d(A_1, \dots, A_n) of the rows of an n×nn \times n matrix that scales in each row, adds in each row, vanishes when two rows are equal, and equals 11 on the identity.
Vol. 2, 2.7 Determinants
Determinant of a block-diagonal matrix Theorem
For square blocks AA and BB, det⁡[AOOB]=det⁡A⋅det⁡B\det\begin{bmatrix}A&O\\O&B\end{bmatrix} = \det A\cdot\det B.
Vol. 2, 2.7 Determinants
Determinant of a triangular matrix Theorem
The determinant of a triangular matrix is the product of its diagonal entries.
Vol. 2, 2.7 Determinants
Determinant of an orthogonal matrix Theorem
An orthogonal matrix has determinant +1 (a rotation) or −1 (it includes a reflection).
Vol. 2, 3.3 Orthogonal matrices, rotations and reflections
Diagonal form means an eigenbasis Theorem
A map has a diagonal matrix in a basis exactly when every vector of that basis is an eigenvector. The diagonal entries are the eigenvalues.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Diagonal form of a linear map Theorem
For T:V→WT: V \to W of rank rr there are bases of VV and WW in which the matrix has 11s in the first rr diagonal places and 00 everywhere else.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Diagonalizable Definition
A map or matrix is diagonalizable if some basis makes its matrix diagonal; equivalently, if there is a basis of eigenvectors.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Diagonalizable exactly when the eigenspaces fill the space Theorem
With all roots among the scalars, AA is diagonalizable if and only if g(λ)=m(λ)g(\lambda) = m(\lambda) for every eigenvalue, that is, if and only if the dimensions of the eigenspaces add up to nn.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Diagonalization as a factorization Theorem
If AA has nn independent eigenvectors, then A=CDC−1A = CDC^{-1}, where the columns of CC are those eigenvectors and DD is diagonal with the matching eigenvalues.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Diffeomorphism Definition
A differentiable field F:U→VF: U \to V between open sets of Rn\mathbb R^n that has a differentiable inverse F−1:V→UF^{-1}: V \to U.
Vol. 2, 5.4 The chain rule for fields
Differentiability from n minus one continuous partials Theorem
If D1f,…,DnfD_1f, \dots, D_nf exist in a ball around aa, and D2f,…,DnfD_2f, \dots, D_nf are continuous at aa (while D1fD_1f merely exists at aa), then ff is differentiable at aa with total derivative v↦∇f(a)⋅vv \mapsto \nabla f(a)\cdot v.
Vol. 2, 5.5 Higher partial derivatives and the equality of mixed partials
Differentiable Definition
ff is differentiable at aa if f′(a)f'(a) exists; equivalently, f(a+h)=f(a)+f′(a)h+E(h)f(a + h) = f(a) + f'(a)h + E(h) with E(h)/h→0E(h)/h \to 0.
Vol. 2, 1.4 The derivative as best linear approximation
Differentiable field Definition
FF is differentiable at the interior point aa if F(a+v)=F(a)+Ta(v)+∥v∥E(a,v)F(a + v) = F(a) + T_a(v) + \lVert v \rVert E(a, v) for small vv, where TaT_a is a linear map and E(a,v)→0E(a, v) \to 0 as v→0v \to 0.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Differentiable fields are continuous Theorem
If FF is differentiable at aa, then FF is continuous at aa.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Differentiable implies continuous Theorem
If ff is differentiable at aa, it is continuous at aa.
Vol. 2, 1.4 The derivative as best linear approximation
Differential form Definition
A kk-form is a rule that assigns to each point a function of kk vectors that is linear in each and changes sign when two of them are swapped. In coordinates it is a sum of functions times dxi1∧⋯∧dxikdx_{i_1}\wedge\dots\wedge dx_{i_k}. A 0-form is a function.
Vol. 2, 6.7 Differential forms and the one big theorem
Differential operator Definition
The map LL that sends a function yy to the function y(n)+an−1y(n−1)+⋯+a0yy^{(n)} + a_{n-1}y^{(n-1)} + \dots + a_0y.
Vol. 2, 7.2 Linear differential equations
Differentiating a uniform limit of derivatives Theorem
If fnf_n have continuous derivatives, fn′→gf_n' \to g uniformly and fn(a)f_n(a) converges, then fn→ff_n \to f with f′=gf' = g.
Vol. 2, 1.6 Series, power series, and uniform convergence
Dimension Definition
The number of vectors in any basis. It is the number of independent directions, the number of coordinates you need.
Vol. 2, 2.2 Span, independence, basis, dimension
Dimension of a quotient space Theorem
If V is finite-dimensional and U a subspace, then dim V/U = dim V − dim U.
Vol. 2, 3.7 Dual spaces and quotient spaces
Dimension of an annihilator Theorem
For a subspace U of a finite-dimensional V, dim U⁰ = dim V − dim U.
Vol. 2, 3.7 Dual spaces and quotient spaces
Dimension of the solution space of a linear ODE Theorem
The solution space ker⁡L\ker L of a homogeneous linear equation of order nn has dimension exactly nn.
Vol. 2, 7.2 Linear differential equations
Direct proof Definition
To prove 'if P then Q': assume P, then derive Q one justified step at a time.
Vol. 2, 0.2 Proof techniques
Directional derivative Definition
For a scalar field ff, a point aa and a vector yy: f′(a;y)=lim⁡h→0f(a+hy)−f(a)hf'(a; y) = \lim_{h \to 0} \frac{f(a + hy) - f(a)}{h}, the rate of change of ff as you walk from aa in the direction yy; it is called the directional derivative when ∥y∥=1\lVert y \rVert = 1.
Vol. 2, 5.2 Directional derivatives, partial derivatives and the gradient
Directional derivative as a dot product with the gradient Theorem
If a scalar field ff is differentiable at aa, then f′(a;y)f'(a; y) exists for every yy and equals Ta(y)=∇f(a)⋅yT_a(y) = \nabla f(a)\cdot y; in particular TaT_a is unique.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Discrete metric Definition
On any set XX: d(x,y)=0d(x, y) = 0 if x=yx = y and d(x,y)=1d(x, y) = 1 if x≠yx \ne y.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Disease-free equilibrium Definition
A state with no infected people, i=0i = 0. In the SIR model every (s∗,0)(s^*, 0) is an equilibrium, so these form a whole line.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Displacement current Definition
The term ε0 ∂E/∂t\varepsilon_0\,\partial E/\partial t that Maxwell added to the current density in Ampère's law, so that ∇×B=μ0(J+ε0∂tE)\nabla\times B = \mu_0\big(J + \varepsilon_0\partial_tE\big).
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Distinct eigenvalues give an eigenbasis Theorem
On an nn-dimensional space a linear map has at most nn distinct eigenvalues, and if it has nn, their eigenvectors are a basis.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Distinct roots give a diagonalizable matrix Theorem
If the characteristic polynomial has nn different roots, the matrix is diagonalizable.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Distribution function Definition
FX(x)=P(X≤x)F_X(x) = P(X \le x): the probability that the random variable is at most xx, as a function of xx.
Vol. 2, 10.1 Probability as measure
Divergence Definition
For F=(P,Q,R)F = (P, Q, R), div⁡F=∇⋅F=Px+Qy+Rz\operatorname{div}F = \nabla\cdot F = P_x + Q_y + R_z: a scalar field that records how much FF spreads out from each point.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Divergence is flux per unit volume Proposition
For a C1C^1 field FF and a point pp, the outward flux of FF through the sphere SεS_\varepsilon of radius ε\varepsilon about pp, divided by the volume of the ball, tends to (div⁡F)(p)(\operatorname{div}F)(p) as ε→0\varepsilon\to0.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Divergent sequence Definition
A sequence that converges to no real number.
Vol. 2, 1.2 Sequences and limits, from zero
Divided difference Definition
f[x0,…,xk]f[x_0, \dots, x_k] is the coefficient of xkx^k in the interpolating polynomial of ff at x0,…,xkx_0, \dots, x_k. It satisfies f[x0,…,xk]=f[x1,…,xk]−f[x0,…,xk−1]xk−x0f[x_0, \dots, x_k] = \dfrac{f[x_1, \dots, x_k] - f[x_0, \dots, x_{k-1}]}{x_k - x_0}.
Vol. 2, 15.1 Numerical analysis
Divides Definition
a∣ba \mid b means bb is a whole-number multiple of aa: b=akb = ak for some integer kk.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Divisibility facts Proposition
Divisors pass through sums and multiples: if aa divides bb and cc, it divides bx+cybx + cy for all integers x,yx, y; divisibility chains; and a divisor of a non-zero number is at most as large in size.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Division algorithm Theorem
For any integer aa and positive integer bb there are unique integers qq and rr with a=bq+ra = bq + r and 0≤r<b0 \le r < b.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Division in Z_p Corollary
If pp is prime, every integer not divisible by pp has an inverse mod pp; and if gcd⁡(c,n)=1\gcd(c, n) = 1, you may cancel cc: ca≡cbca \equiv cb implies a≡ba \equiv b (mod nn).
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Double inclusion Theorem
A=BA = B exactly when A⊆BA \subseteq B and B⊆AB \subseteq A.
Vol. 2, 0.3 Sets, functions, and counting infinity
Double integral Definition
For a bounded ff on a rectangle QQ, the lower integral is the supremum of ∬s\iint s over step functions s≤fs \le f, the upper integral is the infimum of ∬t\iint t over step functions t≥ft \ge f; if they are equal, ff is integrable and the common value is ∬Qf\iint_Q f.
Vol. 2, 6.3 Multiple integrals
Dual basis Definition
Given a basis v₁,…,vₙ of V, the functionals φ₁,…,φₙ with φᵢ(vⱼ) = 1 if i = j and 0 otherwise; φᵢ(v) is the i-th coordinate of v.
Vol. 2, 3.7 Dual spaces and quotient spaces
Dual basis from the inverse matrix Proposition
If the columns of an invertible matrix B are a basis b₁,…,bₙ of Rⁿ, the dual basis functionals are the rows of B⁻¹.
Vol. 2, 3.7 Dual spaces and quotient spaces
Dual map Definition
For T: V → W, the map Tᵀ: W* → V* that sends a functional ψ on W to the functional ψ∘T on V: first apply T, then read with ψ.
Vol. 2, 3.7 Dual spaces and quotient spaces
Dual of a composition Corollary
(S∘T)ᵀ = Tᵀ∘Sᵀ: the dual map of a composition is the composition of the dual maps in the opposite order.
Vol. 2, 3.7 Dual spaces and quotient spaces
Dual space Definition
The set V* of all linear functionals on V, itself a vector space under adding functionals and scaling them value by value.
Vol. 2, 3.7 Dual spaces and quotient spaces
E
e^(A+B) equals e^A e^B when A and B commute Theorem
If AB=BAAB = BA then eA+B=eAeBe^{A+B} = e^Ae^B. Without AB=BAAB = BA the equation can fail.
Vol. 2, 7.4 Systems of equations and the matrix exponential
e^A is always invertible Corollary
For every square matrix AA, eAe^A is invertible and (eA)−1=e−A(e^A)^{-1} = e^{-A}. Moreover det⁡eA=etr⁡A\det e^A = e^{\operatorname{tr}A} (a fact beyond the course).
Vol. 2, 7.4 Systems of equations and the matrix exponential
Eckart–Young theorem Theorem
The truncated SVD A_k is the best rank-k approximation of A; its error is the first discarded singular value σ_{k+1} (in the operator norm).
Vol. 2, 3.4 The singular value decomposition and PCA
Eigenspace Definition
All vectors xx with T(x)=λxT(x) = \lambda x, together with OO: the eigenvectors of λ\lambda plus the zero vector. It equals the null space of T−λIT - \lambda I.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Eigenspaces are subspaces Theorem
E(λ)E(\lambda) is a subspace, because it is the null space of the linear map T−λIT - \lambda I.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Eigenvalue Definition
The scalar λ\lambda in T(x)=λxT(x) = \lambda x: the stretch factor along an eigenvector.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Eigenvalues are roots of the characteristic polynomial Theorem
λ\lambda is an eigenvalue of AA exactly when det⁡(λI−A)=0\det(\lambda I - A) = 0.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Eigenvalues of a stochastic matrix have size at most one Theorem
Every eigenvalue λ\lambda of a stochastic matrix, real or complex, satisfies ∣λ∣≤1|\lambda| \le 1.
Vol. 2, 2.11 Markov chains and PageRank
Eigenvalues of an orthogonal matrix Theorem
Every eigenvalue of an orthogonal (or unitary) matrix has absolute value 1.
Vol. 2, 3.3 Orthogonal matrices, rotations and reflections
Eigenvector Definition
A non-zero vector xx that a map TT from a space to itself only stretches: T(x)=λxT(x) = \lambda x for some scalar λ\lambda.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Eigenvectors give solutions Fact
If Av=λvAv = \lambda v with v≠Ov \ne O, then x(t)=eλtvx(t) = e^{\lambda t}v solves x′=Axx' = Ax.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Eigenvectors of a symmetric matrix are orthogonal Theorem
Eigenvectors of a symmetric matrix for different eigenvalues are perpendicular.
Vol. 2, 3.1 Symmetric matrices and the spectral theorem
Eigenvectors of distinct eigenvalues are independent Theorem
Eigenvectors that belong to different eigenvalues are linearly independent.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Electric field Definition
The vector field EE such that a small charge qq at a point feels the force qEqE; for a point charge qq at the origin, E=q4πε0r∣r∣3E = \dfrac{q}{4\pi\varepsilon_0}\dfrac{r}{\lvert r\rvert^3} (Coulomb's law).
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Electromagnetic waves Theorem
In empty space (ρ=0\rho = 0, J=0J = 0) each Cartesian component of EE satisfies the wave equation ∂t2E=c2∇2E\partial_t^2E = c^2\nabla^2E with c=1/μ0ε0≈2.998×108c = 1/\sqrt{\mu_0\varepsilon_0}\approx2.998\times10^8 m/s.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Elementary matrix Definition
The matrix you get by doing one row operation to the identity matrix.
Vol. 2, 2.6 Systems of equations and elimination
Epsilon-sandwich criterion for the double integral Theorem
 
