computo ergo sum

2026-09-26 (revised 2026-10-09) · book Millennium Problemsquantum field theorygauge theory

Yang–Mills and the mass gap — from the beginner to where things stand

This is the Clay Mathematics Institute's Millennium Prize Problem "Yang–Mills existence and mass gap", set out in the form of a single textbook. It starts where a second-year mathematics or physics student can read, and goes as far as where the world stands and the range measured on this machine. There are 124 chapters in all, and 124 can be read now. You do not need to read them in order. The intended way of reading is to jump from the contents to the chapter you need, and to go back to a prerequisite chapter when a tool you do not know appears.

What the problem is — On four-dimensional space, construct Yang–Mills theory for a compact simple group in a form that satisfies the axioms of quantum field theory, and show that the mass of the lightest excitation is positive (0-03).

Where this book stands — This problem has not been solved. This site has not solved it either. What is here is an exact copy of the shape of the problem, a map of how far the mathematical side and the physical side have each come and where they let go of each other, and a record of measuring what can be measured on the lattice.

Readers — If you know multivariable calculus, linear algebra, complex numbers, introductory mechanics and electromagnetism, and elementary probability, you can read from Part 1 and Part 2. Any further tools are prepared inside this book.

LeanMachine-checked (Lean 4, sorry 0, no native_decide, axioms a subset of the three standard ones) PaperA proof exists, but machine checking is not finished ComputedThe range checked on this machine. Not made into a claim for outside use KnownKnown theorems, restatements, and checks against outside literature PhysicsAccepted at the level of physics but not a theorem of mathematics (numerics, semiclassics, conjectures)


01

Contents

Chapters marked "Detour:" can be skipped without affecting the main line. Each chapter states its "Prerequisite chapters" at the top. Chapters "in preparation" will be added in turn.

Part 0 Entrance — how to read this book

Ch.TitleContentsPrereq.
0-01How to read this bookReaders, prerequisite knowledge, the key to the labels, how to use the contents, how to skip detours, suggested reading orders (five)—
0-02One pictureWhat is asked, and where things let go (a short version of the entrance page)—
0-03Reading the problem statement word by wordClay's text, the group, R⁴, existence, non-triviality, the gap, short distances, notes—
0-04Four dimensions in mathematics and four dimensions in physicsA bridge to the existing `four-dimensions.html` and `spacetime.html`—

Part 1 Mathematical preparation

Ch.TitleContentsPrereq.
1-01Vector spaces and linear mapsEigenvalues, the matrix exponential, Hermitian and unitary—
1-02What a group isSymmetry, the rotation group SO(3), SU(2) and the double cover, a first look at representations1-01
1-03Lie groups and Lie algebrasThe exponential map, commutators, structure constants, the Killing form1-02
1-04SU(2) and SU(3)Pauli, Gell-Mann, the adjoint representation, the list of compact simple groups1-03
1-05Manifolds and tangent spacesCoordinate-free differentiation, vector fields1-01
1-06Differential forms and the exterior derivativeStokes, closed and exact, a first look at de Rham1-05
1-07Vector bundles and connectionsParallel transport, curvature, holonomy, the geometry of gauge transformations1-04, 1-06
1-08Probability and measureProbability as a measure, expectation, independence, Gaussian measures, the law of large numbers and the central limit theorem—
1-09Probability in infinite dimensionsThe absence of Lebesgue measure, Gaussian measures and Cameron–Martin, white noise1-08
1-10Hilbert spaces and self-adjoint operatorsSpectrum, the lowest eigenvalue and the variational principle, the Poincaré inequality1-01
1-11Fourier analysis and distributionsTest functions, propagators, singularities, the difficulty with products1-10
1-12Detour: what happens only in four dimensionsWhat happens only in four dimensions (a guide to the existing page, and the parts that matter in this book)—