Vol. 2, 6.3 Multiple integrals
Equal classes Lemma
For an equivalence relation, a∼ba \sim b exactly when [a]=[b][a] = [b], exactly when [a][a] and [b][b] share at least one element.
Vol. 2, 0.4 Equivalence relations and partitions
Equal mixed partials suffice on a convex set Theorem
If SS is open and convex, F=(P,Q)F = (P, Q) is C1C^1 on SS and Py=QxP_y = Q_x, then FF is a gradient field on SS; in space the same holds when the curl is zero.
Vol. 2, 6.2 Gradient fields and potentials
Equal mixed partials suffice on a simply connected set Theorem
If SS is open and simply connected in the plane and F=(P,Q)F = (P, Q) is C1C^1 with Py=QxP_y = Q_x, then FF is a gradient on SS.
Vol. 2, 6.2 Gradient fields and potentials
Equality of mixed partials (Schwarz, Clairaut) Theorem
If fxf_x, fyf_y, fxyf_{xy}, fyxf_{yx} exist on an open set containing (a,b)(a, b) and fxyf_{xy} and fyxf_{yx} are both continuous at (a,b)(a, b), then fxy(a,b)=fyx(a,b)f_{xy}(a, b) = f_{yx}(a, b).
Vol. 2, 5.5 Higher partial derivatives and the equality of mixed partials
Equilibrium Definition
A point x∗x^* where F(x∗)=0F(x^*) = 0. The constant function x(t)=x∗x(t) = x^* is a solution: a particle placed there stays there.
Vol. 2, 7.6 Phase portraits, stability and linearization
Equivalence class Definition
The equivalence class [a][a] of aa is the set of everything related to aa.
Vol. 2, 0.4 Equivalence relations and partitions
Equivalence classes partition the set Theorem
The equivalence classes of an equivalence relation on AA form a partition of AA.
Vol. 2, 0.4 Equivalence relations and partitions
Equivalence relation Definition
A relation that is reflexive, symmetric and transitive: a valid rule for 'the same for our purposes'.
Vol. 2, 0.4 Equivalence relations and partitions
Equivalent forms of one-to-one for linear maps Theorem
For a linear map TT, these are equivalent: one-to-one; invertible with a linear inverse; and N(T)={O}N(T) = \{O\}.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Equivalent norms Definition
Two norms on the same vector space are equivalent if each is at most a constant multiple of the other.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Equivalent norms give the same continuous maps Proposition
If two norms on VV are equivalent, the identity map between the two normed spaces is a bi-Lipschitz homeomorphism, so a map into or out of VV is continuous for one norm iff it is for the other.
Vol. 2, 4.5 Continuity between metric spaces
Equivalent norms give the same open sets Theorem
If two norms on VV are equivalent, a set is open for one iff it is open for the other, so they also have the same closed sets, interiors, closures and boundaries.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Error amplification bound Theorem
If Ax = b and A(x + δx) = b + δb, then ‖δx‖/‖x‖ ≤ κ(A) · ‖δb‖/‖b‖.
Vol. 2, 3.5 Matrix norms, conditioning, and why numerics fail
Error bound for Chebyshev nodes Corollary
With the Chebyshev nodes on [−1,1][-1, 1], ∣f(x)−pn(x)∣≤Mn+12n (n+1)!|f(x) - p_n(x)| \le \dfrac{M_{n+1}}{2^n\,(n+1)!}, and no choice of n+1n+1 nodes makes the factor max⁡∣w∣\max|w| smaller than 2−n2^{-n}.
Vol. 2, 15.1 Numerical analysis
Error bound for equally spaced nodes Corollary
With nodes xj=a+jhx_j = a + jh, h=(b−a)/nh = (b-a)/n, we have ∣w(x)∣≤14hn+1n!|w(x)| \le \tfrac14 h^{n+1} n! on [a,b][a, b], so ∣f(x)−pn(x)∣≤Mn+1 hn+14(n+1)|f(x) - p_n(x)| \le \dfrac{M_{n+1}\,h^{n+1}}{4(n+1)}.
Vol. 2, 15.1 Numerical analysis
Error of the trapezoidal and Simpson rules Theorem
On an interval of width b−ab - a, ∫abf−T=−(b−a)312f′′(η)\int_a^b f - T = -\dfrac{(b-a)^3}{12}f''(\eta) and ∫abf−S=−(b−a)52880f(4)(η)\int_a^b f - S = -\dfrac{(b-a)^5}{2880}f^{(4)}(\eta) for some η∈(a,b)\eta \in (a, b) (a different η\eta in each).
Vol. 2, 15.1 Numerical analysis
Euclid's algorithm Theorem
Repeat 'divide the larger by the smaller and keep the remainder' until the remainder is zero; the last non-zero remainder is the gcd.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Euclid's lemma Lemma
If a prime pp divides a product abab, then pp divides aa or pp divides bb.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Euclid's reduction step Lemma
If a=bq+ra = bq + r then aa and bb have exactly the same common divisors as bb and rr, so gcd⁡(a,b)=gcd⁡(b,r)\gcd(a, b) = \gcd(b, r).
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Euler's formula Theorem
eiθ=cos⁡θ+isin⁡θe^{i\theta} = \cos\theta + i\sin\theta for every real θ\theta.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Euler's formula via power series Theorem
eiθ=cos⁡θ+isin⁡θe^{i\theta} = \cos\theta + i\sin\theta for every real θ\theta, where ez=∑zk/k!e^{z} = \sum z^k/k!.
Vol. 2, 1.6 Series, power series, and uniform convergence
Euler's rotation theorem Theorem
Every 3×3 rotation (orthogonal, det 1) fixes a line through the origin: it is a turn about an axis.
Vol. 2, 3.3 Orthogonal matrices, rotations and reflections
Every complex polynomial splits into linear factors Corollary
A complex polynomial of degree n≥1n \ge 1 equals a(x−r1)(x−r2)⋯(x−rn)a(x - r_1)(x - r_2)\cdots(x - r_n), where aa is its leading coefficient.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Every lower sum is at most every upper sum Corollary
For any two partitions PP and QQ of [a,b][a, b], L(f,P)≤U(f,Q)L(f, P) \le U(f, Q).
Vol. 2, 1.5 The Riemann integral: area as a limit
Every matrix has an SVD Theorem
Every real m×n matrix has a singular value decomposition A = UΣVᵀ.
Vol. 2, 3.4 The singular value decomposition and PCA
Every matrix reduces to reduced row echelon form Theorem
Row operations can turn any matrix into one in reduced row echelon form.
Vol. 2, 2.6 Systems of equations and elimination
Every n-dimensional space is isomorphic to R^n Theorem
If dim⁡V=n\dim V = n and (e1,…,en)(e_1, \dots, e_n) is an ordered basis, then x↦(c1,…,cn)x \mapsto (c_1, \dots, c_n), the coordinates of xx, is an isomorphism V→RnV \to \mathbb R^n.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Exact differential equation Definition
A first-order equation P(x,y) dx+Q(x,y) dy=0P(x, y)\,dx + Q(x, y)\,dy = 0 is exact if (P,Q)(P, Q) is a gradient field; then its solutions are the level curves φ(x,y)=C\varphi(x, y) = C.
Vol. 2, 6.2 Gradient fields and potentials
Exact form Definition
A form ω\omega that is dηd\eta for some form η\eta (for a 1-form: ω=df\omega = df, a gradient).
Vol. 2, 6.7 Differential forms and the one big theorem
Existence and uniqueness for linear equations of order n Theorem
For continuous coefficients and right-hand side on JJ, any t0∈Jt_0 \in J and any numbers c0,…,cn−1c_0, \dots, c_{n-1}, the equation Ly=RLy = R has exactly one solution on all of JJ with y(k)(t0)=cky^{(k)}(t_0) = c_k for k<nk < n.
Vol. 2, 7.2 Linear differential equations
Existence and uniqueness of the interpolating polynomial Theorem
For distinct nodes there is exactly one polynomial of degree at most nn through the given n+1n+1 points, and it is p(x)=∑jyj ℓj(x)p(x) = \sum_j y_j\,\ell_j(x).
Vol. 2, 15.1 Numerical analysis
Expansion by cofactors Theorem
For any row kk: det⁡A=∑j=1nakjCkj\det A = \sum_{j=1}^n a_{kj}C_{kj}. The same holds along any column.
Vol. 2, 2.7 Determinants
Expansion in Legendre polynomials Corollary
PnP_n is orthogonal to every polynomial of degree less than nn. A polynomial ff of degree at most NN equals ∑k=0NckPk\sum_{k=0}^{N}c_kP_k with ck=2k+12∫−11fPk dxc_k = \frac{2k+1}{2}\int_{-1}^{1}fP_k\,dx.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Expectation Definition
The probability-weighted average of the values of XX: E[X]=∑x p(x)E[X] = \sum x\,p(x) for a discrete variable and E[X]=∫xf(x) dxE[X] = \int x f(x)\,dx for one with a density, when these converge absolutely.
Vol. 2, 10.1 Probability as measure
Exponential of a 2 by 2 matrix Theorem
For a 2×22 \times 2 matrix with eigenvalues λ,μ\lambda, \mu: if λ=μ\lambda = \mu, etA=eλt(I+t(A−λI))e^{tA} = e^{\lambda t}\big(I + t(A - \lambda I)\big); if λ≠μ\lambda \ne \mu, etA=eλtI+eλt−eμtλ−μ(A−λI)e^{tA} = e^{\lambda t}I + \frac{e^{\lambda t} - e^{\mu t}}{\lambda - \mu}(A - \lambda I); if λ,μ=a±ib\lambda, \mu = a \pm ib, etA=eat(cos⁡bt I+sin⁡btb(A−aI))e^{tA} = e^{at}\big(\cos bt\,I + \frac{\sin bt}{b}(A - aI)\big).
Vol. 2, 7.4 Systems of equations and the matrix exponential
Exponential of a diagonalizable matrix Theorem
If A=CDC−1A = CDC^{-1} with DD diagonal, then etA=CetDC−1e^{tA} = Ce^{tD}C^{-1}.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Exponential of a rotation-scaling block Theorem
For A=[a−bba]=aI+bJA = \begin{bmatrix}a & -b\\b & a\end{bmatrix} = aI + bJ with J=[0−110]J = \begin{bmatrix}0 & -1\\1 & 0\end{bmatrix}: etA=eat[cos⁡bt−sin⁡btsin⁡btcos⁡bt]e^{tA} = e^{at}\begin{bmatrix}\cos bt & -\sin bt\\\sin bt & \cos bt\end{bmatrix}.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Exponential of a scalar plus a nilpotent matrix Theorem
If A=λI+NA = \lambda I + N with Nk=ON^k = O, then etA=eλt(I+tN+t2N22!+⋯+tk−1Nk−1(k−1)!)e^{tA} = e^{\lambda t}\Big(I + tN + \frac{t^2N^2}{2!} + \dots + \frac{t^{k-1}N^{k-1}}{(k-1)!}\Big).
Vol. 2, 7.4 Systems of equations and the matrix exponential
Extending to a basis Theorem
In an nn-dimensional space, any independent set can be extended to a basis, and any nn independent vectors already form a basis.
Vol. 2, 2.2 Span, independence, basis, dimension
Exterior derivative Definition
The operation dd that raises the degree of a form by one: on a function df=fx dx+fy dy+fz dzdf = f_x\,dx + f_y\,dy + f_z\,dz, and on f dxIf\,dx_I it is df∧dxIdf\wedge dx_I, extended by linearity.
Vol. 2, 6.7 Differential forms and the one big theorem
Extreme value theorem Theorem
A continuous function on a closed bounded interval [a,b][a, b] attains a maximum and a minimum.
Vol. 2, 1.3 Limits and continuity with epsilon and delta
Extreme value theorem on a compact set Theorem
A continuous real function on a non-empty compact set attains a maximum and a minimum.
Vol. 2, 4.3 Compactness
F
Factor theorem for polynomials Corollary
cc is a root of ff exactly when x−cx - c divides ff.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Faraday's law Definition
The circulation of EE round a loop CC equals minus the rate of change of the magnetic flux through a surface bounded by CC: ∮CE⋅dℓ=−ddt∬SB⋅n dS\oint_CE\cdot d\ell = -\dfrac d{dt}\iint_SB\cdot n\,dS, locally ∇×E=−∂tB\nabla\times E = -\partial_tB.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Fermat's little theorem Theorem
If pp is prime and p∤ap \nmid a, then ap−1≡1(modp)a^{p-1} \equiv 1 \pmod p; equivalently ap≡a(modp)a^p \equiv a \pmod p for every integer aa.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Field Definition
A commutative ring where 1 ≠ 0 and every non-zero element has a multiplicative inverse: a number system where you can add, subtract, multiply and divide by anything non-zero.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Finite set Definition
A set is finite with n elements if it can be matched with 1, 2, ..., n by a bijection; the number n is its size.
Vol. 2, 0.3 Sets, functions, and counting infinity
Finitely additive measure Definition
A finitely additive set function on a Boolean algebra that never takes a negative value.
Vol. 2, 10.1 Probability as measure
Finitely additive set function Definition
A function ff that gives a real number f(A)f(A) to each set AA in a family of sets, so that f(A∪B)=f(A)+f(B)f(A \cup B) = f(A) + f(B) whenever AA and BB are disjoint.
Vol. 2, 10.1 Probability as measure
First fundamental theorem for line integrals Theorem
If SS is open and connected, FF is continuous and its line integral is independent of the path, then φ(x)=∫pxF⋅dr\varphi(x) = \int_p^x F \cdot dr (from a fixed base point pp) is a C1C^1 function with ∇φ=F\nabla\varphi = F.
Vol. 2, 6.2 Gradient fields and potentials
First isomorphism theorem for vector spaces Theorem
For a linear map T: V → W, the rule T̄(v + N(T)) = T(v) is a well-defined isomorphism from V/N(T) onto the range of T.
Vol. 2, 3.7 Dual spaces and quotient spaces
First-order equation with constant coefficients Theorem
If a,ba, b are constants, not both 00, then ff satisfies afx+bfy=0af_x + bf_y = 0 if and only if f(x,y)=g(bx−ay)f(x, y) = g(bx - ay) for some differentiable function gg of one variable.
Vol. 2, 5.9 Partial differential equations
Fixed point Definition
A point x∗x^* that TT leaves where it is: Tx∗=x∗T x^* = x^*.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Floating-point number Definition
A number of the form ±m⋅2e\pm m \cdot 2^{e} with an integer mm having at most pp binary digits (the significand) and an exponent ee in a fixed range. Every real number inside the range is rounded to the nearest one.
Vol. 2, 15.1 Numerical analysis
Flux Definition
The flux of a vector field FF through an oriented surface SS with unit normal nn is ∬SF⋅n dS\iint_S F\cdot n\,dS.
Vol. 2, 6.5 Surfaces, area and flux
Flux as a double integral Theorem
If ru×rvr_u\times r_v points the same way as nn, then ∬SF⋅n dS=∬TF(r(u,v))⋅(ru×rv) du dv\iint_S F\cdot n\,dS = \iint_TF(r(u, v))\cdot(r_u\times r_v)\,du\,dv; if it points the opposite way, the right side has the opposite sign.
Vol. 2, 6.5 Surfaces, area and flux
Forms contain the integrals of 6.1 and 6.5 Proposition
For a curve, r∗(P dx+Q dy+R dz)=F(r)⋅r′ dtr^*(P\,dx + Q\,dy + R\,dz) = F(r)\cdot r'\,dt, so ∫Cω\int_C\omega is the line integral. For a surface, r∗(A dy∧dz+B dz∧dx+C dx∧dy)=G(r)⋅(ru×rv) du∧dvr^*(A\,dy\wedge dz + B\,dz\wedge dx + C\,dx\wedge dy) = G(r)\cdot(r_u\times r_v)\,du\wedge dv, so ∬Sω\iint_S\omega is the flux.
Vol. 2, 6.7 Differential forms and the one big theorem
Fourier sine series Definition
The expansion f(x)=∑n≥1bnsin⁡nπxLf(x) = \sum_{n \ge 1}b_n\sin\dfrac{n\pi x}L on [0,L][0, L], with bn=2L∫0Lf(x)sin⁡nπxL dxb_n = \dfrac2L\int_0^Lf(x)\sin\dfrac{n\pi x}L\,dx.
Vol. 2, 5.9 Partial differential equations
Free variable Definition
An unknown whose column has no pivot. You may choose its value freely, and the others follow.
Vol. 2, 2.6 Systems of equations and elimination
Frobenius series Definition
 
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Fubini's theorem for continuous functions on a rectangle Theorem
If ff is continuous on Q=[a,b]×[c,d]Q = [a, b] \times [c, d], then ∬Qf=∫cd ⁣∫abf dx dy=∫ab ⁣∫cdf dy dx\iint_Qf = \int_c^d\!\int_a^bf\,dx\,dy = \int_a^b\!\int_c^df\,dy\,dx.
Vol. 2, 6.3 Multiple integrals
Function Definition
A rule f:A→Bf: A \to B that assigns to every input in AA exactly one output in BB.
Vol. 2, 0.3 Sets, functions, and counting infinity
Functionals on R^n are rows Proposition
Every linear functional on Rn\mathbb R^n is φ(x)=a1x1+⋯+anxn\varphi(x) = a_1x_1 + \dots + a_nx_n with ai=φ(ei)a_i = \varphi(e_i), which is the row [a1 ⋯ an][a_1\ \cdots\ a_n] times the column xx; and every such row gives a functional.
Vol. 2, 3.7 Dual spaces and quotient spaces
Fundamental theorem of algebra Theorem
Every non-constant polynomial with complex coefficients has at least one complex root.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Fundamental theorem of arithmetic Theorem
Every integer greater than 1 is a product of primes, in exactly one way apart from the order of the factors.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Fundamental theorem of calculus Definition
Differentiation and integration undo each other: (1) the derivative of x↦∫axfx \mapsto \int_a^x f is ff, and (2) ∫abF′=F(b)−F(a)\int_a^b F' = F(b) - F(a).
Vol. 2, 1.5 The Riemann integral: area as a limit
Fundamental theorem of calculus, part 1 Theorem
If ff is continuous on [a,b][a, b] and F(x)=∫axfF(x) = \int_a^x f, then F′(x)=f(x)F'(x) = f(x) for every xx.
Vol. 2, 1.5 The Riemann integral: area as a limit
Fundamental theorem of calculus, part 2 Theorem
If FF is continuous on [a,b][a, b], differentiable on (a,b)(a, b), and F′=fF' = f is integrable, then ∫abf=F(b)−F(a)\int_a^b f = F(b) - F(a).
Vol. 2, 1.5 The Riemann integral: area as a limit
Fundamental vector product Definition
For a parametrization r(u,v)r(u, v) the vector N(u,v)=ru×rvN(u, v) = r_u \times r_v. It is normal to the surface and ∥N∥\lVert N\rVert is the area of the image of a unit parameter square. The parametrization is regular where N≠0N \ne 0 and smooth if it is regular everywhere.
Vol. 2, 6.5 Surfaces, area and flux
G
Gauss's law Definition
The flux of EE out of a closed surface SS is the enclosed charge divided by ε0\varepsilon_0: ∬SE⋅n dS=Qenc/ε0\iint_SE\cdot n\,dS = Q_{enc}/\varepsilon_0. Its local form is ∇⋅E=ρ/ε0\nabla\cdot E = \rho/\varepsilon_0.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Gauss's law follows from Coulomb's law Theorem
For charges at points pip_i with values qiq_i and a closed surface SS not passing through any of them, ∬SE⋅n dS=1ε0∑pi insideqi\iint_SE\cdot n\,dS = \frac1{\varepsilon_0}\sum_{p_i\text{ inside}}q_i.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Gcd Definition
The greatest common divisor of aa and bb is the largest positive integer that divides both.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
General solution Definition
The formula y=yp+c1b1+⋯+cnbny = y_p + c_1b_1 + \dots + c_nb_n with arbitrary constants, which lists every solution of Ly=RLy = R.
Vol. 2, 7.2 Linear differential equations
General solution of a linear equation Corollary
If b1,…,bnb_1, \dots, b_n is a basis of ker⁡L\ker L and ypy_p solves Ly=RLy = R, then every solution is y=yp+c1b1+⋯+cnbny = y_p + c_1b_1 + \dots + c_nb_n.
Vol. 2, 7.2 Linear differential equations
Generalized eigenvector Definition
A vector v with (A − λI)^k v = O for some k ≥ 1: killed by A − λI after enough repetitions, though maybe not after one.
Vol. 2, 3.6 Cayley–Hamilton, Schur, and the Jordan form
Generalized Stokes theorem Theorem
If MM is a compact oriented kk-dimensional region with boundary ∂M\partial M carrying the induced orientation and ω\omega is a C1C^1 (k−1)(k-1)-form on a neighbourhood of MM, then ∫∂Mω=∫Mdω\displaystyle\int_{\partial M}\omega = \int_Md\omega.
Vol. 2, 6.7 Differential forms and the one big theorem
Geometric multiplicity is at most algebraic multiplicity Theorem
An eigenvalue never has more independent eigenvectors than its multiplicity as a root: 1≤g(λ0)≤m(λ0)1 \le g(\lambda_0) \le m(\lambda_0).
Vol. 2, 2.8 Eigenvalues and eigenvectors
Geometric series Theorem
∑k=0∞rk=11−r\sum_{k=0}^\infty r^k = \dfrac{1}{1 - r} when ∣r∣<1|r| < 1, and the series diverges when ∣r∣≥1|r| \ge 1.
Vol. 2, 1.6 Series, power series, and uniform convergence
Google matrix Definition
G=dP+1−dn11TG = dP + \tfrac{1-d}{n}\mathbf 1\mathbf 1^{\mathsf T}: with chance dd the surfer follows a link, and with chance 1−d1 - d jumps to a page chosen uniformly at random.
Vol. 2, 2.11 Markov chains and PageRank
Gradient Definition
The gradient ∇f(a)=(D1f(a),…,Dnf(a))\nabla f(a) = (D_1 f(a), \dots, D_n f(a)) is the vector of all the partial derivatives of ff at aa.
Vol. 2, 5.2 Directional derivatives, partial derivatives and the gradient
Gradient descent Definition
The iteration xk+1=xk−η ∇f(xk)x_{k+1} = x_k - \eta\,\nabla f(x_k), which moves from the current point against the gradient by a step proportional to its length.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Gradient descent is a contraction Corollary
If ff is C2C^2 with μI⪯Hf(x)⪯LI\mu I \preceq H_f(x) \preceq LI everywhere on Rn\mathbb R^n and 0<η<2/L0 \lt \eta \lt 2/L, then T(x)=x−η∇f(x)T(x) = x - \eta\nabla f(x) is a contraction with constant ρ=max⁡(∣1−ημ∣,∣1−ηL∣)<1\rho = \max(|1 - \eta\mu|, |1 - \eta L|) \lt 1, so gradient descent converges to the unique minimiser x∗x^* and ∥xk−x∗∥≤ρk1−ρ∥x1−x0∥\lVert x_k - x^*\rVert \le \dfrac{\rho^k}{1 - \rho}\lVert x_1 - x_0\rVert.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Gradient descent near a saddle Proposition
For f=12(ax2−γy2)f = \frac12(ax^2 - \gamma y^2) with a,γ>0a, \gamma \gt 0, gradient descent with step η\eta has yk=(1+ηγ)ky0y_k = (1 + \eta\gamma)^ky_0: it leaves the saddle exponentially fast but with a time of order 1ηγln⁡1∣y0∣\dfrac1{\eta\gamma}\ln\dfrac1{|y_0|}, which is long when the negative curvature γ\gamma is small.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Gradient descent on a convex smooth function Theorem
If ff is convex and LL-smooth with a minimiser x∗x^*, then gradient descent with η=1/L\eta = 1/L satisfies f(xk)−f(x∗)≤L∥x0−x∗∥22kf(x_k) - f(x^*) \le \dfrac{L\lVert x_0 - x^*\rVert^2}{2k}.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Gradient descent on a quadratic Theorem
For f(x)=12xTAx−bTxf(x) = \frac12x^{\mathsf T}Ax - b^{\mathsf T}x with AA symmetric positive definite with eigenvalues in [μ,L][\mu, L], gradient descent converges to x∗=A−1bx^* = A^{-1}b for every start if and only if 0<η<2/L0 \lt \eta \lt 2/L; the error is multiplied by max⁡(∣1−ημ∣,∣1−ηL∣)\max(|1 - \eta\mu|, |1 - \eta L|) per step, which is smallest, equal to κ−1κ+1\frac{\kappa - 1}{\kappa + 1} with κ=L/μ\kappa = L/\mu, at η=2L+μ\eta = \frac2{L + \mu}.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Gradient field Definition
A vector field FF on a set SS is a gradient field if there is a function φ:S→R\varphi: S \to \mathbb R with ∇φ=F\nabla\varphi = F at every point of SS.
Vol. 2, 6.2 Gradient fields and potentials
Gradient inequality for convex functions Theorem
A differentiable convex function lies above each of its tangent planes: f(y)≥f(x)+∇f(x)⋅(y−x)f(y) \ge f(x) + \nabla f(x)\cdot(y - x).
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Gram–Schmidt process Definition
From independent vectors x1,x2,…x_1, x_2, \dots build orthogonal vectors y1,y2,…y_1, y_2, \dots by subtracting from each xkx_k its projections on the earlier yjy_j.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Gram–Schmidt theorem Theorem
The ymy_m are non-zero and orthogonal, and y1,…,ymy_1, \dots, y_m span the same space as x1,…,xmx_1, \dots, x_m for every mm.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Green's theorem Theorem
If CC is a positively oriented piecewise smooth Jordan curve bounding RR, and PP and QQ are C1C^1 on an open set containing RR, then ∮CP dx+Q dy=∬R(Qx−Py) dA\oint_C P\,dx + Q\,dy = \iint_R (Q_x - P_y)\,dA.
Vol. 2, 6.4 Green's theorem and change of variables
Green's theorem for regions with holes Theorem
If C1C_1 is a Jordan curve and C2,…,CnC_2, \dots, C_n are disjoint Jordan curves inside it, all counterclockwise, and RR is the region inside C1C_1 and outside the others, then ∬R(Qx−Py) dA=∮C1−∮C2−⋯−∮Cn\iint_R(Q_x - P_y)\,dA = \oint_{C_1} - \oint_{C_2} - \dots - \oint_{C_n} of P dx+Q dyP\,dx + Q\,dy, for P,QP, Q of class C1C^1 on an open set containing RR.
Vol. 2, 6.4 Green's theorem and change of variables
Green's theorem in normal form Corollary
For a positively oriented Jordan curve CC bounding DD and a C1C^1 planar field F=(P,Q)F = (P, Q), ∮CF⋅n ds=∬D(Px+Qy) dA\oint_CF\cdot n\,ds = \iint_D(P_x + Q_y)\,dA, where nn is the outward unit normal and dsds is arc length.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Group Definition
A set G with an operation that combines any two elements into one, such that: the operation is associative, there is an identity element, and every element has an inverse.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
H
Hamiltonian Definition
The Hermitian matrix HH (or operator) of a quantum system whose eigenvalues are the possible energies. The state obeys the Schrödinger equation iℏ ψ′(t)=Hψ(t)i\hbar\,\psi'(t) = H\psi(t).
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Hamming distance Definition
For two bit strings of the same length, the number of positions where they differ.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Harmonic function Definition
A C2C^2 function uu on an open set that satisfies ∇2u=0\nabla^2u = 0 there.
Vol. 2, 5.9 Partial differential equations
Hartman–Grobman theorem Theorem
Near a hyperbolic equilibrium, a nonlinear system has the same phase portrait as its linearization, up to a continuous change of coordinates that preserves the direction of time.
Vol. 2, 7.6 Phase portraits, stability and linearization
Heat equation Definition
The equation ut=αuxxu_t = \alpha u_{xx} (or ut=α∇2uu_t = \alpha\nabla^2u in several space variables) for the temperature uu of a conducting body, with α>0\alpha \gt 0 the diffusivity.
Vol. 2, 5.9 Partial differential equations
Heat flux Definition
The vector field qq such that the heat crossing a surface per unit time is ∬q⋅n dS\iint q\cdot n\,dS; Fourier's law says q=−κ∇Tq = -\kappa\nabla T for a material of thermal conductivity κ\kappa.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Heine–Borel theorem Theorem
A subset of Rn\mathbb R^n is compact if and only if it is closed and bounded.
Vol. 2, 4.3 Compactness
Hermitian Definition
A complex matrix equal to its conjugate transpose: aij=aji‾a_{ij} = \overline{a_{ji}}.
Vol. 2, 3.1 Symmetric matrices and the spectral theorem
Hessian matrix Definition
The n×nn \times n matrix Hf(a)H_f(a) whose (i,j)(i, j) entry is the second partial derivative DjDif(a)D_jD_if(a) of a scalar field ff at aa.
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
Higher-order partial derivative Definition
A partial derivative of a partial derivative: differentiate ff with respect to one variable, then the result with respect to a variable, and so on kk times; the result is a partial derivative of order kk.
Vol. 2, 5.5 Higher partial derivatives and the equality of mixed partials
Homeomorphism Definition
A homeomorphism is a bijection f:X→Yf : X \to Y such that both ff and f−1f^{-1} are continuous: a one-to-one correspondence that tears and glues nothing, in either direction.
Vol. 2, 4.5 Continuity between metric spaces
Homogeneous and inhomogeneous solution sets Theorem
The solutions of Ly=0Ly = 0 form a vector space. If Ly=RLy = R and RR is not the zero function, the solutions do NOT form a vector space: they are yp+ker⁡Ly_p + \ker L, where ypy_p is any one solution.
Vol. 2, 7.2 Linear differential equations
Homogeneous equation Definition
A linear equation whose right-hand side is zero everywhere: Ly=0Ly = 0. If RR is not zero everywhere the equation is inhomogeneous.
Vol. 2, 7.2 Linear differential equations
Homomorphism Definition
A function φ: G → H between groups with φ(ab) = φ(a)φ(b): doing the operation before or after φ gives the same result.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Homomorphisms preserve identity and inverses Proposition
A homomorphism sends the identity to the identity and inverses to inverses: φ(e) = e and φ(a⁻¹) = φ(a)⁻¹. Its kernel is a subgroup, and φ is one-to-one iff the kernel contains only the identity.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Hyperbolic equilibrium Definition
An equilibrium x∗x^* of x′=F(x)x' = F(x) where no eigenvalue of the Jacobian matrix DF(x∗)DF(x^*) has real part 00.
Vol. 2, 7.6 Phase portraits, stability and linearization
I
Identities for curl and divergence Theorem
Curl and divergence are linear; div⁡(curl⁡F)=0\operatorname{div}(\operatorname{curl}F) = 0 for C2C^2 fields; curl⁡(∇f)=0\operatorname{curl}(\nabla f) = 0 for C2C^2 functions; div⁡(fF)=fdiv⁡F+∇f⋅F\operatorname{div}(fF) = f\operatorname{div}F + \nabla f\cdot F and curl⁡(fF)=fcurl⁡F+∇f×F\operatorname{curl}(fF) = f\operatorname{curl}F + \nabla f\times F.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Identity matrix Definition
The square matrix InI_n with 11 on the diagonal and 00 elsewhere; it is the matrix of the identity map and satisfies IA=AIA = A and AI=AAI = A.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
If and only if Definition
'P if and only if Q' (P⇔QP \Leftrightarrow Q) means both P⇒QP \Rightarrow Q and Q⇒PQ \Rightarrow P.
Vol. 2, 0.1 How to read a theorem
Implication Definition
'If P then Q' (P⇒QP \Rightarrow Q) is false in exactly one case: P true and Q false.
Vol. 2, 0.1 How to read a theorem
Implicit differentiation formulas Corollary
Under the hypotheses of the implicit function theorem: dydx=−FxFy\dfrac{dy}{dx} = -\dfrac{F_x}{F_y}; for F(x,y,z)=0F(x, y, z) = 0, zx=−FxFzz_x = -\dfrac{F_x}{F_z} and zy=−FyFzz_y = -\dfrac{F_y}{F_z}; for two equations in u,vu, v, ux=−∂(F,G)/∂(x,v)∂(F,G)/∂(u,v)u_x = -\dfrac{\partial(F, G)/\partial(x, v)}{\partial(F, G)/\partial(u, v)}.
Vol. 2, 5.7 Inverse and implicit functions
Implicit function Definition
A function gg with F(x,g(x))=0F(x, g(x)) = 0: it is 'defined implicitly' by the equation F(x,y)=0F(x, y) = 0, with no formula given.
Vol. 2, 5.7 Inverse and implicit functions
Implicit function theorem Theorem
If F(x,y)=OF(x, y) = O at (a,b)(a, b), FF is continuously differentiable and the m×mm \times m matrix DyF(a,b)D_yF(a, b) is invertible, then near (a,b)(a, b) the equation defines exactly one y=g(x)y = g(x), it is continuously differentiable, and Dg(x)=−DyF−1DxFDg(x) = -D_yF^{-1}D_xF.
Vol. 2, 5.7 Inverse and implicit functions
Incompressible flow Definition
A flow of constant density ρ0\rho_0 with velocity field vv; mass conservation then gives ∇⋅v=0\nabla\cdot v = 0, so vv is solenoidal and the flux through every closed surface is zero.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Independence of parametrization Theorem
 
Vol. 2, 6.1 Paths and line integrals
Independent columns give a unique least squares solution Theorem
The columns of AA are independent exactly when ATAA^{\mathsf T}A is invertible. Then the unique least squares solution is x^=(ATA)−1ATb\hat x = (A^{\mathsf T}A)^{-1}A^{\mathsf T}b.
Vol. 2, 2.10 Least squares and regression as projection
Independent events Definition
Events AA and BB are independent when P(A∩B)=P(A) P(B)P(A \cap B) = P(A)\,P(B). Several events are mutually independent when this product rule holds for every sub-collection.
Vol. 2, 10.1 Probability as measure
Independent random variables Definition
XX and YY are independent when every event about XX is independent of every event about YY: P(X∈A,Y∈B)=P(X∈A)P(Y∈B)P(X \in A, Y \in B) = P(X \in A)P(Y \in B) for all intervals AA, BB.
Vol. 2, 10.1 Probability as measure
Indicial equation Definition
For x2y′′+xP(x)y′+Q(x)y=0x^2y'' + xP(x)y' + Q(x)y = 0 with P(0)=p0P(0) = p_0 and Q(0)=q0Q(0) = q_0: the quadratic F(s)=s(s−1)+p0s+q0=0F(s) = s(s-1) + p_0s + q_0 = 0. Its roots are the possible starting exponents ss of a Frobenius series.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Induced orientation Definition
If SS is an oriented surface with unit normal nn, its boundary curve ∂S\partial S is given the direction for which, walking along it with your head pointing in the direction of nn, the surface is on your left. This is the right-hand rule: curl the fingers of the right hand along ∂S\partial S and the thumb points along nn.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Infimum Definition
The infimum of SS is its greatest lower bound.
Vol. 2, 1.1 The real numbers and completeness
Initial value problem Definition
An ODE together with the value of the solution (and, for higher order, of its derivatives) at one starting time: y′=f(t,y)y' = f(t, y), y(t0)=y0y(t_0) = y_0.
Vol. 2, 7.1 Existence and uniqueness for differential equations
Injective Definition
ff is injective (one-to-one) if different inputs always give different outputs: f(x)=f(y)f(x) = f(y) forces x=yx = y.
Vol. 2, 0.3 Sets, functions, and counting infinity
Inner product Definition
A rule (x,y)(x, y) giving a real number for every pair of vectors, symmetric, linear, and positive on non-zero vectors. The dot product is the model.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Integrable Definition
ff is (Riemann) integrable if its lower integral sup⁡PL(f,P)\sup_P L(f, P) equals its upper integral inf⁡PU(f,P)\inf_P U(f, P); the common value is ∫abf\int_a^b f.
Vol. 2, 1.5 The Riemann integral: area as a limit
Integral over a type I region Theorem
If SS is type I and ff is continuous on SS, then ff is integrable on SS and ∬Sf=∫ab ⁣∫φ1(x)φ2(x)f(x,y) dy dx\iint_Sf = \int_a^b\!\int_{\varphi_1(x)}^{\varphi_2(x)}f(x, y)\,dy\,dx.
Vol. 2, 6.3 Multiple integrals
Integrals commute with uniform limits on a rectangle Theorem
If fnf_n are integrable on QQ and fn→ff_n \to f uniformly, then ff is integrable and ∬fn→∬f\iint f_n \to \iint f; in fact ∣∬fn−∬f∣≤∥fn−f∥∞ area(Q)|\iint f_n - \iint f| \le \lVert f_n - f \rVert_\infty\,\text{area}(Q).
Vol. 2, 6.3 Multiple integrals
Integrating a uniform limit Theorem
If continuous fn→ff_n \to f uniformly on [a,b][a, b], then ∫abfn→∫abf\int_a^b f_n \to \int_a^b f.
Vol. 2, 1.6 Series, power series, and uniform convergence
Interior Definition
The interior of AA is the set of points of AA that have a ball around them inside AA.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Interior extremum theorem Theorem
If f has a maximum or minimum at an interior point c and is differentiable there, then f'(c) = 0.
Vol. 2, 1.4 The derivative as best linear approximation
Interior, closure and boundary Theorem
int⁡A\operatorname{int} A is the largest open set inside AA; A‾\overline A is the smallest closed set containing AA and equals AA together with its limit points; ∂A=A‾∖int⁡A\partial A = \overline A \setminus \operatorname{int} A.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Intermediate value theorem Theorem
If ff is continuous on [a,b][a, b] and f(a)<0<f(b)f(a) < 0 < f(b), then f(c)=0f(c) = 0 for some cc in (a,b)(a, b).
Vol. 2, 1.3 Limits and continuity with epsilon and delta
Intermediate value theorem from connectedness Corollary
If XX is a connected metric space and f:X→Rf : X \to \mathbb R is continuous, then ff takes every value between any two of its values.
Vol. 2, 4.4 Connectedness and path-connectedness
Interpolating polynomial Definition
Given distinct nodes x0,…,xnx_0, \dots, x_n and values y0,…,yny_0, \dots, y_n, a polynomial pp of degree at most nn with p(xj)=yjp(x_j) = y_j for every jj.
Vol. 2, 15.1 Numerical analysis
Interpolation error formula Theorem
If ff has n+1n+1 continuous derivatives on [a,b][a, b] and pnp_n interpolates it at distinct nodes in [a,b][a, b], then for each xx in [a,b][a, b] there is a point ξ\xi in (a,b)(a, b) with f(x)−pn(x)=f(n+1)(ξ)(n+1)!∏j=0n(x−xj)f(x) - p_n(x) = \dfrac{f^{(n+1)}(\xi)}{(n+1)!}\prod_{j=0}^{n}(x - x_j).
Vol. 2, 15.1 Numerical analysis
Intersection Definition
A∩BA \cap B is the set of everything that is in both AA and BB.
Vol. 2, 0.3 Sets, functions, and counting infinity
Intersections and finite unions of closed sets Corollary
∅\varnothing and XX are closed; any intersection of closed sets is closed; the union of finitely many closed sets is closed.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Interval Definition
A set I⊆RI \subseteq \mathbb R such that whenever x<z<yx < z < y and x,y∈Ix, y \in I, also z∈Iz \in I: it has no holes.
Vol. 2, 4.4 Connectedness and path-connectedness
Invariance of a line integral under deformation Corollary
If Py=QxP_y = Q_x on an open connected set SS and C2C_2 lies inside C1C_1 with the region between them in SS, then ∮C1P dx+Q dy=∮C2P dx+Q dy\oint_{C_1}P\,dx + Q\,dy = \oint_{C_2}P\,dx + Q\,dy, both counterclockwise.
Vol. 2, 6.4 Green's theorem and change of variables
Invariant subspace Definition
A subspace W is invariant under A if A maps W into itself: w in W implies Aw in W.
Vol. 2, 3.6 Cayley–Hamilton, Schur, and the Jordan form
Inverse Definition
A map that undoes TT: a left inverse satisfies S(T(x))=xS(T(x)) = x for every xx, a right inverse satisfies T(R(w))=wT(R(w)) = w for every ww in the range.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Inverse function theorem Theorem
If F:U→RnF: U \to \mathbb R^n is continuously differentiable on an open set UU and det⁡DF(a)≠0\det DF(a) \ne 0, then FF has a continuously differentiable local inverse GG near aa, with DG(F(x))=DF(x)−1DG(F(x)) = DF(x)^{-1}.
Vol. 2, 5.7 Inverse and implicit functions
Inverse matrix Definition
For a square matrix AA, a matrix BB with AB=BA=IAB = BA = I. It is written A−1A^{-1}.
Vol. 2, 2.6 Systems of equations and elimination
Inverse mod n Definition
An inverse of aa mod nn is a number bb with ab≡1(modn)ab \equiv 1 \pmod n; it lets you divide by aa.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Inverse of a 2 by 2 matrix Proposition
[abcd]\begin{bmatrix}a&b\\c&d\end{bmatrix} is invertible exactly when ad−bc≠0ad - bc \ne 0, and then its inverse is 1ad−bc[d−b−ca]\frac{1}{ad - bc}\begin{bmatrix}d&-b\\-c&a\end{bmatrix}.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Inverse of a composition reverses the order Theorem
If SS and TT are invertible, so is STST, and (ST)−1=T−1S−1(ST)^{-1} = T^{-1}S^{-1}.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Inverses mod n exist exactly when coprime Theorem
aa has an inverse mod nn if and only if gcd⁡(a,n)=1\gcd(a, n) = 1; the inverse is unique mod nn and is found by the extended Euclidean algorithm.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Invertible Definition
A function is invertible when it is one-to-one. Its unique left inverse, which is also a right inverse, is the inverse T−1T^{-1}.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Invertible matrix theorem Theorem
For an n×nn \times n matrix AA, eleven conditions are equivalent: invertible, one-to-one, null space zero, independent columns, rank nn, columns span Rn\mathbb R^n, onto, a unique solution for every bb, nn pivots, product of elementary matrices, invertible transpose.
Vol. 2, 2.6 Systems of equations and elimination
Irrotational field Definition
A field with curl 00 everywhere on its domain. A flow with this property is called a potential flow.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Isometry Definition
A linear map that preserves length: ∥Qx∥=∥x∥\lVert Qx \rVert = \lVert x \rVert for every xx.
Vol. 2, 3.3 Orthogonal matrices, rotations and reflections
Isomorphic is an equivalence relation Theorem
Every space is isomorphic to itself, if V≅WV \cong W then W≅VW \cong V, and if V≅WV \cong W and W≅XW \cong X then V≅XV \cong X.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Isomorphism Definition
A linear map between two vector spaces that is one-to-one and onto. Two spaces joined by one are isomorphic: the same space with the vectors renamed.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Iterated integral Definition
∫cd ⁣(∫abf(x,y) dx)dy\int_c^d\!\left(\int_a^b f(x, y)\,dx\right)dy: for each fixed yy integrate in xx from aa to bb to get a number A(y)A(y), then integrate A(y)A(y) in yy from cc to dd.
Vol. 2, 6.3 Multiple integrals
J
J0 solves Bessel's equation of order zero Theorem
The series J0J_0 converges for every real xx and solves x2y′′+xy′+x2y=0x^2y'' + xy' + x^2y = 0. The indicial equation is s2=0s^2 = 0 (a double root), so a second solution contains ln⁡x\ln x.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Jacobian determinant Definition
For a field F:Rn→RnF: \mathbb R^n \to \mathbb R^n with the same number of inputs and outputs, det⁡JF(a)\det J_F(a): the factor by which FF scales small volumes near aa.
Vol. 2, 5.4 The chain rule for fields
Jacobian determinants multiply Corollary
If ff and gg both map Rn\mathbb R^n to Rn\mathbb R^n, then det⁡D(f∘g)(a)=det⁡Df(g(a))⋅det⁡Dg(a)\det D(f \circ g)(a) = \det Df(g(a))\cdot\det Dg(a).
Vol. 2, 5.4 The chain rule for fields
Jacobian matrix Definition
The m×nm \times n matrix JF(a)J_F(a) of partial derivatives whose entry in row ii and column jj is DjFi(a)D_jF_i(a): the matrix of the total derivative.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Jordan block Definition
J_k(λ) is the k×k matrix with λ on the diagonal, 1 directly above it, and 0 elsewhere; it is λI plus a 'push' along a chain.
Vol. 2, 3.6 Cayley–Hamilton, Schur, and the Jordan form
Jordan curve Definition
A closed curve that does not cross or touch itself: α:[a,b]→R2\alpha: [a, b] \to \mathbb R^2 with α(a)=α(b)\alpha(a) = \alpha(b) and α\alpha one-to-one on [a,b)[a, b).
Vol. 2, 6.4 Green's theorem and change of variables
Jordan form Definition
Every complex square matrix is similar to a block-diagonal matrix of Jordan blocks, unique up to the order of the blocks.
Vol. 2, 3.6 Cayley–Hamilton, Schur, and the Jordan form
Jordan normal form theorem Theorem
Every complex square matrix is similar to a Jordan form, unique up to reordering the blocks.
Vol. 2, 3.6 Cayley–Hamilton, Schur, and the Jordan form
K
Kernel of a factor lies in the kernel of the product Fact
If A=A1A2⋯AkA = A_1A_2\cdots A_k are constant-coefficient operators, then ker⁡Aj⊆ker⁡A\ker A_j \subseteq \ker A for every jj.
Vol. 2, 7.2 Linear differential equations
L
Lagrange basis polynomial Definition
ℓj(x)=∏k≠jx−xkxj−xk\ell_j(x) = \prod_{k \ne j} \dfrac{x - x_k}{x_j - x_k}: the degree-nn polynomial that equals 11 at the node xjx_j and 00 at all the other nodes.
Vol. 2, 15.1 Numerical analysis
Lagrange multiplier Definition
A number λi\lambda_i in the equation ∇f(a)=∑iλi∇gi(a)\nabla f(a) = \sum_i\lambda_i\nabla g_i(a); there is one multiplier for each constraint.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Lagrange multiplier theorem Theorem
If f,g1,…,gmf, g_1, \dots, g_m are C1C^1, ff has a local constrained extremum at aa, and aa is a regular point of gg (the gradients ∇gi(a)\nabla g_i(a) are linearly independent), then ∇f(a)=∑λi∇gi(a)\nabla f(a) = \sum\lambda_i\nabla g_i(a) for unique numbers λi\lambda_i.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Lagrange's theorem Theorem
If H is a subgroup of a finite group G, then the order of H divides the order of G: |G| = [G : H] · |H|.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Lagrangian Definition
The field L(x,λ)=f(x)−∑iλi(gi(x)−ci)L(x, \lambda) = f(x) - \sum_i\lambda_i\big(g_i(x) - c_i\big) of n+mn + m variables, whose critical points are exactly the solutions of ∇f=∑λi∇gi\nabla f = \sum\lambda_i\nabla g_i together with the constraints.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Laplace equation Definition
The equation ∇2u=uxx+uyy=0\nabla^2u = u_{xx} + u_{yy} = 0 (or uxx+uyy+uzz=0u_{xx} + u_{yy} + u_{zz} = 0): the steady state of the heat equation.
Vol. 2, 5.9 Partial differential equations
Laplacian Definition
For a scalar field ff the Laplacian is ∇2f=div⁡∇f=fxx+fyy+fzz\nabla^2 f = \operatorname{div}\nabla f = f_{xx} + f_{yy} + f_{zz}.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Law of total probability Theorem
 
Vol. 2, 10.1 Probability as measure
Laws of complex arithmetic Theorem
Addition and multiplication of complex numbers are commutative and associative, multiplication distributes over addition, 1=(1,0)1 = (1, 0) is the identity, and every z≠0z \ne 0 has an inverse.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Learning rate Definition
The step-size multiplier η\eta in gradient descent; in machine learning it is the most important hyperparameter.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Least squares solution Definition
A vector x^\hat x that makes ∥b−Ax^∥\lVert b - A\hat x \rVert as small as possible, even when Ax=bAx = b has no solution.
Vol. 2, 2.10 Least squares and regression as projection
Least squares solutions solve the normal equations Theorem
x^\hat x is a least squares solution of Ax=bAx = b exactly when ATA x^=ATbA^{\mathsf T}A\,\hat x = A^{\mathsf T}b, which says the residual is perpendicular to every column of AA.
Vol. 2, 2.10 Least squares and regression as projection
Lebesgue number lemma Lemma
 
Vol. 2, 4.3 Compactness
Left inverse exists exactly when one-to-one Theorem
A function TT has a left inverse if and only if different inputs always give different outputs.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Left null space Definition
The null space of the transpose: all y∈Rmy \in \mathbb R^m with ATy=OA^{\mathsf T}y = O, equivalently yTA=Oy^{\mathsf T}A = O.
Vol. 2, 2.6 Systems of equations and elimination
Legendre polynomial Definition
The polynomial Pn(x)=12nn!dndxn(x2−1)nP_n(x) = \dfrac{1}{2^n n!}\dfrac{d^n}{dx^n}(x^2 - 1)^n of degree nn (Rodrigues' formula). It solves Legendre's equation with ν=n\nu = n and has Pn(1)=1P_n(1) = 1.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Legendre polynomials solve Legendre's equation Theorem
PnP_n has degree nn and satisfies (1−x2)Pn′′−2xPn′+n(n+1)Pn=0(1 - x^2)P_n'' - 2xP_n' + n(n+1)P_n = 0 and Pn(1)=1P_n(1) = 1.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Length and direction of the cross product Theorem
a×ba \times b is orthogonal to aa and to bb; ∥a×b∥2=∥a∥2∥b∥2−(a⋅b)2\lVert a \times b\rVert^2 = \lVert a\rVert^2\lVert b\rVert^2 - (a\cdot b)^2; so ∥a×b∥=∥a∥∥b∥sin⁡θ\lVert a\times b\rVert = \lVert a\rVert\lVert b\rVert\sin\theta is the area of the parallelogram with sides aa and bb. Also b×a=−a×bb \times a = -a \times b and e1×e2=e3e_1\times e_2 = e_3.
Vol. 2, 6.5 Surfaces, area and flux
Level set Definition
For a scalar field ff and a number cc, the level set L(c)={x:f(x)=c}L(c) = \{x : f(x) = c\}: all points where ff takes the value cc.
Vol. 2, 5.1 Scalar and vector fields, limits and continuity
Level sets near a regular point are graphs Corollary
If aa is a regular point of F:RN→RmF: \mathbb R^N \to \mathbb R^m with F(a)=cF(a) = c, then near aa the level set {F=c}\{F = c\} is the graph of a C1C^1 function of N−mN - m of the coordinates, and its tangent vectors at aa are exactly the vectors in the null space of DF(a)DF(a).
Vol. 2, 5.7 Inverse and implicit functions
Limit cycle Definition
An isolated closed orbit of a planar system: nearby orbits spiral toward it (stable) or away from it (unstable).
Vol. 2, 7.6 Phase portraits, stability and linearization
Limit laws for fields Theorem
If F→bF \to b and G→cG \to c as x→ax \to a, then F+G→b+cF + G \to b + c, λF→λb\lambda F \to \lambda b, F⋅G→b⋅cF \cdot G \to b \cdot c and ∥F∥→∥b∥\lVert F \rVert \to \lVert b \rVert.
Vol. 2, 5.1 Scalar and vector fields, limits and continuity
Limit of a function Definition
 
Vol. 2, 1.3 Limits and continuity with epsilon and delta
Limit of a map between metric spaces Definition
 