Part 2 Physical preparation

Ch.TitleContentsPrereq.
2-01Lagrangians and the actionLeast action, Euler–Lagrange, Noether (symmetries and conservation laws)1-01
2-02The idea of a fieldFrom the vibrating string to the wave equation, energy, infinitely many degrees of freedom2-01
2-03Electromagnetism is a gauge theoryPotentials, gauge transformations, U(1), Aharonov–Bohm2-02
2-04Special relativity and spacetimeOne sign differs (a bridge to the existing `spacetime.html`), Lorentz-invariant actions2-01
2-05The bones of quantum mechanicsStates, the Hamiltonian, the spectrum, the ground state, what "gap" means1-10
2-06The harmonic oscillator and creation and annihilationThe smallest unit of quantum field theory, Fock space2-05
2-07The idea of the path integralFeynman, imaginary time, the match with statistical mechanics, Gaussian integrals2-05, 1-08
2-08Statistical mechanics and phase transitionsThe partition function, correlations, the correlation length, criticality, universality1-08
2-09Detour: the gap and the correlation length in the Ising modelThe "gap" and the correlation length seen in the Ising model (with computations on this machine)2-08
2-10The relaxation time and the dynamical exponent zLangevin and Glauber dynamics, relaxation time τ=ξ² for the Gaussian chain (exact), C_P/ξ² ∼ L^{z−2} on a small band of the two-dimensional Ising model (computed), η_dyn=2−z is fixed here, known examples where the type of Assumption H (C_P≍ξ²) fails (z≠2), the heat bath and Langevin are not identified2-08, 2-09

Part 3 Yang–Mills theory (classical)

Ch.TitleContentsPrereq.
3-01The gauge principleDemanding a local symmetry produces a force2-03, 1-04
3-02Non-abelian gauge fieldsYang–Mills 1954, the covariant derivative, the field strength, self-interaction3-01
3-03The action and the equationstr F², Bianchi, self-duality, energy3-02
3-04Gauge theory as geometryThe space of connections, the gauge orbit space, Singer's theorem (the impossibility of a global gauge fixing)1-07, 3-02
3-05Instantons and topologyThe second Chern number, BPST, the θ term3-03
3-06Detour: Donaldson and exotic R⁴Donaldson and exotic R⁴ — classical Yang–Mills sees the topology of four dimensions3-05
3-07Yang–Mills inside the Standard ModelSU(3)×SU(2)×U(1), quarks, Higgs, how it differs from pure YM3-02

Part 4 Quantisation

Ch.TitleContentsPrereq.
4-01Canonical quantisation and the HamiltonianThe Gauss constraint, physical states2-05, 3-03
4-02The path integral and EuclideanisationWick rotation, field theory as a probability measure, "spacetime" becomes "space"2-07, 2-04
4-03Perturbation theory and Feynman diagramsPropagators, vertices, loops4-02
4-04Divergences and renormalisationWhy infinities appear, counterterms, the renormalisation group equation4-03
4-05The algebra of divergencesBPHZ, Epstein–Glaser, dimensional regularisation, Connes–Kreimer, Costello4-04
4-06Asymptotic freedomThe β function, 11N/3, the history of the discovery, consistency with the lattice4-04
4-07Dimensional transmutation and ΛOne scale, exp(−1/g²), quantities invisible to perturbation theory4-06
4-08Gauge fixing and Faddeev–PopovBRST, Gribov copies, the 0/0 on the lattice (Neuberger)4-03, 3-04
4-09The axioms of quantum field theoryWightman, Haag's theorem, representations of infinitely many degrees of freedom1-10, 2-06
4-10The Osterwalder–Schrader axioms and reconstructionReflection positivity is the key4-02, 4-09
4-11The definition of the mass gapThe gap in the spectrum, how it differs from particle states, clustering, the correlation length4-10, 2-08
4-12Detour: the perturbation series divergesPerturbation series diverge — Dyson, renormalons, Borel, transseries4-04

Part 5 Lattice gauge theory

Ch.TitleContentsPrereq.
5-01Wilson's latticeLink variables, plaquettes, the action, gauge invariance kept exactly3-03, 1-04
5-02The strong-coupling expansionSmall β, the area law, confinement, convergence5-01
5-03Reflection positivity and the transfer matrixOsterwalder–Seiler, the lattice Hamiltonian5-01, 4-10
5-04The infinite-volume limit and the cluster expansionWhat can be shown on the strong-coupling side5-02
5-05Weak coupling and the continuum limita(β), scaling, the lattice version of asymptotic freedom, Symanzik5-01, 4-06
5-06How U(1) differs from the non-abelian caseGuth, Fröhlich–Spencer, whether there is a phase transition, the exact form of "because it is non-abelian"5-02
5-07The Monte Carlo methodUpdates, detailed balance, autocorrelation, errors, critical slowing down5-01, 1-08
5-08Measuring glueballs and the string tensionThe variational method, m/√σ, numbers from primary sources5-07
5-09What to hold fixed when taking the limitProblem 5.1, dimensionless ratios, the misreading of "a uniform gap"5-05, 4-11
5-10Lattice gauge theory with finite groupsExponential decay at weak coupling, the absence of confinement5-02
5-11Detour: Bakry–Émery and one-link integrationBakry–Émery and one-link integration (this site's paper) — an example of a theorem on the strong-coupling side5-02, 1-10