Vol. 2, 4.5 Continuity between metric spaces
Limit point Definition
xx is a limit point of AA if every ball around xx contains a point of AA other than xx itself.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Limits are unique Theorem
A sequence cannot converge to two different limits.
Vol. 2, 1.2 Sequences and limits, from zero
Limits in a metric space are unique Theorem
A sequence in a metric space converges to at most one point.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Line integral Definition
For a piecewise smooth path r:[a,b]→Rnr: [a, b] \to \mathbb R^n and a vector field FF continuous on the curve, ∫CF⋅dr=∫abF(r(t))⋅r′(t) dt\int_C F \cdot dr = \int_a^b F(r(t)) \cdot r'(t)\,dt, a sum of one ordinary integral per smooth piece.
Vol. 2, 6.1 Paths and line integrals
Line integral with respect to arc length Definition
For a scalar field φ\varphi and a path rr with continuous r′r', ∫Cφ ds=∫abφ(r(t)) ∥r′(t)∥ dt\int_C \varphi\,ds = \int_a^b \varphi(r(t))\,\lVert r'(t) \rVert\,dt.
Vol. 2, 6.1 Paths and line integrals
Line integrals are linear and additive Proposition
∫C(λF+μG)⋅dr=λ∫CF⋅dr+μ∫CG⋅dr\int_C (\lambda F + \mu G) \cdot dr = \lambda\int_C F \cdot dr + \mu\int_C G \cdot dr, and if CC is C1C_1 followed by C2C_2 then ∫CF⋅dr=∫C1F⋅dr+∫C2F⋅dr\int_C F \cdot dr = \int_{C_1} F \cdot dr + \int_{C_2} F \cdot dr.
Vol. 2, 6.1 Paths and line integrals
Linear combination Definition
A sum of scalar multiples, c1x1+c2x2+⋯+ckxkc_1 x_1 + c_2 x_2 + \dots + c_k x_k.
Vol. 2, 2.2 Span, independence, basis, dimension
Linear combinations of two integers Corollary
ax+by=cax + by = c has an integer solution (x,y)(x, y) exactly when gcd⁡(a,b)\gcd(a, b) divides cc. In particular aa and bb are coprime iff ax+by=1ax + by = 1 is solvable.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Linear differential equation Definition
An equation y(n)+an−1(t)y(n−1)+⋯+a0(t)y=R(t)y^{(n)} + a_{n-1}(t)y^{(n-1)} + \dots + a_0(t)y = R(t), in which the unknown yy and its derivatives each appear to the first power, multiplied only by functions of tt.
Vol. 2, 7.2 Linear differential equations
Linear functional Definition
A linear map from a vector space V to the scalars: it takes a vector and returns a number, and respects sums and multiples.
Vol. 2, 3.7 Dual spaces and quotient spaces
Linear map Definition
A function between vector spaces with T(x+y)=T(x)+T(y)T(x + y) = T(x) + T(y) and T(cx)=c T(x)T(cx) = c\,T(x).
Vol. 2, 2.3 Linear maps, null space, range, rank–nullity
Linear maps form a vector space Theorem
The set L(V,W)L(V, W) of all linear maps from VV to WW is a vector space under pointwise addition and scaling.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Linear systems have solutions on the whole interval Theorem
If A(t)A(t) and g(t)g(t) are continuous on an interval JJ, then x′=A(t)x+g(t)x' = A(t)x + g(t), x(t0)=x0x(t_0) = x_0 has exactly one solution, and it is defined on all of JJ.
Vol. 2, 7.1 Existence and uniqueness for differential equations
Linearity and monotonicity of the integral Theorem
If f,gf, g are integrable and cc is a constant, then f+gf + g and cfcf are integrable, with ∫(f+g)=∫f+∫g\int (f+g) = \int f + \int g, ∫cf=c∫f\int cf = c\int f, and f≤gf \le g implies ∫f≤∫g\int f \le \int g.
Vol. 2, 1.5 The Riemann integral: area as a limit
Linearity of expectation Theorem
For random variables on a countable sample space with finite expectation, E[X+Y]=E[X]+E[Y]E[X + Y] = E[X] + E[Y] and E[aX+b]=aE[X]+bE[aX + b] = aE[X] + b.
Vol. 2, 10.1 Probability as measure
Linearity, additivity and monotonicity of step integrals Theorem
For step functions s,ts, t on the same QQ: ∬(c1s+c2t)=c1∬s+c2∬t\iint(c_1s + c_2t) = c_1\iint s + c_2\iint t; ∬Qs=∬Q1s+∬Q2s\iint_Q s = \iint_{Q_1}s + \iint_{Q_2}s if a line cuts QQ into Q1Q_1 and Q2Q_2; and s≤ts \le t implies ∬s≤∬t\iint s \le \iint t.
Vol. 2, 6.3 Multiple integrals
Linearization Definition
The affine function L(x)=F(a)+F′(a)(x−a)L(x) = F(a) + F'(a)(x - a) that approximates a differentiable field FF near aa.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Linearization and stability Theorem
If every eigenvalue of J=DF(x∗)J = DF(x^*) has negative real part, then x∗x^* is asymptotically stable for the nonlinear system. If some eigenvalue has positive real part, it is unstable.
Vol. 2, 7.6 Phase portraits, stability and linearization
Linearly dependent Definition
Some combination of the vectors equals zero without all coefficients being zero; equivalently, one of them is a combination of the others.
Vol. 2, 2.2 Span, independence, basis, dimension
Linearly independent Definition
The only combination of the vectors equal to zero is the one with every coefficient zero.
Vol. 2, 2.2 Span, independence, basis, dimension
Lipschitz condition Definition
A function f(t,x)f(t, x) satisfies a Lipschitz condition in xx with constant LL if ∥f(t,x)−f(t,z)∥≤L ∥x−z∥\lVert f(t, x) - f(t, z) \rVert \le L\,\lVert x - z \rVert for all tt and all x,zx, z.
Vol. 2, 7.1 Existence and uniqueness for differential equations
Lipschitz implies uniformly continuous Theorem
A Lipschitz map is uniformly continuous, hence continuous.
Vol. 2, 4.5 Continuity between metric spaces
Lipschitz map Definition
f:X→Yf : X \to Y is Lipschitz with constant LL if dY(f(x),f(y))≤L dX(x,y)d_Y(f(x), f(y)) \le L\,d_X(x, y) for all x,yx, y: the output distance is at most LL times the input distance.
Vol. 2, 4.5 Continuity between metric spaces
Local inverse Definition
For a field FF defined near aa, a differentiable field GG defined on a neighbourhood of F(a)F(a) with G(F(x))=xG(F(x)) = x for all xx near aa and F(G(y))=yF(G(y)) = y for all yy near F(a)F(a).
Vol. 2, 5.7 Inverse and implicit functions
Local maximum Definition
A point aa such that f(x)≤f(a)f(x) \le f(a) for all xx in some ball around aa (a relative maximum in Apostol).
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
Local minimum Definition
A point aa such that f(x)≥f(a)f(x) \ge f(a) for all xx in some ball around aa (a relative minimum in Apostol).
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
Loss function Definition
The scalar field ℓ(w)\ell(w) of the parameters ww of a model that measures how badly the model fits the data; training means minimising it.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Low-rank approximation Definition
Keep the first k terms of the SVD sum: A_k = σ₁u₁v₁ᵀ + … + σ_k u_k v_kᵀ, a rank-k matrix close to A.
Vol. 2, 3.4 The singular value decomposition and PCA
Lower sum Definition
L(f,P)=∑i=1nmi ΔxiL(f, P) = \sum_{i=1}^n m_i\,\Delta x_i: the total area of the inner rectangles.
Vol. 2, 1.5 The Riemann integral: area as a limit
Lyapunov function Definition
 
Vol. 2, 7.6 Phase portraits, stability and linearization
Lyapunov's direct method Theorem
If there is a Lyapunov function near x∗x^*, then x∗x^* is stable. If there is a strict one, x∗x^* is asymptotically stable.
Vol. 2, 7.6 Phase portraits, stability and linearization
M
Machine epsilon Definition
The largest relative error from rounding a real number to the nearest floating-point number: about 1.1 × 10⁻¹⁶ in standard double precision.
Vol. 2, 3.5 Matrix norms, conditioning, and why numerics fail
Magnetic field Definition
The vector field BB such that a charge qq moving with velocity vv feels the force qv×Bqv\times B; its flux through every closed surface is 00.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Maps and matrices are the same thing Theorem
For fixed bases, the function T↦m(T)T \mapsto m(T) is an isomorphism from L(V,W)L(V, W) onto Rm×n\mathbb R^{m \times n}.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Markov chain Definition
A process that moves among states, where the chance of the next state depends only on the current state and is given by fixed numbers PijP_{ij}.
Vol. 2, 2.11 Markov chains and PageRank
Markov's inequality Theorem
 
Vol. 2, 10.1 Probability as measure
Matching coefficients Theorem
If a power series ∑cn(x−x0)n\sum c_n(x - x_0)^n equals 00 at every point of an interval around x0x_0, then every coefficient cnc_n is 00.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Mathematical induction Definition
To prove S(n) for every n ≥ 1: prove S(1), and prove that S(k) implies S(k+1) for every k ≥ 1.
Vol. 2, 0.2 Proof techniques
Matrix Definition
A rectangular array of numbers with mm rows and nn columns; aija_{ij} is the entry in row ii and column jj.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Matrix exponential Definition
For a square matrix MM, eM=∑k=0∞Mkk!=I+M+M22!+⋯e^M = \sum_{k=0}^{\infty}\frac{M^k}{k!} = I + M + \frac{M^2}{2!} + \cdots.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Matrix multiplication Definition
For AA of size m×pm \times p and BB of size p×np \times n, ABAB is the m×nm \times n matrix with (AB)ij=∑kaikbkj(AB)_{ij} = \sum_k a_{ik}b_{kj}.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Matrix multiplication is associative and distributive Theorem
A(BC)=(AB)CA(BC) = (AB)C, (A+B)C=AC+BC(A + B)C = AC + BC and C(A+B)=CA+CBC(A + B) = CA + CB whenever the products are defined.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Matrix norm Definition
For this chapter, ∥A∥=∑i,j∣aij∣\lVert A \rVert = \sum_{i,j}\lvert a_{ij}\rvert: the sum of the absolute values of all entries. It is a norm, and it satisfies ∥AB∥≤∥A∥ ∥B∥\lVert AB\rVert \le \lVert A\rVert\,\lVert B\rVert.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Matrix of a composition Theorem
The (i,j)(i, j) entry of m(ST)m(ST) is ∑ksiktkj\sum_{k} s_{ik}t_{kj}: row ii of m(S)m(S) times column jj of m(T)m(T).
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Matrix of a linear map Definition
With bases chosen, the matrix whose column kk is the coordinates of T(ek)T(e_k).
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Matrix space has dimension mn Theorem
The space of m×nm \times n matrices has dimension mnmn.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Matrix times vector Theorem
If xx has coordinates xkx_k, then T(x)T(x) has coordinates yi=∑ktikxky_i = \sum_k t_{ik}x_k, which is x1⋅(column 1)+⋯+xn⋅(column n)x_1 \cdot (\text{column }1) + \dots + x_n \cdot (\text{column }n).
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Matrix times vector is a combination of the columns Theorem
Ax=x1a1+⋯+xnanAx = x_1 a_1 + \dots + x_n a_n, so the column space is the range of x↦Axx \mapsto Ax and the rank of AA is its dimension.
Vol. 2, 2.6 Systems of equations and elimination
Maximum principle for harmonic functions Corollary
If uu is harmonic on a connected open set Ω\Omega and has a maximum (or a minimum) at a point of Ω\Omega, then uu is constant. So a non-constant harmonic function on a bounded region, continuous up to the boundary, attains its largest and smallest values on the boundary only.
Vol. 2, 5.9 Partial differential equations
Maxwell's equations Definition
The four laws: ∇⋅E=ρ/ε0\nabla\cdot E = \rho/\varepsilon_0, ∇⋅B=0\nabla\cdot B = 0, ∇×E=−∂tB\nabla\times E = -\partial_tB, ∇×B=μ0J+μ0ε0∂tE\nabla\times B = \mu_0J + \mu_0\varepsilon_0\partial_tE, together with the force law on a charge, q(E+v×B)q(E + v\times B).
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
Mean value inequality for fields Lemma
If HH is differentiable on a convex set KK and ∥DH(z)∥≤M\lVert DH(z)\rVert \le M for all z∈Kz \in K, then ∥H(x1)−H(x2)∥≤M∥x1−x2∥\lVert H(x_1) - H(x_2)\rVert \le M\lVert x_1 - x_2\rVert for x1,x2∈Kx_1, x_2 \in K.
Vol. 2, 5.7 Inverse and implicit functions
Mean value property of harmonic functions Theorem
If uu is harmonic on an open set containing the closed disc of radius RR about aa, then u(a)=12π∫02πu(a1+Rcos⁡θ, a2+Rsin⁡θ) dθu(a) = \dfrac1{2\pi}\displaystyle\int_0^{2\pi}u\big(a_1 + R\cos\theta,\ a_2 + R\sin\theta\big)\,d\theta: the value at the centre is the average over the circle.
Vol. 2, 5.9 Partial differential equations
Mean value theorem Theorem
If f is continuous on [a, b] and differentiable on (a, b), some c in (a, b) has f'(c) = (f(b) − f(a))/(b − a).
Vol. 2, 1.4 The derivative as best linear approximation
Metric space Definition
A set XX with a distance d(x,y)d(x, y) for each pair of points, never negative, zero only for equal points, symmetric, and obeying the triangle inequality.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Minimal polynomial Definition
The monic polynomial of smallest degree with m(A) = 0; it divides the characteristic polynomial and has the same roots.
Vol. 2, 3.6 Cayley–Hamilton, Schur, and the Jordan form
Minor Definition
The matrix AkjA_{kj} obtained from AA by deleting row kk and column jj.
Vol. 2, 2.7 Determinants
Mixed partial derivative Definition
A higher-order partial derivative in which at least two different variables occur, such as fxyf_{xy} and fyxf_{yx} in two variables.
Vol. 2, 5.5 Higher partial derivatives and the equality of mixed partials
Modulus Definition
The modulus of z=a+biz = a + bi is ∣z∣=a2+b2|z| = \sqrt{a^2 + b^2}, its distance from the origin.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Moment of inertia Definition
The moment of inertia of a wire about an axis LL is IL=∫Cδ2 φ dsI_L = \int_C \delta^2\,\varphi\,ds, where δ\delta is the distance from a point of the wire to LL.
Vol. 2, 6.1 Paths and line integrals
Momentum Definition
The modification xk+1=xk−η∇f(xk)+β(xk−xk−1)x_{k+1} = x_k - \eta\nabla f(x_k) + \beta(x_k - x_{k-1}) that adds a fraction β\beta of the previous step to the gradient step (the heavy-ball method of Polyak).
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Momentum on a quadratic Theorem
For a quadratic with eigenvalues in [μ,L][\mu, L], the heavy-ball method with η=4(L+μ)2\eta = \dfrac4{(\sqrt L + \sqrt\mu)^2} and β=(κ−1κ+1)2\beta = \Big(\dfrac{\sqrt\kappa - 1}{\sqrt\kappa + 1}\Big)^2 makes the error decay at the rate κ−1κ+1\dfrac{\sqrt\kappa - 1}{\sqrt\kappa + 1} (up to a factor polynomial in kk).
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Monotone convergence theorem Theorem
An increasing sequence that is bounded above converges, to the supremum of its terms.
Vol. 2, 1.2 Sequences and limits, from zero
Monotone sequence Definition
A sequence that only goes up (an≤an+1a_n \le a_{n+1}) or only goes down (an≥an+1a_n \ge a_{n+1}).
Vol. 2, 1.2 Sequences and limits, from zero
More vectors than a spanning set means dependent Theorem
If kk vectors span a space, then any k+1k + 1 vectors in that space are linearly dependent.
Vol. 2, 2.2 Span, independence, basis, dimension
Multiplying in polar form Theorem
rcis⁡α⋅scis⁡β=rscis⁡(α+β)r\operatorname{cis}\alpha \cdot s\operatorname{cis}\beta = rs\operatorname{cis}(\alpha + \beta): multiply the lengths and add the angles.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
N
Necessary condition for a gradient Theorem
If F=(f1,…,fn)F = (f_1, \dots, f_n) is C1C^1 on an open set and is a gradient, then ∂fi/∂xj=∂fj/∂xi\partial f_i/\partial x_j = \partial f_j/\partial x_i for all i,ji, j; in the plane, Py=QxP_y = Q_x.
Vol. 2, 6.2 Gradient fields and potentials
Negation Definition
The negation of a statement is the statement that is true exactly when the original is false.
Vol. 2, 0.1 How to read a theorem
Negative Definition
The negative of xx is (−1)x(-1)x, written −x-x. It is the only yy with x+y=Ox + y = O (proved below).
Vol. 2, 2.1 Vector spaces and subspaces
Newton's divided-difference formula Theorem
With pkp_k the interpolant through the first k+1k+1 nodes, pn(x)=∑k=0nf[x0,…,xk] (x−x0)⋯(x−xk−1)p_n(x) = \sum_{k=0}^{n} f[x_0, \dots, x_k]\,(x - x_0)\cdots(x - x_{k-1}), and the divided differences satisfy the quotient recursion in the definition.
Vol. 2, 15.1 Numerical analysis
Newton's method Definition
The iteration xk+1=xk−Hf(xk)−1∇f(xk)x_{k+1} = x_k - H_f(x_k)^{-1}\nabla f(x_k) for minimising ff, which is Newton's method for solving the system ∇f=O\nabla f = O, and jumps to the minimum of the second-order Taylor model at each step.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Newton's method converges quadratically Theorem
If f(r)=0f(r) = 0, f′(xk)≠0f'(x_k) \ne 0 and ff is twice differentiable, then xk+1−r=f′′(ξk)2f′(xk) (xk−r)2x_{k+1} - r = \dfrac{f''(\xi_k)}{2f'(x_k)}\,(x_k - r)^2 for some ξk\xi_k between xkx_k and rr.
Vol. 2, 15.1 Numerical analysis
Newton's method is a local contraction Theorem
 
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Nilpotent matrix Definition
A square matrix NN with Nk=ON^k = O for some kk.
Vol. 2, 7.4 Systems of equations and the matrix exponential
No zero divisors, and the degree of a product Lemma
If zw=0zw = 0 then z=0z = 0 or w=0w = 0; and deg⁡(fg)=deg⁡f+deg⁡g\deg(fg) = \deg f + \deg g for non-zero polynomials.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Node Definition
The origin of x′=Axx' = Ax when AA has real eigenvalues of the same sign, both non-zero: every orbit runs into the origin (a stable node) or out of it (an unstable node), without turning.
Vol. 2, 7.6 Phase portraits, stability and linearization
Noise floor of stochastic gradient descent Theorem
For the loss 1N∑12(w−ai)2\frac1N\sum\frac12(w - a_i)^2, whose minimiser is the mean aˉ\bar a, SGD with a fixed step η∈(0,2)\eta \in (0, 2) has E[wk]−aˉ→0\mathrm{E}[w_k] - \bar a \to 0 but E[(wk−aˉ)2]→ησ22−η\mathrm{E}[(w_k - \bar a)^2] \to \dfrac{\eta\sigma^2}{2 - \eta}, where σ2\sigma^2 is the variance of the aia_i; with steps ηk=1k+1\eta_k = \frac1{k + 1} the iterate is the running average and the error tends to 00.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Norm Definition
The length of a vector, ∥x∥=(x,x)\lVert x\rVert = \sqrt{(x, x)}, defined from the inner product.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Normal and area element of a parametrized surface Theorem
N=ru×rvN = r_u \times r_v is perpendicular to the tangent plane at each regular point, and the area element is dS=∥ru×rv∥ du dvdS = \lVert r_u\times r_v\rVert\,du\,dv.
Vol. 2, 6.5 Surfaces, area and flux
Normal equations Definition
The square system ATA x=ATbA^{\mathsf T}A\,x = A^{\mathsf T}b. Its solutions are exactly the least squares solutions of Ax=bAx = b.
Vol. 2, 2.10 Least squares and regression as projection
Normal mode Definition
A solution of x′′=−Mxx'' = -Mx in which every coordinate oscillates at the same frequency in a fixed pattern: x(t)=cos⁡(ωt−ϕ) vx(t) = \cos(\omega t - \phi)\,v. Then vv is an eigenvector of MM and ω2\omega^2 its eigenvalue.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Normal of a graph Proposition
For the graph z=g(x,y)z = g(x, y) with r(x,y)=(x,y,g(x,y))r(x, y) = (x, y, g(x, y)): rx×ry=(−gx,−gy,1)r_x \times r_y = (-g_x, -g_y, 1), which points upward, and ∥rx×ry∥=1+gx2+gy2\lVert r_x\times r_y\rVert = \sqrt{1 + g_x^2 + g_y^2}.
Vol. 2, 6.5 Surfaces, area and flux
Normal-mode decomposition Theorem
If MM is symmetric positive definite with orthonormal eigenvectors v1,…,vnv_1, \dots, v_n and eigenvalues ωj2\omega_j^2, then every solution of x′′=−Mxx'' = -Mx is x(t)=∑j(ajcos⁡ωjt+bjsin⁡ωjt)vjx(t) = \sum_j\big(a_j\cos\omega_jt + b_j\sin\omega_jt\big)v_j with aj=vj⋅x(0)a_j = v_j\cdot x(0) and bj=vj⋅x′(0)/ωjb_j = v_j\cdot x'(0)/\omega_j.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Normed space Definition
A vector space with a length ∥x∥\lVert x \rVert for every vector that is never negative, zero only for OO, scales by ∣c∣\lvert c \rvert, and obeys the triangle inequality.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Null space Definition
All inputs that TT sends to zero, N(T)={x∈V:T(x)=O}N(T) = \{x \in V : T(x) = O\}. Also called the kernel.
Vol. 2, 2.3 Linear maps, null space, range, rank–nullity
Null space and range are subspaces Theorem
N(T)N(T) is a subspace of the domain and T(V)T(V) is a subspace of the codomain.
Vol. 2, 2.3 Linear maps, null space, range, rank–nullity
Nullity Definition
The dimension of the null space: how many independent directions TT destroys.
Vol. 2, 2.3 Linear maps, null space, range, rank–nullity
O
One is always an eigenvalue of a stochastic matrix Theorem
Every stochastic matrix has eigenvalue 1.
Vol. 2, 2.11 Markov chains and PageRank
One-form Definition
In R3\mathbb R^3 a 1-form is an expression ω=P dx+Q dy+R dz\omega = P\,dx + Q\,dy + R\,dz with functions P,Q,RP, Q, R; at each point it takes a vector vv to the number Pv1+Qv2+Rv3Pv_1 + Qv_2 + Rv_3.
Vol. 2, 6.7 Differential forms and the one big theorem
One-to-one in finite dimension Theorem
For a linear TT on an nn-dimensional VV, these are equivalent: TT is one-to-one; independent sets stay independent; dim⁡T(V)=n\dim T(V) = n; bases go to bases.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Open ball Definition
B(x,r)B(x, r) is the set of all points whose distance from xx is less than rr: the points strictly within rr of xx.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Open balls are open Proposition
Every open ball B(x,r)B(x, r) is an open set.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Open connected sets in R^n are path-connected Theorem
If U⊆RnU \subseteq \mathbb R^n is open and connected, then any two points of UU can be joined by a path in UU.
Vol. 2, 4.4 Connectedness and path-connectedness
Open cover Definition
An open cover of a set KK is a collection of open sets of the space whose union contains KK. A finite subcover is a finite part of the collection that still covers KK.
Vol. 2, 4.3 Compactness
Open set Definition
A set UU is open if every point of UU has an open ball around it that lies completely inside UU.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Open sets inside a subset Lemma
UU is open in AA if and only if U=A∩WU = A \cap W for some open set WW of XX.
Vol. 2, 4.4 Connectedness and path-connectedness
Operator norm Definition
∥A∥=max⁡x≠O∥Ax∥∥x∥\lVert A \rVert = \max_{x \ne O}\frac{\lVert Ax \rVert}{\lVert x \rVert}: the largest factor by which A stretches any vector; for the usual length it equals σ₁.
Vol. 2, 3.5 Matrix norms, conditioning, and why numerics fail
Orbit Definition
The curve in the plane traced out by one solution x(t)x(t) of an autonomous system, without any record of the time.
Vol. 2, 7.6 Phase portraits, stability and linearization
Orbits do not cross Fact
Two orbits of an autonomous system either coincide or never meet. A solution that comes back to its starting point is periodic, and its orbit is a closed curve.
Vol. 2, 7.6 Phase portraits, stability and linearization
Order does not matter for C^k fields Corollary
If ff is of class CkC^k on an open set, then any two partial derivatives of order at most kk that differentiate the same number of times in each variable are equal; in particular the matrix of second partials of a C2C^2 field is symmetric.
Vol. 2, 5.5 Higher partial derivatives and the equality of mixed partials
Order of an element Definition
The order of g is the smallest k ≥ 1 with gᵏ = e (in additive notation k·g = 0), or infinity if there is none.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Ordinary differential equation Definition
An equation for an unknown function y(t)y(t) of ONE variable that involves its derivatives, such as y′=3yy' = 3y or y′′+y=0y'' + y = 0.
Vol. 2, 7.1 Existence and uniqueness for differential equations
Ordinary point Definition
A point x0x_0 is an ordinary point of y′′+py′+qy=0y'' + py' + qy = 0 if both pp and qq are analytic on an interval around x0x_0.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Orientable surface Definition
A surface that admits an orientation. Spheres, cylinders, graphs, tori and flat pieces are orientable; the Moebius strip is not.
Vol. 2, 6.5 Surfaces, area and flux
Oriented surface Definition
A surface together with a continuous choice of unit normal vector nn at every point.
Vol. 2, 6.5 Surfaces, area and flux
Orthogonal Definition
Two vectors are orthogonal when their inner product is 00; a set is orthogonal when every two different members are.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Orthogonal 2 by 2 matrices Theorem
Every 2×2 orthogonal matrix is a rotation R_θ (det 1) or a reflection across a line (det −1).
Vol. 2, 3.3 Orthogonal matrices, rotations and reflections
Orthogonal complement Definition
All vectors orthogonal to every vector of a subspace SS; written S⊥S^\perp ('S perp').
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Orthogonal decomposition theorem Theorem
If SS is a finite-dimensional subspace, every xx splits uniquely as x=s+s⊥x = s + s^\perp with s∈Ss \in S and s⊥∈S⊥s^\perp \in S^\perp, and ∥x∥2=∥s∥2+∥s⊥∥2\lVert x\rVert^2 = \lVert s\rVert^2 + \lVert s^\perp\rVert^2.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Orthogonal matrix Definition
A square real matrix whose columns are orthonormal; equivalently QTQ=IQ^{\mathsf T}Q = I, so Q−1=QTQ^{-1} = Q^{\mathsf T}.
Vol. 2, 3.3 Orthogonal matrices, rotations and reflections
Orthogonal means length-preserving Theorem
For a square real matrix Q, these are equivalent: QᵀQ = I; Q preserves dot products; Q preserves lengths.
Vol. 2, 3.3 Orthogonal matrices, rotations and reflections
Orthogonal sets are independent Theorem
An orthogonal set of non-zero vectors is linearly independent.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Orthogonality of the Legendre polynomials Theorem
∫−11Pm(x)Pn(x) dx=0\int_{-1}^{1}P_m(x)P_n(x)\,dx = 0 for m≠nm \ne n, and ∫−11Pn(x)2 dx=22n+1\int_{-1}^{1}P_n(x)^2\,dx = \dfrac{2}{2n+1}.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Orthogonality of the sine modes Lemma
∫0Lsin⁡nπxLsin⁡mπxL dx=0\displaystyle\int_0^L\sin\frac{n\pi x}L\sin\frac{m\pi x}L\,dx = 0 for n≠mn \ne m and =L2= \frac L2 for n=mn = m; hence if f=∑bmsin⁡mπxLf = \sum b_m\sin\frac{m\pi x}L (finite sum) then bn=2L∫0Lfsin⁡nπxLb_n = \frac2L\int_0^Lf\sin\frac{n\pi x}L.
Vol. 2, 5.9 Partial differential equations
Orthogonally diagonalizable Definition
A=QΛQTA = Q\Lambda Q^{\mathsf T} with Λ\Lambda diagonal and QQ having orthonormal columns: diagonalized by a rotation or reflection of axes.
Vol. 2, 3.1 Symmetric matrices and the spectral theorem
Orthonormal Definition
An orthogonal set in which every vector has length 11.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Other eigenvectors have entries adding to zero Lemma
If Pv=λvPv = \lambda v with λ≠1\lambda \ne 1, the entries of vv add to 00.
Vol. 2, 2.11 Markov chains and PageRank
P
Parametric surface Definition
A surface SS given by a map r(u,v)=(x(u,v), y(u,v), z(u,v))r(u, v) = (x(u, v),\ y(u, v),\ z(u, v)) from a parameter region TT in the uvuv-plane; SS is the set of points r(u,v)r(u, v) with (u,v)(u, v) in TT.
Vol. 2, 6.5 Surfaces, area and flux
Partial derivative Definition
The partial derivative Dkf(a)=f′(a;ek)D_k f(a) = f'(a; e_k) is the derivative of ff along the kk-th coordinate axis: differentiate in xkx_k with every other variable held fixed.
Vol. 2, 5.2 Directional derivatives, partial derivatives and the gradient
Partial derivatives vanish at an interior extremum Theorem
If ff has a local maximum or minimum at an interior point aa and a partial derivative Dkf(a)D_kf(a) exists, then Dkf(a)=0D_kf(a) = 0; so ∇f(a)=O\nabla f(a) = O when all partials exist.
Vol. 2, 5.2 Directional derivatives, partial derivatives and the gradient
Partial differential equation Definition
An equation involving an unknown function of two or more variables and some of its partial derivatives.
Vol. 2, 5.9 Partial differential equations
Partial sum Definition
Sn=a1+a2+⋯+anS_n = a_1 + a_2 + \dots + a_n, the total of the first nn terms.
Vol. 2, 1.6 Series, power series, and uniform convergence
Particular solution Definition
Any single function ypy_p with Lyp=RLy_p = R.
Vol. 2, 7.2 Linear differential equations
Partition Definition
A way of cutting a set into non-empty, non-overlapping pieces (called blocks) that together cover the whole set.
Vol. 2, 0.4 Equivalence relations and partitions
Partition of an interval Definition
A finite list of points a=x0<x1<⋯<xn=ba = x_0 < x_1 < \dots < x_n = b cutting [a,b][a, b] into nn pieces [xi−1,xi][x_{i-1}, x_i].
Vol. 2, 1.5 The Riemann integral: area as a limit
Partitions give equivalence relations Theorem
Given a partition of AA, 'lying in the same block' is an equivalence relation whose classes are exactly the blocks.
Vol. 2, 0.4 Equivalence relations and partitions
Path Definition
A path in a space XX is a continuous map γ\gamma from the interval [0,1][0, 1] into XX: a journey that starts at γ(0)\gamma(0) and ends at γ(1)\gamma(1) without jumping.
Vol. 2, 4.4 Connectedness and path-connectedness
Path independence Definition
The line integral of FF is independent of the path in SS if any two piecewise smooth paths in SS with the same start and the same end give the same value.
Vol. 2, 6.2 Gradient fields and potentials
Path-connected Definition
A space is path-connected if any two of its points are joined by a path inside it.
Vol. 2, 4.4 Connectedness and path-connectedness
Path-connected implies connected Theorem
A path-connected space is connected.
Vol. 2, 4.4 Connectedness and path-connectedness
Peak and final size of an epidemic Theorem
Along every solution of the SIR system, i+s−1R0ln⁡si + s - \dfrac1{R_0}\ln s is constant. Hence the infection peaks when s=1/R0s = 1/R_0 at imax⁡=i0+s0−1+ln⁡(R0s0)R0i_{\max} = i_0 + s_0 - \dfrac{1 + \ln(R_0s_0)}{R_0}, and the epidemic ends with i→0i \to 0 and s→s∞s \to s_\infty where ln⁡s0s∞=R0(s0+i0−s∞)\ln\dfrac{s_0}{s_\infty} = R_0(s_0 + i_0 - s_\infty).
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Peano's refinement of Schwarz's theorem Theorem
If fxf_x, fyf_y and fxyf_{xy} exist on an open set containing (a,b)(a, b) and fxyf_{xy} is continuous at (a,b)(a, b), then fyx(a,b)f_{yx}(a, b) exists and equals fxy(a,b)f_{xy}(a, b).
Vol. 2, 5.5 Higher partial derivatives and the equality of mixed partials
Permutation Definition
A rearrangement of 1,2,…,n1, 2, \dots, n: a list σ(1),…,σ(n)\sigma(1), \dots, \sigma(n) using each number once. Its sign is +1+1 or −1-1 according to whether the number of out-of-order pairs is even or odd.
Vol. 2, 2.7 Determinants
Perpendicular error means closest point Theorem
If pp is in a subspace WW and b−pb - p is perpendicular to all of WW, then pp is the closest point of WW to bb, and no other point of WW is as close.
Vol. 2, 2.10 Least squares and regression as projection
Perron–Frobenius theorem for regular chains Theorem
If some power of the stochastic matrix PP has all entries strictly positive (a regular chain), then 11 is a simple eigenvalue with a positive eigenvector, every other eigenvalue has size less than 1, and Pkx0→πP^kx_0 \to \pi for every probability vector x0x_0.
Vol. 2, 2.11 Markov chains and PageRank
Phase portrait Definition
A sketch of the orbits of an autonomous system in the plane, with arrows for the direction of motion and the equilibria marked.
Vol. 2, 7.6 Phase portraits, stability and linearization
Picard iteration Definition
Start with the constant function y0(t)=x0y_0(t) = x_0 and repeatedly set yk+1(t)=x0+∫t0tf(s,yk(s)) dsy_{k+1}(t) = x_0 + \int_{t_0}^{t} f(s, y_k(s))\,ds.
Vol. 2, 7.1 Existence and uniqueness for differential equations
Picard–Lindelöf theorem Theorem
If ff is continuous and Lipschitz in xx on a rectangle around (t0,x0)(t_0, x_0), the IVP has exactly one solution on a short interval around t0t_0, and Picard iteration converges to it.
Vol. 2, 7.1 Existence and uniqueness for differential equations
Piecewise smooth path Definition
A continuous path r:[a,b]→Rnr: [a, b] \to \mathbb R^n for which there is a finite partition a=t0<⋯<tm=ba = t_0 < \dots < t_m = b such that on each piece [tj−1,tj][t_{j-1}, t_j] the derivative r′r' exists and is continuous.
Vol. 2, 6.1 Paths and line integrals
Pigeonhole principle Theorem
 
Vol. 2, 0.3 Sets, functions, and counting infinity
Pivot Definition
A leading entry of a matrix in echelon form. A column that holds one is a pivot column.
Vol. 2, 2.6 Systems of equations and elimination
Poincare lemma Theorem
On a star-shaped region (such as a ball or all of Rn\mathbb R^n) every closed form of degree ≥1\ge1 is exact.
Vol. 2, 6.7 Differential forms and the one big theorem
Pointwise convergence Definition
fn→ff_n \to f pointwise on DD if for every x∈Dx \in D the numbers fn(x)f_n(x) converge to f(x)f(x).
Vol. 2, 1.6 Series, power series, and uniform convergence
Polar form Definition
Writing a non-zero zz as z=r(cos⁡θ+isin⁡θ)z = r(\cos\theta + i\sin\theta), where r=∣z∣r = |z| and θ\theta is an angle, called an argument of zz.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Polar form of the Laplacian Lemma
If U(r,θ)=u(rcos⁡θ,rsin⁡θ)U(r, \theta) = u(r\cos\theta, r\sin\theta) with uu of class C2C^2, then for r>0r \gt 0: uxx+uyy=Urr+1rUr+1r2Uθθu_{xx} + u_{yy} = U_{rr} + \dfrac1rU_r + \dfrac1{r^2}U_{\theta\theta}.
Vol. 2, 5.9 Partial differential equations
Polynomial Definition
An expression f(x)=anxn+⋯+a1x+a0f(x) = a_nx^n + \dots + a_1x + a_0 with coefficients in R\mathbb R or C\mathbb C.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Polynomial division algorithm Theorem
For polynomials ff and g≠0g \ne 0 there are unique polynomials qq and rr with f=gq+rf = gq + r and either r=0r = 0 or deg⁡r<deg⁡g\deg r < \deg g.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Positive definite Definition
 
Vol. 2, 3.2 Quadratic forms and principal axes
Positive definite iff positive eigenvalues Theorem
A symmetric matrix is positive definite exactly when every eigenvalue is positive.
Vol. 2, 3.2 Quadratic forms and principal axes
Positive orientation Definition
A Jordan curve is positively oriented (counterclockwise) if the region it bounds lies on your left as you walk along it.
Vol. 2, 6.4 Green's theorem and change of variables
Positive semidefinite Hessian implies convex Theorem
If ff is C2C^2 on an open convex set and its Hessian is positive semidefinite everywhere, then ff is convex; in particular 12xTAx−bTx\tfrac12x^{\mathsf T}Ax - b^{\mathsf T}x is convex when AA is symmetric positive semidefinite.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Potential Definition
A potential of FF is a function φ\varphi with ∇φ=F\nabla\varphi = F on the whole domain of FF.
Vol. 2, 6.2 Gradient fields and potentials
Potential energy Definition
If a force field FF has a potential φ\varphi, the potential energy is −φ-\varphi (Apostol's sign convention), so that kinetic plus potential energy stays constant.
Vol. 2, 6.2 Gradient fields and potentials
Power method Definition
Find the dominant eigenvector by starting anywhere and applying the matrix again and again.
Vol. 2, 2.11 Markov chains and PageRank
Power series Definition
A series ∑k=0∞ckxk\sum_{k=0}^\infty c_k x^k whose terms are constants times powers of xx; a polynomial of infinite degree.
Vol. 2, 1.6 Series, power series, and uniform convergence
Power series converge uniformly inside the radius Theorem
If 0<r<R0 < r < R, then ∑ckxk\sum c_k x^k converges uniformly on [−r,r][-r, r], so its sum is continuous on (−R,R)(-R, R).
Vol. 2, 1.6 Series, power series, and uniform convergence
Prescribed values on a basis Theorem
Given a basis e1,…,ene_1, \dots, e_n of VV and ANY vectors u1,…,unu_1, \dots, u_n in WW, there is exactly one linear map TT with T(ek)=ukT(e_k) = u_k.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Prime Definition
A prime is an integer greater than 1 whose only positive divisors are 1 and itself.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Principal axes Definition
The orthonormal eigenvectors of A: the perpendicular directions in which the quadratic form has no cross terms.
Vol. 2, 3.2 Quadratic forms and principal axes
Principal axes theorem Theorem
Rotating to an orthonormal eigenbasis of A turns xTAxx^{\mathsf T}Ax into λ1y12+⋯+λnyn2\lambda_1 y_1^2 + \dots + \lambda_n y_n^2, with no cross terms.
Vol. 2, 3.2 Quadratic forms and principal axes
Principal component analysis Definition
Center the data, take the SVD of the data matrix; the right singular vectors are the directions of greatest variance, in decreasing order.
Vol. 2, 3.4 The singular value decomposition and PCA
Probability density function Definition
A function f≥0f \ge 0 with FX(x)=∫−∞xf(t) dtF_X(x) = \int_{-\infty}^{x} f(t)\,dt for all xx. Then probabilities of intervals are areas under ff.
Vol. 2, 10.1 Probability as measure
Probability mass function Definition
For a random variable that takes only countably many values, p(x)=P(X=x)p(x) = P(X = x). The values p(x)p(x) are non-negative and add to 1.
Vol. 2, 10.1 Probability as measure
Probability measure Definition
A function PP on a sigma-algebra F\mathcal F of subsets of Ω\Omega with P(A)≥0P(A) \ge 0, P(Ω)=1P(\Omega) = 1, and P(A1∪A2∪⋯ )=P(A1)+P(A2)+⋯P(A_1 \cup A_2 \cup \cdots) = P(A_1) + P(A_2) + \cdots for disjoint A1,A2,…A_1, A_2, \dots.
Vol. 2, 10.1 Probability as measure
Product of absolutely convergent series Theorem
If ∑aj\sum a_j and ∑bk\sum b_k converge absolutely, then ∑ncn\sum_n c_n with cn=∑j+k=najbkc_n = \sum_{j+k=n} a_j b_k converges to (∑aj)(∑bk)\left(\sum a_j\right)\left(\sum b_k\right).
Vol. 2, 1.6 Series, power series, and uniform convergence
Product rule for determinants Theorem
det⁡(AB)=det⁡A⋅det⁡B\det(AB) = \det A\cdot\det B for all n×nn \times n matrices.
Vol. 2, 2.7 Determinants
Projection Definition
The SS-part ss of x=s+s⊥x = s + s^\perp: the shadow of xx on the subspace SS.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Projection matrix Definition
The matrix P=A(ATA)−1ATP = A(A^{\mathsf T}A)^{-1}A^{\mathsf T} that sends every bb to the closest point of the column space of AA.
Vol. 2, 2.10 Least squares and regression as projection
Proof by cases Definition
Split the situation into cases that together cover every possibility, and prove the statement in each.
Vol. 2, 0.2 Proof techniques
Proof by contradiction Definition
Assume the statement is false and derive something impossible; then it cannot be false.
Vol. 2, 0.2 Proof techniques
Proof by contrapositive Definition
To prove 'if P then Q', prove 'if not Q then not P' directly; the two statements are equivalent.
Vol. 2, 0.2 Proof techniques
Proof write-up Definition
The finished argument: declared objects, forward steps each with a reason, and a final sentence stating what was proved.
Vol. 2, 0.7 Writing a proof a grader accepts
Properties of a distribution function Theorem
FF is non-decreasing, tends to 0 at minus infinity and to 1 at plus infinity, is continuous from the right, satisfies P(a<X≤b)=F(b)−F(a)P(a < X \le b) = F(b) - F(a), and has P(X=a)=F(a)−F(a−)P(X = a) = F(a) - F(a^-), the size of its jump at aa.
Vol. 2, 10.1 Probability as measure
Properties of a finitely additive measure Theorem
For a finitely additive measure ff: f(A∪B)≤f(A)+f(B)f(A \cup B) \le f(A) + f(B); if A⊆BA \subseteq B then f(B∖A)=f(B)−f(A)f(B \setminus A) = f(B) - f(A) and f(A)≤f(B)f(A) \le f(B); and f(∅)=0f(\varnothing) = 0.
Vol. 2, 10.1 Probability as measure
Properties of the Chebyshev polynomials Theorem
Tn(cos⁡θ)=cos⁡nθT_n(\cos\theta) = \cos n\theta; TnT_n has degree nn and leading coefficient 2n−12^{n-1} (for n≥1n \ge 1); it has nn distinct roots cos⁡(2k+1)π2n\cos\frac{(2k+1)\pi}{2n} in (−1,1)(-1, 1); ∣Tn∣≤1|T_n| \le 1 on [−1,1][-1, 1] and Tn(cos⁡kπn)=(−1)kT_n(\cos\frac{k\pi}n) = (-1)^k.
Vol. 2, 15.1 Numerical analysis
Properties of the exponential series Theorem
E′=EE' = E, S′=CS' = C, C′=−SC' = -S, and E(x+y)=E(x) E(y)E(x + y) = E(x)\,E(y), so E(x)=exE(x) = e^x with e=E(1)=2.71828…e = E(1) = 2.71828\ldots
Vol. 2, 1.6 Series, power series, and uniform convergence
Properties of the norm Theorem
∥x∥≥0\lVert x\rVert \ge 0 with equality only for OO; ∥cx∥=∣c∣∥x∥\lVert cx\rVert = |c|\lVert x\rVert; and the triangle inequality ∥x+y∥≤∥x∥+∥y∥\lVert x + y\rVert \le \lVert x\rVert + \lVert y\rVert.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
Properties preserved by homeomorphisms Theorem
A homeomorphism sends open sets to open sets, convergent sequences to convergent sequences, compact sets to compact sets and connected sets to connected sets, in both directions.
Vol. 2, 4.5 Continuity between metric spaces
Pullback Definition
If φ\varphi is a map from parameters (u,v)(u, v) to (x,y,z)(x, y, z), the pullback φ∗ω\varphi^*\omega of a form ω\omega is obtained by substituting x=x(u,v)x = x(u, v) and so on into the coefficients and dx=xu du+xv dvdx = x_u\,du + x_v\,dv into the basic forms, then expanding with the wedge rules.
Vol. 2, 6.7 Differential forms and the one big theorem
Pullback commutes with d Proposition
For a C2C^2 map φ\varphi and a form ω\omega, φ∗(dω)=d(φ∗ω)\varphi^*(d\omega) = d(\varphi^*\omega).
Vol. 2, 6.7 Differential forms and the one big theorem
Putzer's method Theorem
With eigenvalues λ1,…,λn\lambda_1, \dots, \lambda_n listed with multiplicity and P0=IP_0 = I, Pk=(A−λ1I)⋯(A−λkI)P_k = (A - \lambda_1I)\cdots(A - \lambda_kI), one has etA=∑k=0n−1rk+1(t)Pke^{tA} = \sum_{k=0}^{n-1}r_{k+1}(t)P_k, where r1′=λ1r1r_1' = \lambda_1r_1, r1(0)=1r_1(0) = 1 and rk+1′=λk+1rk+1+rkr_{k+1}' = \lambda_{k+1}r_{k+1} + r_k, rk+1(0)=0r_{k+1}(0) = 0.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Q
QR from Gram–Schmidt Theorem
A matrix AA with independent columns factors as A=QRA = QR: QQ has orthonormal columns and RR is square, upper triangular and invertible. Then x^\hat x solves Rx^=QTbR\hat x = Q^{\mathsf T}b and P=QQTP = QQ^{\mathsf T}.
Vol. 2, 2.10 Least squares and regression as projection
Quadratic convergence of Newton's method Theorem
If F(x∗)=OF(x^*) = O, JF(x∗)J_F(x^*) is invertible with ∥JF(x∗)−1∥≤β0\lVert J_F(x^*)^{-1}\rVert \le \beta_0 and JFJ_F is MM-Lipschitz near x∗x^*, then for ∥x0−x∗∥≤12β0M\lVert x_0 - x^*\rVert \le \dfrac1{2\beta_0M} the Newton iterates satisfy ∥xk+1−x∗∥≤β0M∥xk−x∗∥2\lVert x_{k+1} - x^*\rVert \le \beta_0M\lVert x_k - x^*\rVert^2: the number of correct digits doubles at each step.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Quadratic form Definition
A function q(x)=xTAx=∑i,jaijxixjq(x) = x^{\mathsf T}Ax = \sum_{i,j} a_{ij}x_ix_j with AA symmetric: a sum of squares and cross terms.
Vol. 2, 3.2 Quadratic forms and principal axes
Quadrature rule Definition
An approximation ∫abf≈∑jwjf(xj)\int_a^b f \approx \sum_j w_j f(x_j) by a weighted sum of values at chosen nodes. Integrating the interpolating polynomial gives one.
Vol. 2, 15.1 Numerical analysis
Quality factor Definition
Q=ω0LR=1RLCQ = \dfrac{\omega_0L}{R} = \dfrac1R\sqrt{\dfrac LC} for a series RLC circuit: the ratio of the resonant frequency to the width of the resonance peak.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Quantifier Definition
'For every' (∀\forall) and 'there exists' (∃\exists): they say how many objects a predicate is claimed for.
Vol. 2, 0.1 How to read a theorem
Quotient space Definition
V/U is the set of all cosets of U, with (v + U) + (w + U) = (v + w) + U and c(v + U) = cv + U; it is the vector space of V with U collapsed to a point.
Vol. 2, 3.7 Dual spaces and quotient spaces
R
R^n is complete Theorem
Rn\mathbb R^n with the 1-, 2- or max-distance is complete.
Vol. 2, 4.2 Convergence, completeness and the contraction mapping theorem
Radius of convergence Definition
 