Part 6 Constructive field theory

Ch.TitleContentsPrereq.
6-01What constructive field theory isSix stages4-10
6-02Solvability in two dimensions and the Yang–Mills measureDriver, Gross–King–Sengupta, Lévy, reconstruction by stochastic quantisation5-01
6-03Constructing scalar fieldsφ⁴₂, φ⁴₃, the Glimm–Jaffe road6-01
6-04The cluster expansionAs a tool6-03
6-05The sequence of renormalisation group stepsThe ideas behind Bałaban's method (blocking, large fields, local gauges)6-01, 4-04
6-06Ultraviolet stability of three-dimensional Yang–MillsWhat has been shown, and what is not yet constructed6-05
6-07Four dimensionsBałaban and Magnen–Rivasseau–Sénéor — what "the level of control" means6-05
6-08Triviality of φ⁴ in four dimensionsThe triviality theorem (Aizenman–Duminil-Copin) and the requirements for non-triviality6-03
6-09Stochastic quantisation and regularity structuresHairer, CCHS, Chevyrev–Shen, subcritical and critical6-01, 1-09
6-10Where four dimensions stopsStage by stage, the words of the problem's authors6-07
6-11Obstacles other than divergenceSix of them6-10
6-12Detour: "if 1/0 is given a symbol""If 1/0 were given a symbol" — the algebra of divergences and exp(−1/g²)4-05, 4-12

Part 7 From the side of physics

Ch.TitleContentsPrereq.
7-01How physics sees itAsymptotic freedom, dimensional transmutation, the picture of confinement, the premise that "the theory exists"4-07
7-02Mechanisms of confinementDual superconductivity, monopoles, centre vortices, Gribov–Zwanziger7-01
7-03The string pictureNambu–Goto, the Lüscher term, fluctuations of the tube, the Wulff shape7-01
7-04Large N't Hooft, planar diagrams, random surfaces4-03
7-05String theory and extra dimensionsWhere 26, 10 and 11 dimensions come from7-04
7-06How extra dimensions become invisibleKaluza–Klein, Calabi–Yau, branes, experimental lower bounds7-05
7-07Where gauge fields come fromD-branes, heterotic strings, geometric engineering7-06
7-08HolographyA first look at AdS/CFT, radius = scale, correspondences that can be written exactly7-05
7-09The mass gap becomes geometryWitten 1998, the cigar, Klebanov–Strassler, glueball numbers7-08
7-10Back to four dimensionsThe order of limits, the non-separation of KK, N→∞, λ→∞, the distance from the problem statement7-09
7-11Supersymmetry and Seiberg–WittenAn example where duality makes the gap visible (at the level of physics)7-08
7-12The sentence that plays the role of an equivalence principleOne scale, Assumption H, the three chains7-01, 4-07
7-13Where the way physics digs parts from mathematics7-10