Vol. 2, 1.6 Series, power series, and uniform convergence
Random variable Definition
A function XX from the sample space to the real numbers such that each event 'X is at most x' is in the sigma-algebra, so that it has a probability.
Vol. 2, 10.1 Probability as measure
Range Definition
All outputs of TT, T(V)={T(x):x∈V}T(V) = \{T(x) : x \in V\}. Also called the image.
Vol. 2, 2.3 Linear maps, null space, range, rank–nullity
Rank Definition
The dimension of the range: how many independent directions survive in the output.
Vol. 2, 2.3 Linear maps, null space, range, rank–nullity
Rank equals the number of pivots Theorem
If an echelon form of AA has rr pivots, then rank A=rA = r, nullity =n−r= n - r, and the pivot columns of the original AA are a basis of the column space.
Vol. 2, 2.6 Systems of equations and elimination
Rank–nullity from the first isomorphism theorem Corollary
dim V − dim N(T) = dim V/N(T) = dim range T, which is rank–nullity.
Vol. 2, 3.7 Dual spaces and quotient spaces
Rank–nullity theorem Theorem
For a linear map out of a finite-dimensional space, dim⁡V=rank⁡T+nullity⁡T\dim V = \operatorname{rank} T + \operatorname{nullity} T.
Vol. 2, 2.3 Linear maps, null space, range, rank–nullity
Rate of change along a curve Theorem
If rr is differentiable at tt and ff is differentiable at r(t)r(t), then g(t)=f(r(t))g(t) = f(r(t)) has g′(t)=∇f(r(t))⋅r′(t)g'(t) = \nabla f(r(t))\cdot r'(t).
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Ratio formula for the radius Theorem
If ck≠0c_k \ne 0 and ∣ck+1ck∣→L\left|\frac{c_{k+1}}{c_k}\right| \to L, then R=1LR = \frac1L (with R=∞R = \infty if L=0L = 0 and R=0R = 0 if L=∞L = \infty).
Vol. 2, 1.6 Series, power series, and uniform convergence
Ratio test Theorem
 
Vol. 2, 1.6 Series, power series, and uniform convergence
Reading the solutions off the reduced form Theorem
The system is inconsistent exactly when the last column is a pivot column. Otherwise each pivot variable equals its right side minus a combination of the free variables.
Vol. 2, 2.6 Systems of equations and elimination
Real and imaginary parts of a complex solution Theorem
If AA is real and Av=λvAv = \lambda v with λ=a+ib\lambda = a + ib, b≠0b \ne 0, and v=u+iwv = u + iw with u,wu, w real vectors, then x1=eat(cos⁡bt u−sin⁡bt w)x_1 = e^{at}(\cos bt\,u - \sin bt\,w) and x2=eat(sin⁡bt u+cos⁡bt w)x_2 = e^{at}(\sin bt\,u + \cos bt\,w) are two independent real solutions of x′=Axx' = Ax.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Real polynomials factor into real linear and quadratic factors Corollary
Every polynomial with real coefficients and degree at least 1 is a constant times a product of real polynomials of degree 1 or 2.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Real solutions from complex roots Theorem
If AA has real coefficients and r=α+iβr = \alpha + i\beta (β≠0\beta \ne 0) is a root of multiplicity mm, then so is rˉ\bar r, and the 2m2m functions tjeαtcos⁡βtt^je^{\alpha t}\cos\beta t and tjeαtsin⁡βtt^je^{\alpha t}\sin\beta t (0≤j<m0 \le j < m) replace the 2m2m complex solutions tjertt^je^{rt} and tjerˉtt^je^{\bar rt}.
Vol. 2, 7.2 Linear differential equations
Rearranging an absolutely convergent series Theorem
If ∑ak\sum a_k converges absolutely, every rearrangement converges to the same sum.
Vol. 2, 1.6 Series, power series, and uniform convergence
Recurrence for Legendre's equation Theorem
Series solutions y=∑anxny = \sum a_nx^n of Legendre's equation satisfy an+2=(n−ν)(n+ν+1)(n+1)(n+2) ana_{n+2} = \dfrac{(n-\nu)(n+\nu+1)}{(n+1)(n+2)}\,a_n. They converge for ∣x∣<1\lvert x \rvert < 1, and they stop (are polynomials) when ν\nu is an integer of the right parity.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Reduced row echelon form Definition
Echelon form where every pivot is 1 and is the only non-zero entry in its column.
Vol. 2, 2.6 Systems of equations and elimination
Refinement lemma Lemma
Adding cut points to a partition can only raise the lower sum and lower the upper sum.
Vol. 2, 1.5 The Riemann integral: area as a limit
Regular point Definition
For F:RN→RmF: \mathbb R^N \to \mathbb R^m with m<Nm \lt N, a point aa where the Jacobian DF(a)DF(a) has rank mm: the mm gradients ∇F1(a),…,∇Fm(a)\nabla F_1(a), \dots, \nabla F_m(a) are linearly independent.
Vol. 2, 5.7 Inverse and implicit functions
Regular singular point Definition
A singular point x0x_0 of y′′+py′+qy=0y'' + py' + qy = 0 where (x−x0)p(x)(x - x_0)p(x) and (x−x0)2q(x)(x - x_0)^2q(x) are analytic. Any other singular point is irregular.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Relation Definition
A relation on a set AA is a rule that says, for each ordered pair (a,b)(a, b), whether aa is related to bb; formally, a subset of A×AA \times A.
Vol. 2, 0.4 Equivalence relations and partitions
Remainder theorem for polynomials Corollary
Dividing ff by x−cx - c leaves the constant remainder f(c)f(c).
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Reparametrization Definition
 
Vol. 2, 6.1 Paths and line integrals
Riemann–Darboux criterion Theorem
 
Vol. 2, 1.5 The Riemann integral: area as a limit
Ring Definition
A set with addition and multiplication where addition makes it an abelian group, multiplication is associative with an identity 1, and multiplication distributes over addition.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
RLC circuit Definition
A loop with a resistor RR, an inductor LL, a capacitor CC and a source E(t)E(t). The charge qq on the capacitor satisfies Lq′′+Rq′+qC=E(t)Lq'' + Rq' + \dfrac qC = E(t).
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Root Definition
A root of ff is a number cc with f(c)=0f(c) = 0.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Rotation matrix Definition
Rθ=[cos⁡θ−sin⁡θsin⁡θcos⁡θ]R_\theta = \begin{bmatrix}\cos\theta & -\sin\theta\\ \sin\theta & \cos\theta\end{bmatrix} turns the plane counterclockwise by θ.
Vol. 2, 3.3 Orthogonal matrices, rotations and reflections
Row echelon form Definition
A staircase shape: zero rows at the bottom, and the first non-zero entry of each row is further right than the first non-zero entry of the row above.
Vol. 2, 2.6 Systems of equations and elimination
Row operations Definition
The three allowed moves on the rows of a matrix: swap two rows, multiply a row by a non-zero number, add a multiple of one row to another row.
Vol. 2, 2.6 Systems of equations and elimination
Row operations are multiplication by elementary matrices Theorem
Doing a row operation to AA gives the same result as multiplying AA on the left by the elementary matrix of that operation. Elementary matrices are invertible, with elementary inverses.
Vol. 2, 2.6 Systems of equations and elimination
Row operations do not change the solutions Theorem
If [A′∣b′][A' \mid b'] comes from [A∣b][A \mid b] by row operations, the two systems have exactly the same solutions.
Vol. 2, 2.6 Systems of equations and elimination
Row rank equals column rank Theorem
The row space and the column space of a matrix have the same dimension, the number of pivots. So rank AA = rank ATA^{\mathsf T}.
Vol. 2, 2.6 Systems of equations and elimination
Row rank equals column rank, by duality Corollary
rank Tᵀ = rank T, so a matrix and its transpose have the same rank.
Vol. 2, 3.7 Dual spaces and quotient spaces
Row space Definition
The span of the rows of AA, which is the column space of the transpose ATA^{\mathsf T}.
Vol. 2, 2.6 Systems of equations and elimination
RSA decryption works Theorem
If n=pqn = pq for distinct primes and ed≡1(mod(p−1)(q−1))ed \equiv 1 \pmod{(p-1)(q-1)}, then (me)d≡m(modn)(m^e)^d \equiv m \pmod n for every integer mm.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Rules for conjugates Proposition
zzˉ=∣z∣2z\bar z = |z|^2, z+w‾=zˉ+wˉ\overline{z + w} = \bar z + \bar w, zw‾=zˉ wˉ\overline{zw} = \bar z\,\bar w, and z−1=zˉ/∣z∣2z^{-1} = \bar z / |z|^2.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
Rules for negating Fact
Not(and) is or-of-nots; not(or) is and-of-nots; not(if P then Q) is P and not Q; not(for all) is exists-not; not(exists) is for-all-not.
Vol. 2, 0.1 How to read a theorem
Rules for not in Fact
Not in an intersection means missing from at least one; not in a union means missing from both; not in a complement means in the original set.
Vol. 2, 0.3 Sets, functions, and counting infinity
S
Saddle Definition
The origin of x′=Axx' = Ax when AA has two real eigenvalues of opposite signs: orbits come in along one eigendirection and leave along the other.
Vol. 2, 7.6 Phase portraits, stability and linearization
Saddle point Definition
A critical point aa such that every ball around aa contains points where ff is larger than f(a)f(a) and points where it is smaller.
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
Same dimension exactly when isomorphic Theorem
Two finite-dimensional vector spaces are isomorphic if and only if they have the same dimension.
Vol. 2, 2.4 Inverses, one-to-one maps, isomorphism
Same value is an equivalence relation Proposition
For any function f:A→Bf: A \to B, the relation a∼ba \sim b iff f(a)=f(b)f(a) = f(b) is an equivalence relation on AA.
Vol. 2, 0.4 Equivalence relations and partitions
Scalar Definition
A number you multiply vectors by. In this book it is a real number unless we say complex.
Vol. 2, 2.1 Vector spaces and subspaces
Scalar field Definition
A function ff that gives a real number f(x)=f(x1,…,xn)f(x) = f(x_1, \dots, x_n) at each point xx of a set S⊆RnS \subseteq \mathbb R^n.
Vol. 2, 5.1 Scalar and vector fields, limits and continuity
Scaling a direction scales the derivative Lemma
If f′(a;y)f'(a; y) exists then f′(a;cy)=c f′(a;y)f'(a; cy) = c\,f'(a; y) for every real cc.
Vol. 2, 5.2 Directional derivatives, partial derivatives and the gradient
Scaling by zero Theorem
0x=O0x = O for every vector xx.
Vol. 2, 2.1 Vector spaces and subspaces
Schur decomposition Definition
A = UTU* with U unitary and T upper triangular: every complex matrix is triangular in a suitable orthonormal basis.
Vol. 2, 3.6 Cayley–Hamilton, Schur, and the Jordan form
Schur's theorem Theorem
Every complex square matrix has a Schur decomposition A = UTU*.
Vol. 2, 3.6 Cayley–Hamilton, Schur, and the Jordan form
Scratch work Definition
The private search for a proof: any order, any guesses, often working backwards from the goal.
Vol. 2, 0.7 Writing a proof a grader accepts
Second derivative along a path Theorem
If rr is twice differentiable and ff has continuous second partials, then d2dt2f(r(t))=∑i,jDjDif(r(t)) ri′(t) rj′(t)+∇f(r(t))⋅r′′(t)\dfrac{d^2}{dt^2}f(r(t)) = \sum_{i,j} D_jD_if(r(t))\,r_i'(t)\,r_j'(t) + \nabla f(r(t))\cdot r''(t).
Vol. 2, 5.4 The chain rule for fields
Second derivatives of a composite field Theorem
If h=f∘gh = f \circ g with ff a scalar field and g:Rp→Rng: \mathbb R^p \to \mathbb R^n, all C2C^2, then the matrix of second partials of hh is Dg(a)T [DlDkf(b)] Dg(a)+∑k=1nDkf(b) [DjDigk(a)]Dg(a)^{\mathsf T}\,[D_lD_kf(b)]\,Dg(a) + \sum_{k=1}^n D_kf(b)\,[D_jD_ig_k(a)].
Vol. 2, 5.4 The chain rule for fields
Second fundamental theorem for line integrals Theorem
If F=∇φF = \nabla\varphi on an open set SS with φ\varphi of class C1C^1, then for any piecewise smooth path r:[a,b]→Sr: [a, b] \to S, ∫rF⋅dr=φ(r(b))−φ(r(a))\int_r F \cdot dr = \varphi(r(b)) - \varphi(r(a)).
Vol. 2, 6.2 Gradient fields and potentials
Second-order Taylor formula for scalar fields Theorem
If ff is C2C^2 on a ball B(a,r)B(a, r) and ∥v∥<r\lVert v \rVert < r, then f(a+v)=f(a)+∇f(a)⋅v+12vTHf(a+cv) vf(a + v) = f(a) + \nabla f(a)\cdot v + \frac12v^{\mathsf T}H_f(a + cv)\,v for some c∈(0,1)c \in (0, 1), and also f(a+v)=f(a)+∇f(a)⋅v+12vTHf(a) v+∥v∥2E2(a,v)f(a + v) = f(a) + \nabla f(a)\cdot v + \frac12v^{\mathsf T}H_f(a)\,v + \lVert v \rVert^2E_2(a, v) with E2(a,v)→0E_2(a, v) \to 0 as v→Ov \to O.
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
Second-order test for constrained extrema Theorem
At a regular point with multipliers λi\lambda_i: if vTHv>0v^{\mathsf T}Hv \gt 0 for all nonzero vv in the tangent space then aa is a strict local constrained minimum; if <0\lt 0, a strict local maximum; a local minimum forces vTHv≥0v^{\mathsf T}Hv \ge 0 on the tangent space.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
Separation Definition
A separation of a set AA is a way of writing A=U∪VA = U \cup V with UU and VV disjoint, non-empty, and both open in AA.
Vol. 2, 4.4 Connectedness and path-connectedness
Separation of variables Definition
The method of looking for solutions of a PDE that are products of functions of one variable each, such as u=X(x)T(t)u = X(x)T(t), which turns the PDE into ordinary differential equations.
Vol. 2, 5.9 Partial differential equations
Sequence Definition
An infinite list of real numbers a1,a2,a3,…a_1, a_2, a_3, \dots; formally a function from the natural numbers to the reals.
Vol. 2, 1.2 Sequences and limits, from zero
Sequential criterion for continuity Theorem
ff is continuous at aa if and only if xn→ax_n \to a always implies f(xn)→f(a)f(x_n) \to f(a).
Vol. 2, 1.3 Limits and continuity with epsilon and delta
Sequentially compact Definition
A set KK is sequentially compact if every sequence of points of KK has a subsequence that converges to a point of KK.
Vol. 2, 4.3 Compactness
Sequentially compact implies totally bounded Lemma
A sequentially compact metric space can be covered by finitely many balls of any given radius.
Vol. 2, 4.3 Compactness
Sequentially compact sets are closed and bounded Theorem
In any metric space, a sequentially compact set is closed and bounded.
Vol. 2, 4.3 Compactness
Series Definition
An infinite sum ∑k=1∞ak\sum_{k=1}^\infty a_k, defined as the limit of the partial sums when that limit exists.
Vol. 2, 1.6 Series, power series, and uniform convergence
Series solutions at an ordinary point Theorem
If pp and qq are analytic on (x0−r,x0+r)(x_0 - r, x_0 + r), then y′′+py′+qy=0y'' + py' + qy = 0 has two independent solutions that are power series in x−x0x - x_0 converging on the whole interval. The coefficients come from a recurrence, with a0a_0 and a1a_1 free.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Set Definition
A collection of objects, called its elements; what matters is only which objects are in it.
Vol. 2, 0.3 Sets, functions, and counting infinity
Shape of a particular solution Theorem
If R=q(t)ertR = q(t)e^{rt} with qq a polynomial of degree dd and rr is a root of PLP_L of multiplicity ss (s=0s = 0 if rr is not a root), then Ly=RLy = R has a particular solution yp=ts h(t) erty_p = t^s\,h(t)\,e^{rt} with hh a polynomial of degree at most dd.
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Shape of the characteristic polynomial Theorem
det⁡(λI−A)=λn−(tr⁡A)λn−1+⋯+(−1)ndet⁡A\det(\lambda I - A) = \lambda^n - (\operatorname{tr} A)\lambda^{n-1} + \dots + (-1)^n\det A.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Shifting an exponential Fact
For a polynomial pp and a number rr: (D−r)(p(t)ert)=p′(t) ert(D - r)\big(p(t)e^{rt}\big) = p'(t)\,e^{rt}.
Vol. 2, 7.2 Linear differential equations
Sigma-algebra Definition
A family F\mathcal F of subsets of Ω\Omega that contains Ω\Omega, the complement of each member, and the union of any countable list of members.
Vol. 2, 10.1 Probability as measure
Similar matrices Definition
Matrices AA and BB with B=C−1ACB = C^{-1}AC for some invertible CC; equivalently, two descriptions of the same map in different bases.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Similar matrices share a characteristic polynomial Theorem
If B=C−1ACB = C^{-1}AC then BB and AA have the same characteristic polynomial, hence the same eigenvalues, trace and determinant.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Simply connected set Definition
An open connected set in the plane is simply connected if it has no holes: every simple closed curve in it encloses a region lying entirely inside the set.
Vol. 2, 6.2 Gradient fields and potentials
Simpson's rule Definition
S=b−a6(f(a)+4f(m)+f(b))S = \dfrac{b-a}{6}\big(f(a) + 4f(m) + f(b)\big) with m=a+b2m = \frac{a+b}2: the integral of the quadratic interpolant at aa, mm, bb.
Vol. 2, 15.1 Numerical analysis
Singular point Definition
A point that is not an ordinary point of y′′+py′+qy=0y'' + py' + qy = 0: pp or qq fails to be analytic there, usually because it is infinite.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
Singular value Definition
The singular values of A are the square roots of the eigenvalues of AᵀA, listed from largest to smallest: the stretch factors of A.
Vol. 2, 3.4 The singular value decomposition and PCA
Singular value decomposition Definition
A = UΣVᵀ with U (m×m) and V (n×n) orthogonal and Σ (m×n) diagonal with σ₁ ≥ σ₂ ≥ … ≥ 0.
Vol. 2, 3.4 The singular value decomposition and PCA
SIR model Definition
The system s′=−βsis' = -\beta si, i′=βsi−γii' = \beta si - \gamma i, r′=γir' = \gamma i for the fractions of susceptible, infected and recovered people.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Solenoidal field Definition
A field with divergence 00 everywhere on its domain; a flow with this property is incompressible.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Solid region Definition
A bounded region EE of space with non-empty interior whose boundary ∂E\partial E is a piecewise smooth surface.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Solution of the linear system Theorem
The IVP x′=Axx' = Ax, x(a)=bx(a) = b has the unique solution x(t)=e(t−a)Abx(t) = e^{(t-a)A}b, defined for all real tt.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Solutions are a particular solution plus the null space Theorem
If xpx_p solves Ax=bAx = b, then the solutions are exactly xp+yx_p + y with yy in the null space of AA.
Vol. 2, 2.6 Systems of equations and elimination
Span Definition
The set of all linear combinations of the given vectors: everything they can build.
Vol. 2, 2.2 Span, independence, basis, dimension
Spectral theorem Theorem
Every real symmetric matrix is orthogonally diagonalizable: A=QΛQTA = Q\Lambda Q^{\mathsf T}, with real eigenvalues and an orthonormal basis of eigenvectors.
Vol. 2, 3.1 Symmetric matrices and the spectral theorem
Spiral Definition
 