Part 8 A dictionary of two languages — the physical and the mathematical view

Ch.TitleContentsPrereq.
8-01How to read the dictionaryThe degree of certainty of each correspondence is given in **two columns** — (a) the correspondence as a definition (settled = the same as a theorem / conditional / unsettled) and (b) its reality in four-dimensional Yang–Mills (constructed / conditional / absent). Which language to take as primary, and who judges that two things are "the same" (a theorem or a convention)0-03
8-02Dictionary AThe theory itself — path integral / Feynman–Kac, functional integral / Euclidean measure, vacuum / ground state / uniqueness of the measure, particle / isolated eigenvalue of the mass operator, S-matrix / Haag–Ruelle, Wick rotation / OS reconstruction, unitarity / reflection positivity, Green functions / Wightman–Schwinger, gauge fixing / a section of the orbit space, spacetime / R⁴ and the lattice, regularisation / the lattice spacing, Hamiltonian / transfer matrix, physical states / reconstruction from gauge invariants, renormalisability / BPHZ, field / operator-valued distribution, Källén–Lehmann / the spectral measure of the transfer matrix, Elitzur's theorem4-02, 4-10
8-03Dictionary BMass and length — the mass gap / exponential decay of correlations, the correlation length / inverse mass, V(R) / Wilson loops, the string tension / the coefficient of the area law, three ways of saying confinement (V→∞, σ>0, centre symmetry), Λ and dimensional transmutation / one scale, glueballs / one-particle states (reality unsettled), **two times** (the Hamiltonian H_T of the transfer matrix and the Fokker–Planck generator L of Langevin, gaps 1/ξ and 1/C_P), autocorrelation / the Poincaré constant (equality only for reversible continuous-time dynamics, HMC is separate), the conventional theory of critical slowing down (van Hove, z=2−η_s) and the RG (Halperin–Hohenberg–Ma 1972), the lower bound z≥γ/ν, static η_s and dynamic η_dyn, m/√σ / the limit of dimensionless ratios (Problem 5.1), the Lüscher term / effective strings, roughening / Wulff, freezing of topological charge / bottlenecks in the state space4-11, 5-08, 2-08
8-04Dictionary CScale and limits — the renormalisation group / a sequence of steps, the β function / the flow of the effective coupling, the continuum limit / the scaling limit, universality / uniqueness of the limit, a(β) (the ε(β) of Problem 5.2 is existentially quantified over Wilson loops), the distinction between scaling and asymptotic scaling, Symanzik O(a²) (the expansion variable differs from that of δ(b)), the Δβ of MCRG and the scheme change of Λ (Dashen–Gross), Migdal–Kadanoff / hierarchical lattices, large N / planar graphs, the master field, the holographic radius / the RG scale, topological charge / the second Chern number (admissible), instantons / self-dual connections, Wilson flow / gradient flow, the KK tower / the first eigenvalue of the internal Laplacian, Polchinski's ERG / multiscale Bakry–Émery, the Gribov region / convexity of the positive domain of the FP operator, the clash between improved actions and reflection positivity, the trace anomaly (no counterpart word on the mathematical side)4-06, 6-05, 7-08
8-05The physical counterparts of our assumptions**as questions and analogies**): Assumption H is the slowest relaxation of Langevin and is exact for the free field — does it have a name on the physical side? / Is H↓ the same thing as the lower bound "local dynamics cannot relax faster than the susceptibility" (z≥γ/ν = 2−η_s)? / Is H↑ ⟺ z≤2 a restatement under the dynamic scaling hypothesis (the HH hypothesis only states that z exists)? / The η of the record refers to two quantities (the static η_s of §1 and the dynamic η_dyn of §6.27), and 8-05 fixes it to one / Is the summability of δ(b) closer to the Δβ and scheme change of MCRG than to Symanzik? / Is (S4)⟺Σδ∧η=0 the combination of "mass is RG-invariant" and "z=2"? / Is "one scale ⟺ the extra dimensions are visible" an analogy with the non-separation of KK? / What is settled as known (the correction of direction = Problem 5.1, κ=4Nb₀, Migdal–Kadanoff, (S2)) is written as such. Our side's definitions are cited from 7-12 and 10-03 (10-03 after renumbering), and detailed derivations are left to later parts (this does not go against the order of the contents8-03, 8-04, 7-12

Part 9 Where things stand, and open tasks

Ch.TitleContentsPrereq.
9-01How far the world has comeA timeline, and a table by dimension6-10
9-02Where the two ways of digging partThe seven seams6-11, 7-13
9-03Candidates for new conceptsWhat plays the role of "Ricci flow"6-09
9-04The list of open tasksWhat would move if what were known9-02
9-05Common misconceptions"Infinities are the centre", "two and three dimensions are done", "because it is non-abelian", "the mass of a particle"0-03

Part 10 Towards a proof of the mass gap — building the first step of the staircase