Vol. 2, 7.6 Phase portraits, stability and linearization
Squeeze for fields Proposition
If ∥F(x)−b∥≤φ(∥x−a∥)\lVert F(x) - b \rVert \le \varphi(\lVert x - a \rVert) near aa and φ(r)→0\varphi(r) \to 0 as r→0+r \to 0^+, then F(x)→bF(x) \to b.
Vol. 2, 5.1 Scalar and vector fields, limits and continuity
Stability of a linear system Theorem
For x′=Axx' = Ax with AA real n×nn \times n: the origin is asymptotically stable if every eigenvalue has negative real part (and then ∥etA∥≤Ce−μt\lVert e^{tA}\rVert \le Ce^{-\mu t}); unstable if some eigenvalue has positive real part. If all real parts are ≤0\le 0 it is stable exactly when every eigenvalue with real part 00 has only 1×11 \times 1 Jordan blocks.
Vol. 2, 7.6 Phase portraits, stability and linearization
Stable Definition
 
Vol. 2, 7.6 Phase portraits, stability and linearization
Statement Definition
A sentence that is either true or false, with no third option.
Vol. 2, 0.1 How to read a theorem
Stationary distribution Definition
A probability vector π\pi with Pπ=πP\pi = \pi: the chances do not change when the surfer takes another step.
Vol. 2, 2.11 Markov chains and PageRank
Steady-state response of the driven RLC circuit Theorem
For E(t)=E0cos⁡ωtE(t) = E_0\cos\omega t, every solution is a decaying transient plus the steady state Iss(t)=E0∣Z∣cos⁡(ωt−φ)I_{ss}(t) = \dfrac{E_0}{\lvert Z\rvert}\cos(\omega t - \varphi), where Z=R+i(ωL−1ωC)Z = R + i\left(\omega L - \dfrac{1}{\omega C}\right) is the impedance.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Step function Definition
A function that is constant on each open piece of some partition, like a staircase; its integral is the sum of value times width.
Vol. 2, 1.5 The Riemann integral: area as a limit
Step function on a rectangle Definition
A function s:Q→Rs: Q \to \mathbb R for which some partition of QQ makes ss constant on every open subrectangle; its integral is the sum of (value) times (area) over the pieces.
Vol. 2, 6.3 Multiple integrals
Stochastic gradient descent Definition
The iteration wk+1=wk−ηk∇ℓik(wk)w_{k+1} = w_k - \eta_k\nabla\ell_{i_k}(w_k) in which iki_k is an example chosen at random; each step costs one example instead of NN.
Vol. 2, 5.10 Gradient descent, momentum and Newton's method
Stochastic matrix Definition
A square matrix with no negative entries in which every column adds to 1. Its columns are probability vectors.
Vol. 2, 2.11 Markov chains and PageRank
Stokes' theorem Theorem
If SS is a piecewise smooth oriented surface whose boundary curve ∂S\partial S carries the induced orientation and FF is C1C^1 on an open set containing SS, then ∮∂SF⋅dr=∬S(curl⁡F)⋅n dS\oint_{\partial S}F\cdot dr = \iint_S(\operatorname{curl}F)\cdot n\,dS.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
Strong induction Definition
In the inductive step you may assume S(1), S(2), …, S(k) all at once, not only S(k).
Vol. 2, 0.2 Proof techniques
Subgroup Definition
A subset H of a group G that is itself a group under the same operation.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Subgroup test Proposition
A non-empty subset H of a group G is a subgroup as soon as ab⁻¹ is in H whenever a and b are in H.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Subsequence Definition
A sequence formed by picking terms of (an)(a_n) in order, skipping any: an1,an2,…a_{n_1}, a_{n_2}, \dots with n1<n2<…n_1 < n_2 < \dots.
Vol. 2, 1.2 Sequences and limits, from zero
Subset Definition
A⊆BA \subseteq B means every element of AA is also an element of BB.
Vol. 2, 0.3 Sets, functions, and counting infinity
Subspace Definition
A non-empty subset SS of a vector space VV that is itself a vector space with the same operations.
Vol. 2, 2.1 Vector spaces and subspaces
Subspace test Theorem
A non-empty subset of a vector space is a subspace exactly when it is closed under addition and under scalar multiplication.
Vol. 2, 2.1 Vector spaces and subspaces
Sup metric Definition
On C[a,b]C[a, b], d∞(f,g)=max⁡a≤x≤b∣f(x)−g(x)∣d_\infty(f, g) = \max_{a \le x \le b} |f(x) - g(x)|: the largest vertical gap between the graphs.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Superposition for linear homogeneous equations Proposition
The solutions of a linear homogeneous PDE form a vector space: sums and multiples of solutions are solutions.
Vol. 2, 5.9 Partial differential equations
Supremum Definition
The supremum of SS is its least upper bound: an upper bound that is smaller than every other upper bound.
Vol. 2, 1.1 The real numbers and completeness
Surface area Definition
The area of S=r(T)S = r(T) for a smooth parametrization is ∬T∥ru×rv∥ du dv\iint_T \lVert r_u \times r_v\rVert\,du\,dv.
Vol. 2, 6.5 Surfaces, area and flux
Surface integral Definition
For a continuous scalar field ff and a smooth parametrization r:T→Sr: T \to S, ∬Sf dS=∬Tf(r(u,v)) ∥ru×rv∥ du dv\iint_S f\,dS = \iint_T f(r(u, v))\,\lVert r_u\times r_v\rVert\,du\,dv.
Vol. 2, 6.5 Surfaces, area and flux
Surface integrals do not depend on the parametrization Proposition
 
Vol. 2, 6.5 Surfaces, area and flux
Surjective Definition
ff is surjective (onto) if every element of the codomain is an output: the range is the whole codomain.
Vol. 2, 0.3 Sets, functions, and counting infinity
Swapping two values flips the sign of a permutation Lemma
If σ′\sigma' is σ\sigma with the values at two positions exchanged, then sgn⁡σ′=−sgn⁡σ\operatorname{sgn}\sigma' = -\operatorname{sgn}\sigma.
Vol. 2, 2.7 Determinants
Symmetric matrices have real eigenvalues Theorem
Every eigenvalue of a Hermitian (in particular real symmetric) matrix is a real number.
Vol. 2, 3.1 Symmetric matrices and the spectral theorem
Symmetric operator Definition
A real linear map with A∗=AA^* = A, that is (Ax,y)=(x,Ay)(Ax, y) = (x, Ay); for a matrix, AT=AA^{\mathsf T} = A.
Vol. 2, 3.1 Symmetric matrices and the spectral theorem
System of differential equations Definition
Several unknown functions x1(t),…,xn(t)x_1(t), \dots, x_n(t) whose derivatives are given in terms of tt and the unknowns; in vector form x′=F(t,x)x' = F(t, x). It is linear if x′=A(t)x+g(t)x' = A(t)x + g(t) and has constant coefficients if AA does not depend on tt.
Vol. 2, 7.4 Systems of equations and the matrix exponential
System of linear equations Definition
mm equations in nn unknowns, each of the form (numbers) times x1,…,xnx_1, \dots, x_n added up, equal to a number. Written Ax=bAx = b.
Vol. 2, 2.6 Systems of equations and elimination
T
Tangent plane Definition
For a level surface f(x,y,z)=cf(x, y, z) = c and a point aa on it with ∇f(a)≠O\nabla f(a) \ne O, the tangent plane is {x:∇f(a)⋅(x−a)=0}\{x : \nabla f(a)\cdot(x - a) = 0\}; in the plane the tangent line to a level curve is defined the same way.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Taylor polynomial Definition
Tn(x)=∑k=0nf(k)(a)k!(x−a)kT_n(x) = \sum_{k=0}^n \frac{f^{(k)}(a)}{k!}(x - a)^k: the polynomial of degree n with the same value and first n derivatives as f at a.
Vol. 2, 1.4 The derivative as best linear approximation
Taylor's theorem with Lagrange remainder Theorem
If f has n + 1 derivatives, f(x) = T_n(x) + f^{(n+1)}(c)(x − a)^{n+1}/(n+1)! for some c between a and x.
Vol. 2, 1.4 The derivative as best linear approximation
The chain rule for fields Theorem
If gg is differentiable at aa and ff is differentiable at b=g(a)b = g(a), then h=f∘gh = f \circ g is differentiable at aa and h′(a)=f′(b)∘g′(a)h'(a) = f'(b) \circ g'(a); in matrices, Dh(a)=Df(b) Dg(a)Dh(a) = Df(b)\,Dg(a).
Vol. 2, 5.4 The chain rule for fields
The continuity equation Theorem
If the amount of a quantity in every fixed region EE changes only through the flux across ∂E\partial E, then ∂tu+∇⋅j=0\partial_tu + \nabla\cdot j = 0.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
The continuous image of a connected set is connected Theorem
If XX is connected and f:X→Yf : X \to Y is continuous, then f(X)f(X) is connected.
Vol. 2, 4.4 Connectedness and path-connectedness
The counting-number pairs are countable Theorem
N×N\mathbb N \times \mathbb N can be listed diagonal by diagonal, and the position of (m,n)(m, n) is P(m,n)=(m+n−2)(m+n−1)2+mP(m, n) = \tfrac{(m + n - 2)(m + n - 1)}{2} + m.
Vol. 2, 0.3 Sets, functions, and counting infinity
The derivative of a slice Theorem
For g(t)=f(a+ty)g(t) = f(a + ty), the derivative g′(t)g'(t) exists exactly when f′(a+ty;y)f'(a + ty; y) exists, and then g′(t)=f′(a+ty;y)g'(t) = f'(a + ty; y).
Vol. 2, 5.2 Directional derivatives, partial derivatives and the gradient
The derivative of an inverse field Theorem
If F:U→VF: U \to V is a diffeomorphism, then DF(x)DF(x) is an invertible matrix for every xx, and D(F−1)(F(x))=(DF(x))−1D(F^{-1})(F(x)) = \big(DF(x)\big)^{-1}.
Vol. 2, 5.4 The chain rule for fields
The derivative of e^(tA) Theorem
ddtetA=AetA=etAA\dfrac{d}{dt}e^{tA} = Ae^{tA} = e^{tA}A.
Vol. 2, 7.4 Systems of equations and the matrix exponential
The determinant is unique Corollary
There is at most one function satisfying all four axioms.
Vol. 2, 2.7 Determinants
The determinant of the transpose Theorem
det⁡AT=det⁡A\det A^{\mathsf T} = \det A. So everything true for rows is true for columns.
Vol. 2, 2.7 Determinants
The differential form of Gauss's law Corollary
If Gauss's law holds for every closed surface, and EE is C1C^1 and ρ\rho continuous, then ∇⋅E=ρ/ε0\nabla\cdot E = \rho/\varepsilon_0 at every point.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
The discrete metric and the Hamming distance are metrics Theorem
The discrete metric on any set, and dHd_H on bit strings of length nn, satisfy (M1), (M2) and (M3).
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
The divergence theorem Theorem
If EE is a solid region with boundary a closed piecewise smooth surface S=∂ES = \partial E with outward unit normal nn, and FF is C1C^1 on an open set containing EE, then ∬SF⋅n dS=∭Ediv⁡F dV\iint_SF\cdot n\,dS = \iiint_E\operatorname{div}F\,dV.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
The dual basis is a basis Theorem
If φ₁,…,φₙ is the dual basis of a basis v₁,…,vₙ of V, it is a basis of V*. In particular dim V* = dim V, and every functional is φ = φ(v₁)φ₁ + … + φ(vₙ)φₙ.
Vol. 2, 3.7 Dual spaces and quotient spaces
The dual map has the transposed matrix Theorem
If A is the matrix of T: V → W in bases v₁…vₙ and w₁…wₘ, then the matrix of Tᵀ: W* → V* in the dual bases is Aᵀ.
Vol. 2, 3.7 Dual spaces and quotient spaces
The epidemic threshold Theorem
 
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
The exponential distribution forgets Theorem
 
Vol. 2, 10.1 Probability as measure
The exponential of a diagonal matrix Fact
etdiag⁡(d1,…,dn)=diag⁡(ed1t,…,ednt)e^{t\operatorname{diag}(d_1, \dots, d_n)} = \operatorname{diag}(e^{d_1t}, \dots, e^{d_nt}).
Vol. 2, 7.4 Systems of equations and the matrix exponential
The Frobenius recurrence Theorem
The Frobenius series xs∑anxnx^s\sum a_nx^n with a0=1a_0 = 1 solves x2y′′+xPy′+Qy=0x^2y'' + xPy' + Qy = 0 exactly when F(s)=0F(s) = 0 and, for every n≥1n \ge 1, F(s+n) an=−∑k=0n−1[(s+k)pn−k+qn−k]akF(s+n)\,a_n = -\sum_{k=0}^{n-1}\big[(s+k)p_{n-k} + q_{n-k}\big]a_k.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
The Frobenius theorem Theorem
At a regular singular point with indicial roots α1≥α2\alpha_1 \ge \alpha_2, the larger root always gives a Frobenius series solution u1u_1. If α1−α2\alpha_1 - \alpha_2 is not a whole number, the smaller root gives a second one. If the roots are equal, or differ by a whole number, a second solution contains u1ln⁡xu_1\ln x.
Vol. 2, 7.5 Power series solutions, Legendre and Bessel
The Gaussian integral Theorem
∫−∞∞e−x2/2 dx=2π\displaystyle\int_{-\infty}^{\infty} e^{-x^2/2}\,dx = \sqrt{2\pi}, so the standard normal density has total area 1.
Vol. 2, 10.1 Probability as measure
The Google matrix has a unique stationary distribution Theorem
For 0≤d<10 \le d < 1, GG has exactly one stationary distribution π\pi, all its entries are at least 1−dn\tfrac{1-d}{n}, and from any starting probability vector ∥Gkx0−π∥1≤2dk\lVert G^kx_0 - \pi \rVert_1 \le 2d^k. Every eigenvalue other than 11 has size at most dd.
Vol. 2, 2.11 Markov chains and PageRank
The gradient is perpendicular to level sets Theorem
If ff is differentiable at aa and rr is a curve in the level set f=cf = c through aa, then ∇f(a)⋅r′(t0)=0\nabla f(a)\cdot r'(t_0) = 0: the gradient is perpendicular to the tangent vector of every such curve.
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
The gradient is the direction of steepest ascent Theorem
If f′(a;y)=∇f(a)⋅yf'(a; y) = \nabla f(a)\cdot y for all yy and ∇f(a)≠O\nabla f(a) \ne O, then among unit vectors uu the rate f′(a;u)f'(a; u) is largest, equal to ∥∇f(a)∥\lVert\nabla f(a)\rVert, for u=∇f(a)/∥∇f(a)∥u = \nabla f(a)/\lVert\nabla f(a)\rVert, smallest for u=−∇f(a)/∥∇f(a)∥u = -\nabla f(a)/\lVert\nabla f(a)\rVert, and 00 for uu perpendicular to ∇f(a)\nabla f(a).
Vol. 2, 5.2 Directional derivatives, partial derivatives and the gradient
The gradient of a composite Corollary
If ff is a scalar field and g=(g1,…,gn)g = (g_1, \dots, g_n) a vector field, then ∇(f∘g)(a)=∑k=1nDkf(g(a)) ∇gk(a)=Dg(a)T ∇f(g(a))\nabla(f \circ g)(a) = \sum_{k=1}^n D_kf(g(a))\,\nabla g_k(a) = Dg(a)^{\mathsf T}\,\nabla f(g(a)).
Vol. 2, 5.4 The chain rule for fields
The graph of a continuous function has content zero Lemma
If φ:[a,b]→R\varphi: [a, b] \to \mathbb R is continuous, its graph {(x,φ(x))}\{(x, \varphi(x))\} has content zero.
Vol. 2, 6.3 Multiple integrals
The harmonic series diverges Theorem
∑k=1∞1k\sum_{k=1}^\infty \frac1k diverges, although 1k→0\frac1k \to 0.
Vol. 2, 1.6 Series, power series, and uniform convergence
The heat equation from conservation of energy Theorem
Energy conservation (continuity) plus Fourier's law gives ρc ∂tT=κ∇2T\rho c\,\partial_tT = \kappa\nabla^2T.
Vol. 2, 6.8 Maxwell's equations, conservation laws and heat
The integers are countable Theorem
Z\mathbb Z can be listed as 0,1,−1,2,−2,3,−3,…0, 1, -1, 2, -2, 3, -3, \dots with every integer exactly once.
Vol. 2, 0.3 Sets, functions, and counting infinity
The integral of a step function does not depend on the partition Proposition
Two partitions that both make ss constant on every open piece give the same sum.
Vol. 2, 6.3 Multiple integrals
The law of exponents for one matrix Theorem
e0A=Ie^{0A} = I, e(s+t)A=esAetAe^{(s+t)A} = e^{sA}e^{tA}, and etAe^{tA} is invertible with inverse e−tAe^{-tA}.
Vol. 2, 7.4 Systems of equations and the matrix exponential
The Lotka–Volterra conservation law Theorem
For x′=x(a−by)x' = x(a - by), y′=y(dx−c)y' = y(dx - c) with positive constants, H=dx−cln⁡x+by−aln⁡yH = dx - c\ln x + by - a\ln y is constant along solutions in the open first quadrant. Every orbit there is a closed curve around the equilibrium (c/d, a/b)(c/d,\ a/b), and the average of xx and of yy over a period equal its equilibrium value.
Vol. 2, 7.6 Phase portraits, stability and linearization
The matrix exponential always converges Theorem
For every square matrix MM the series ∑Mk/k!\sum M^k/k! converges, and ∥eM∥≤n−1+e∥M∥\lVert e^M\rVert \le n - 1 + e^{\lVert M\rVert}.
Vol. 2, 7.4 Systems of equations and the matrix exponential
The matrix norm is submultiplicative Theorem
∥AB∥≤∥A∥ ∥B∥\lVert AB\rVert \le \lVert A\rVert\,\lVert B\rVert, hence ∥Ak∥≤∥A∥k\lVert A^k\rVert \le \lVert A\rVert^k.
Vol. 2, 7.4 Systems of equations and the matrix exponential
The matrix of an inverse is the inverse of the matrix Theorem
If T:V→VT: V \to V is invertible and A=m(T)A = m(T) in one basis, then A−1=m(T−1)A^{-1} = m(T^{-1}) in the same basis, and AA−1=A−1A=IAA^{-1} = A^{-1}A = I.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
The modulus is multiplicative Theorem
∣zw∣=∣z∣ ∣w∣|zw| = |z|\,|w|: the length of a product is the product of the lengths.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
The multiplier is the price of the constraint Theorem
If the constrained optimum x∗(c)x^*(c) depends differentiably on cc and V(c)=f(x∗(c))V(c) = f(x^*(c)), then V′(c)=λ(c)V'(c) = \lambda(c): the multiplier is the rate at which the best value changes when the constraint g=cg = c is moved.
Vol. 2, 5.8 Constrained extrema and Lagrange multipliers
The n-th roots of unity Theorem
zn=1z^n = 1 has exactly nn complex solutions, ωk=e2πik/n\omega_k = e^{2\pi i k / n} for k=0,1,…,n−1k = 0, 1, \dots, n - 1, the corners of a regular nn-gon on the unit circle; for n≥2n \ge 2 they add up to 00.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
The Neumann series Theorem
If ∥A∥<1\lVert A\rVert < 1 for the matrix norm of this chapter, then I−AI - A is invertible and (I−A)−1=∑k≥0Ak(I - A)^{-1} = \sum_{k\ge0}A^k.
Vol. 2, 7.4 Systems of equations and the matrix exponential
The norm of an integral Fact
For a continuous curve v:[a,b]→Rmv : [a, b] \to \mathbb R^m, ∥∫abv(s) ds∥≤∫ab∥v(s)∥ ds\lVert \int_a^b v(s)\,ds \rVert \le \int_a^b \lVert v(s) \rVert\,ds.
Vol. 2, 7.1 Existence and uniqueness for differential equations
The nth-term test Theorem
If ∑ak\sum a_k converges, then ak→0a_k \to 0.
Vol. 2, 1.6 Series, power series, and uniform convergence
The orthogonal complement is a subspace meeting S only at O Theorem
S⊥S^\perp is a subspace, and the only vector in both SS and S⊥S^\perp is OO.
Vol. 2, 2.9 Inner products, orthogonality, Gram–Schmidt, projection
The permutation formula gives a determinant function Theorem
det⁡A=∑σsgn⁡(σ) a1σ(1)a2σ(2)⋯anσ(n)\det A = \sum_\sigma\operatorname{sgn}(\sigma)\,a_{1\sigma(1)}a_{2\sigma(2)}\cdots a_{n\sigma(n)} satisfies all four axioms. So the determinant exists for every nn.
Vol. 2, 2.7 Determinants
The projection matrix projects Theorem
PbPb is the closest point of the column space to bb, P2=PP^2 = P and PT=PP^{\mathsf T} = P.
Vol. 2, 2.10 Least squares and regression as projection
The quotient space is a vector space Theorem
The sum and scalar multiple on V/U are well defined, V/U is a vector space with zero vector O + U = U, and v ↦ v + U is a linear map from V onto V/U whose null space is U.
Vol. 2, 3.7 Dual spaces and quotient spaces
The Rabi formula Theorem
For H=ℏ2(δσz+Ωσx)H = \frac\hbar2(\delta\sigma_z + \Omega\sigma_x) and ΩR=δ2+Ω2\Omega_R = \sqrt{\delta^2 + \Omega^2}: e−iHt/ℏ=cos⁡ΩRt2 I−isin⁡ΩRt2⋅δσz+ΩσxΩRe^{-iHt/\hbar} = \cos\frac{\Omega_Rt}{2}\,I - i\sin\frac{\Omega_Rt}{2}\cdot\frac{\delta\sigma_z + \Omega\sigma_x}{\Omega_R}. Starting in level 1, the probability of level 2 is Ω2ΩR2sin⁡2ΩRt2\dfrac{\Omega^2}{\Omega_R^2}\sin^2\dfrac{\Omega_Rt}{2}.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
The rationals are countable Theorem
Q\mathbb Q can be listed, even though between any two rationals there are infinitely many more.
Vol. 2, 0.3 Sets, functions, and counting infinity
The rationals are dense Theorem
Between any two real numbers there is a rational number.
Vol. 2, 1.1 The real numbers and completeness
The real numbers are uncountable Theorem
The interval (0,1)(0, 1), and so the set R\mathbb R of all real numbers, cannot be listed.
Vol. 2, 0.3 Sets, functions, and counting infinity
The reals are Archimedean Theorem
The natural numbers are not bounded above in R\mathbb R.
Vol. 2, 1.1 The real numbers and completeness
The rectangle lemma Lemma
If fxf_x and fxyf_{xy} exist on an open set containing the rectangle with corners (a,b)(a, b) and (a+h,b+k)(a + h, b + k), then Δ(h,k)=hk fxy(ξ,η)\Delta(h, k) = hk\,f_{xy}(\xi, \eta) for some point (ξ,η)(\xi, \eta) strictly inside the rectangle.
Vol. 2, 5.5 Higher partial derivatives and the equality of mixed partials
The second-derivative test Theorem
 
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
The second-derivative test for two variables Theorem
 
Vol. 2, 5.6 Taylor's formula, the Hessian and extrema
The series C and S are cosine and sine Lemma
For every real xx, C(x)=cos⁡xC(x) = \cos x and S(x)=sin⁡xS(x) = \sin x, where cos⁡\cos and sin⁡\sin are the unit-circle functions.
Vol. 2, 1.6 Series, power series, and uniform convergence
The sign is a homomorphism Theorem
For permutations σ and τ of {1,…,n}, sgn(τ∘σ) = sgn(τ)·sgn(σ). So sgn: Sₙ → ({1, −1}, ×) is a homomorphism, whose kernel is the group Aₙ of even permutations.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
The span is a subspace Theorem
For any finite set SS in VV, the span L(S)L(S) is a subspace of VV.
Vol. 2, 2.2 Span, independence, basis, dimension
The square of i Theorem
With the product above, i⋅i=−1i \cdot i = -1.
Vol. 2, 0.6 Complex numbers and polynomials, done properly
The square root of 2 is irrational Theorem
There are no integers p,qp, q with (p/q)2=2(p/q)^2 = 2.
Vol. 2, 0.2 Proof techniques
The standard norms are norms Theorem
∥⋅∥1\lVert \cdot \rVert_1, ∥⋅∥2\lVert \cdot \rVert_2 and ∥⋅∥∞\lVert \cdot \rVert_\infty are norms on Rn\mathbb R^n, and the sup norm is a norm on C[a,b]C[a, b].
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
The topologist's sine curve Proposition
S=G∪LS = G \cup L is connected, but there is no path in SS from (0,0)(0, 0) to (1,sin⁡1)(1, \sin 1).
Vol. 2, 4.4 Connectedness and path-connectedness
The unit ball of C[0,1] is closed and bounded but not compact Proposition
In C[0,1]C[0, 1] with the sup metric, the closed unit ball {f:max⁡∣f∣≤1}\{f : \max|f| \le 1\} is closed and bounded and has a sequence with no convergent subsequence, so it is not compact.
Vol. 2, 4.3 Compactness
The Vandermonde determinant Theorem
det⁡V=∏0≤i<j≤n(xj−xi)\det V = \prod_{0 \le i < j \le n} (x_j - x_i). So VV is invertible exactly when the nodes are distinct.
Vol. 2, 15.1 Numerical analysis
The work-energy theorem Theorem
For a particle of mass mm moving under a force field FF, the work done in a time interval equals the change in kinetic energy 12mv2\frac12mv^2.
Vol. 2, 6.2 Gradient fields and potentials
There are exactly n residue classes Theorem
Every integer is congruent mod nn to exactly one of 0,1,…,n−10, 1, \dots, n - 1, namely its remainder; so there are exactly nn classes, and a≡ba \equiv b iff aa and bb have the same remainder.
Vol. 2, 0.5 Integers mod n, gcd and Bézout
Three equivalent descriptions of a gradient field Theorem
For a continuous field on an open connected set, (a) FF is a gradient, (b) its line integral is independent of the path, and (c) its line integral around every closed piecewise smooth path is 00, are equivalent.
Vol. 2, 6.2 Gradient fields and potentials
Three faces of continuity Theorem
For f:X→Yf : X \to Y between metric spaces: ff is continuous (with ε\varepsilon and δ\delta) iff xn→ax_n \to a implies f(xn)→f(a)f(x_n) \to f(a) iff the preimage of every open set is open iff the preimage of every closed set is closed.
Vol. 2, 4.5 Continuity between metric spaces
Three ways to show a set is countable Theorem
AA is countable iff there is an injection A→NA \to \mathbb N; and a non-empty AA is countable iff there is a surjection N→A\mathbb N \to A (a list that may have repeats).
Vol. 2, 0.3 Sets, functions, and counting infinity
Total derivative Definition
The linear map TaT_a in the definition of a differentiable field; it is unique, and it is written F′(a)F'(a) or DF(a)DF(a).
Vol. 2, 5.3 The total derivative, the Jacobian matrix and tangent planes
Totally bounded Definition
 
Vol. 2, 4.3 Compactness
Trace Definition
The sum of the diagonal entries of a square matrix, tr⁡A=a11+a22+⋯+ann\operatorname{tr} A = a_{11} + a_{22} + \dots + a_{nn}.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Trace and determinant from the eigenvalues Theorem
The trace is the sum of the eigenvalues and the determinant is their product, each counted with multiplicity.
Vol. 2, 2.8 Eigenvalues and eigenvectors
Transpose Definition
The matrix ATA^{\mathsf T} whose rows are the columns of AA: (AT)ij=aji(A^{\mathsf T})_{ij} = a_{ji}.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Transpose of a product Theorem
(AB)T=BTAT(AB)^{\mathsf T} = B^{\mathsf T}A^{\mathsf T}.
Vol. 2, 2.5 Matrices as maps, multiplication, change of basis
Trapezoidal rule Definition
T=b−a2(f(a)+f(b))T = \dfrac{b-a}{2}\big(f(a) + f(b)\big): the area of the trapezoid under the chord from (a,f(a))(a, f(a)) to (b,f(b))(b, f(b)), which is the integral of the linear interpolant.
Vol. 2, 15.1 Numerical analysis
Triangle inequality Definition
∣x+y∣≤∣x∣+∣y∣|x + y| \le |x| + |y|: the direct distance is never longer than a detour.
Vol. 2, 1.2 Sequences and limits, from zero
Triple integral Definition
The triple integral ∭Ef dV\iiint_Ef\,dV is defined exactly as the double integral, with boxes [a,b]×[c,d]×[e,g][a, b] \times [c, d] \times [e, g], step functions constant on open sub-boxes, and volume in place of area.
Vol. 2, 6.3 Multiple integrals
Two solutions that meet are equal Corollary
If ff is continuous and satisfies a Lipschitz condition on every closed rectangle inside its domain, then two solutions of the same IVP agree on every interval where both are defined.
Vol. 2, 7.1 Existence and uniqueness for differential equations
Two-form Definition
In R3\mathbb R^3 a 2-form is A dy∧dz+B dz∧dx+C dx∧dyA\,dy\wedge dz + B\,dz\wedge dx + C\,dx\wedge dy; at each point it takes two vectors a,ba, b to (A,B,C)⋅(a×b)(A, B, C)\cdot(a\times b), the amount of the field (A,B,C)(A, B, C) crossing the parallelogram on aa and bb.
Vol. 2, 6.7 Differential forms and the one big theorem
Two-level system Definition
A quantum system whose state space is C2\mathbb C^2: a vector ψ=(ψ1,ψ2)\psi = (\psi_1, \psi_2) with ∣ψ1∣2+∣ψ2∣2=1\lvert\psi_1\rvert^2 + \lvert\psi_2\rvert^2 = 1, and a 2×22 \times 2 Hermitian Hamiltonian.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Type I region Definition
A region S={(x,y):a≤x≤b, φ1(x)≤y≤φ2(x)}S = \{(x, y): a \le x \le b,\ \varphi_1(x) \le y \le \varphi_2(x)\} with φ1≤φ2\varphi_1 \le \varphi_2 continuous: between a lower curve and an upper curve.
Vol. 2, 6.3 Multiple integrals
Type II region Definition
A region S={(x,y):c≤y≤d, ψ1(y)≤x≤ψ2(y)}S = \{(x, y): c \le y \le d,\ \psi_1(y) \le x \le \psi_2(y)\} with ψ1≤ψ2\psi_1 \le \psi_2 continuous: between a left curve and a right curve.
Vol. 2, 6.3 Multiple integrals
U
Uncountable Definition
A set is uncountable if it is not countable: no list, however cleverly made, contains all its elements.
Vol. 2, 0.3 Sets, functions, and counting infinity
Undetermined coefficients Definition
Guess a particular solution of the form dictated by the right-hand side, with unknown constants, substitute, and match coefficients.
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Uniform continuity Definition
 
Vol. 2, 1.3 Limits and continuity with epsilon and delta
Uniform continuity between metric spaces Theorem
 
Vol. 2, 4.5 Continuity between metric spaces
Uniform convergence Definition
 
Vol. 2, 1.6 Series, power series, and uniform convergence
Uniform limit of continuous functions is continuous Theorem
If each fnf_n is continuous and fn→ff_n \to f uniformly, then ff is continuous.
Vol. 2, 1.6 Series, power series, and uniform convergence
Union Definition
A∪BA \cup B is the set of everything that is in AA or in BB (or both).
Vol. 2, 0.3 Sets, functions, and counting infinity
Union bound Theorem
For any events A1,A2,…A_1, A_2, \dots, P(A1∪A2∪⋯ )≤P(A1)+P(A2)+⋯P(A_1 \cup A_2 \cup \cdots) \le P(A_1) + P(A_2) + \cdots (overlaps are counted twice, so the sum can only be too big).
Vol. 2, 10.1 Probability as measure
Unions and finite intersections of open sets Theorem
∅\varnothing and XX are open; any union of open sets is open; the intersection of finitely many open sets is open.
Vol. 2, 4.1 Metric and normed spaces; open and closed sets
Unique coordinates Theorem
If e1,…,ene_1, \dots, e_n is a basis, each vector is ∑ciei\sum c_i e_i for exactly one list (c1,…,cn)(c_1, \dots, c_n).
Vol. 2, 2.2 Span, independence, basis, dimension
Uniqueness for the heat equation Theorem
A C2C^2 solution of ut=αuxxu_t = \alpha u_{xx} on [0,L]×[0,T][0, L]\times[0, T] with given initial temperature and given end temperatures is unique.
Vol. 2, 5.9 Partial differential equations
Uniqueness of negatives Theorem
Each xx has exactly one yy with x+y=Ox + y = O, namely (−1)x(-1)x.
Vol. 2, 2.1 Vector spaces and subspaces
Uniqueness of the zero vector Theorem
A vector space has exactly one zero element.
Vol. 2, 2.1 Vector spaces and subspaces
Unitary evolution Theorem
The solution of iℏψ′=Hψi\hbar\psi' = H\psi is ψ(t)=U(t)ψ(0)\psi(t) = U(t)\psi(0) with U(t)=e−iHt/ℏU(t) = e^{-iHt/\hbar}. For Hermitian HH the matrix U(t)U(t) is unitary, so ∥ψ(t)∥=∥ψ(0)∥\lVert\psi(t)\rVert = \lVert\psi(0)\rVert for all tt: total probability stays 11.
Vol. 2, 7.7 Applications to springs, circuits, epidemics and qubits
Unitary matrix Definition
A complex square matrix with U∗U=IU^*U = I (conjugate transpose); the complex version of orthogonal.
Vol. 2, 3.3 Orthogonal matrices, rotations and reflections
Upper bound Definition
MM is an upper bound of SS if every element of SS is at most MM.
Vol. 2, 1.1 The real numbers and completeness
Upper sum Definition
U(f,P)=∑i=1nMi ΔxiU(f, P) = \sum_{i=1}^n M_i\,\Delta x_i: the total area of the outer rectangles.
Vol. 2, 1.5 The Riemann integral: area as a limit
V
Vandermonde matrix Definition
The (n+1)×(n+1)(n+1) \times (n+1) matrix whose row jj is (1,xj,xj2,…,xjn)(1, x_j, x_j^2, \dots, x_j^n). Its determinant is the product of all differences xj−xix_j - x_i with i<ji < j.
Vol. 2, 15.1 Numerical analysis
Variance Definition
Var⁡(X)=E[(X−μ)2]\operatorname{Var}(X) = E\big[(X - \mu)^2\big] with μ=E[X]\mu = E[X]: the average squared distance from the mean, a measure of spread.
Vol. 2, 10.1 Probability as measure
Variance of a sum of independent variables Theorem
If XX and YY are independent discrete random variables with finite variance, then E[XY]=E[X]E[Y]E[XY] = E[X]E[Y] and Var⁡(X+Y)=Var⁡(X)+Var⁡(Y)\operatorname{Var}(X + Y) = \operatorname{Var}(X) + \operatorname{Var}(Y).
Vol. 2, 10.1 Probability as measure
Variance shortcut and scaling Theorem
Var⁡(X)=E[X2]−(E[X])2\operatorname{Var}(X) = E[X^2] - (E[X])^2 and Var⁡(aX+b)=a2Var⁡(X)\operatorname{Var}(aX + b) = a^2\operatorname{Var}(X).
Vol. 2, 10.1 Probability as measure
Variation of constants for systems Theorem
The IVP x′=Ax+g(t)x' = Ax + g(t), x(a)=bx(a) = b has the unique solution x(t)=e(t−a)Ab+∫ate(t−s)Ag(s) dsx(t) = e^{(t-a)A}b + \int_a^te^{(t-s)A}g(s)\,ds.
Vol. 2, 7.4 Systems of equations and the matrix exponential
Variation of parameters Definition
Look for a particular solution y=u1(t)b1(t)+⋯+un(t)bn(t)y = u_1(t)b_1(t) + \dots + u_n(t)b_n(t), where the bib_i are a basis of the homogeneous solutions and the coefficients uiu_i are unknown functions; impose n−1n - 1 extra conditions that make the derivatives clean.
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Variation of parameters formula Theorem
If b1,…,bnb_1, \dots, b_n is a basis of ker⁡L\ker L with Wronskian matrix W\mathcal W, and u′=W−1(0,…,0,R)Tu' = \mathcal W^{-1}(0, \dots, 0, R)^{\mathsf T}, then yp=u1b1+⋯+unbny_p = u_1b_1 + \dots + u_nb_n solves Ly=RLy = R.
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Vector field Definition
A function FF that gives a vector F(x)∈RmF(x) \in \mathbb R^m at each point xx of a set S⊆RnS \subseteq \mathbb R^n; its mm components F1,…,FmF_1, \dots, F_m are scalar fields.
Vol. 2, 5.1 Scalar and vector fields, limits and continuity
Vector space Definition
A non-empty set VV with an addition and a scalar multiplication that obey the ten axioms below; its elements are called vectors.
Vol. 2, 2.1 Vector spaces and subspaces
Vitali: no uniform probability on every subset Theorem
There is no way to assign a probability to every subset of the interval [0, 1) so that probabilities add over countably many disjoint sets, the whole interval has probability 1, and sliding a set around the circle (mod 1) never changes its probability.
Vol. 2, 10.1 Probability as measure
Vorticity Definition
The vorticity of a velocity field vv is curl⁡v\operatorname{curl}v.
Vol. 2, 6.6 Curl, divergence, Stokes' theorem and Gauss's theorem
W
Wave equation Definition
The equation utt=c2uxxu_{tt} = c^2u_{xx} for the displacement u(x,t)u(x, t) of a vibrating string, with cc the wave speed.
Vol. 2, 5.9 Partial differential equations
Weak law of large numbers Theorem
 
Vol. 2, 10.1 Probability as measure
Wedge product Definition
The product of forms, bilinear and associative, with ω∧η=(−1)jkη∧ω\omega\wedge\eta = (-1)^{jk}\eta\wedge\omega for degrees j,kj, k; in particular dxi∧dxj=−dxj∧dxidx_i\wedge dx_j = -dx_j\wedge dx_i and dxi∧dxi=0dx_i\wedge dx_i = 0.
Vol. 2, 6.7 Differential forms and the one big theorem
Weierstrass M-test Theorem
If ∣fk(x)∣≤Mk|f_k(x)| \le M_k for all x∈Dx \in D and ∑Mk\sum M_k converges, then ∑fk\sum f_k converges uniformly (and absolutely) on DD.
Vol. 2, 1.6 Series, power series, and uniform convergence
Well-ordering principle Definition
Every non-empty set of positive integers has a smallest element.
Vol. 2, 0.2 Proof techniques
What the first three axioms force on the rows Lemma
A function with Axioms 1 to 3 is zero if a row is zero, changes sign when two rows are swapped, is unchanged when a multiple of one row is added to another, and is zero when the rows are dependent.
Vol. 2, 2.7 Determinants
Winding number Definition
The winding number W(r;p)W(r; p) of a closed piecewise smooth path rr about a point pp not on it is 12π∮−(y−y0) dx+(x−x0) dy(x−x0)2+(y−y0)2\frac1{2\pi}\oint\frac{-(y - y_0)\,dx + (x - x_0)\,dy}{(x - x_0)^2 + (y - y_0)^2}: the number of times rr goes counterclockwise around pp.
Vol. 2, 6.4 Green's theorem and change of variables
Work Definition
The work done by a force field FF on a particle moving along CC is the line integral ∫CF⋅dr\int_C F \cdot dr.
Vol. 2, 6.1 Paths and line integrals
Wronskian Definition
For nn functions with n−1n - 1 derivatives, the determinant of the n×nn \times n matrix whose rows are the functions and their successive derivatives: W=det⁡(fi(j))W = \det\big(f_i^{(j)}\big).
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Wronskian of exponentials Fact
For distinct numbers r1,…,rnr_1, \dots, r_n, W(er1t,…,ernt)=e(r1+⋯+rn)t⋅VW(e^{r_1t}, \dots, e^{r_nt}) = e^{(r_1 + \dots + r_n)t}\cdot V with V=det⁡(ri j)V = \det(r_i^{\,j}) non-zero, so the exponentials are independent.
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Wronskian of solutions of a linear equation Theorem
For nn solutions of Ly=0Ly = 0 the following are equivalent: they are linearly independent; W(t)≠0W(t) \ne 0 for every tt; W(t0)≠0W(t_0) \ne 0 for some t0t_0. So WW is either zero everywhere or non-zero everywhere.
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Wronskian test for power series Theorem
If ff and gg are power series with radius of convergence 11, then f,gf, g are linearly independent on (−1,1)(-1, 1) if and only if W(f,g)W(f, g) is not identically zero.
Vol. 2, 7.3 The Wronskian, variation of parameters and undetermined coefficients
Z
Z_n is a field exactly when n is prime Theorem
For n ≥ 2, the ring Zₙ of integers mod n is a field if and only if n is prime.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Zero derivative means constant Corollary
If f′(x)=0f'(x) = 0 for every x in an interval, f is constant there.
Vol. 2, 1.4 The derivative as best linear approximation
Zero gradient on a connected open set means constant Theorem
If U⊆RnU \subseteq \mathbb R^n is open and connected and ff is differentiable on UU with ∇f=O\nabla f = O everywhere, then ff is constant on UU.
Vol. 2, 4.4 Connectedness and path-connectedness
Zero times anything in a ring Proposition
In any ring, 0·a = 0 and (−1)·a = −a.
Vol. 2, 3.9 Groups, rings and fields: a preview built from what you know
Zero vector Definition
The element OO of axiom 5, with x+O=xx + O = x for every xx; it is unique.
Vol. 2, 2.1 Vector spaces and subspaces