Ch.TitleContentsPrereq.
10-00Entrance — the staircase, and the random walk, the ruler and the clockA map of the part, the four steps of the staircase, the five quantities as metaphors, Assumption H in one sentence [Y2]2-10, 4-11, 2-07
10-01The line of construction and Assumption H(S1)–(S8), the direction of the lattice version, the three C_P, Assumption H in six stages (the statement, what it gives, what it does not give, the one-sided bridge) [Y2]–[Y3]10-00, 5-09
10-02Roads tried on the four-dimensional lattice, and wallsOne step of bookkeeping, the seventeen roads G0–G15′, the twenty-one walls GA1–GE4, why we go down to the first step [Y3]10-01, 5-11
10-03The four steps of the staircase — why we start from 0+1 dimensionsThe definition of the four steps, the conditions on the model of the first step, the power form of H, what lifts [Y2]10-01
10-04The path measure of the double well, and kinksThe path measure, ξ and the tunnelling splitting, kinks and the diffusion coefficient, the lower bound C_P≥ξ² (Proposition L) [Y2]–[Y3]10-03, 2-05, 2-07
10-05The statement of the first step — four conditions and Proposition 4.5The splitting of the variance, conditions (H1)–(H4), Proposition 4.5 as a single line, the dependency graph [Y3]10-04
10-06(H1) Local Poincaré within a phaseProposition H1 (six nodes), the methods and costs between nodes [Res]10-05
10-07The map of (H2) — seven routes and the seam of the ringThe state of routes 1–7, the chain outside and the chain inside the ring [Y3]10-05
10-08What computer-assisted means — the conditions on the chain inside the windowInterval arithmetic, premises, an example of the chain outside the window, what is not said [Y2]–[Y3]10-07
10-09The sector framework and the three strands of route 5Five stages, the conditions for closing, the three strands, the common wall [Res]10-07
10-10The list of detour plans — types of breakageR1–R24, the line that killed it, seven types [Y3]–[Res]10-09
10-11(H3)(H4) and the constant of the coreProposition H3, the product of boxes, Proposition H4, Proposition CORE3, the set of ends [Res]10-05
10-12The integrated table and the dependency graphThe 111-row table in the five grades, the numbering rules, that there is no ħ that fits all, the required set of leaves [Y3]10-06, 10-07, 10-09, 10-11
10-13Lean statements and the limits of machine checkingThe list of bundles, the criterion of cleanliness, four limits, translating conventions [Y2]–[Y3]10-12
10-14Reconciliation — the numbers of the record and the known numbersThe distance from known theorems, checking the bibliography, positive controls, nineteen rows on the four-dimensional lattice [Y3]10-12
10-15What remains and its cost — the distance to a theoremThe rows and work needed for each of the two roads, estimates of cost, a ħ that fits all, the distance from the second step on [Y3]10-12
10-16What is not claimedA table matching the fourteen items to the text, three meanings [Y2]—
10-17Insights and small questionsTwelve ideas and small questions, discarded hypotheses, Q1–Q17 [Y2]–[Y3]10-12

Part 11 Further considerations — beyond Assumption H, and other views

Ch.TitleContentsPrereq.
11-00Further considerations — entrancePositioning, the sentences received from Part 10, a map of the nine chapters and what each chapter can say [Y2]10-00, 10-01
11-01One form that obstructs H — a nearly conserved global quantityFive examples in one type, three strengths, two ways of counting the charge of a subregion [Y3]10-01, 10-02, 2-10
11-02Choosing the ruler and the coordinates again — the length at which conservation breaksThree rulers, coordinates and Dirichlet forms, five points of the band for two-dimensional U(1), a two-dimensional test bed [Y3]11-01, 10-01, 2-10
11-03Two ways to repair H — the sector H and the local HDefinitions of the local H and the sector H, the ratio form and references, open boxes and closed boxes [Res]11-01, 10-01, 10-11
11-04Which H the one-sided bridge needsFamilies local in time, the window bridge and Proposition W, thresholds and three references, a note on 0+1 [Res]11-03, 10-01
11-05Making time continuous — the Hamiltonian lattice and the vacuum measureProposition V (the gap = the Poincaré constant of the vacuum measure), three Poincaré constants, the Kogut–Susskind lattice [Y3]11-04, 10-01, 2-05
11-06Paying with rarity instead of convexity — renormalisation on groups and log-SobolevA lemma on the ceiling of convexity, the reversal of where things are convex and non-convex, tools for paying with rarity, a class of measures that pay with rarity (candidates), stochastic quantisation [Res]11-02, 10-09, 10-10, 10-11
11-07Because it is four dimensions — the dimensionless coupling and topologyTwo points: the critical dimension and topology, the hurdles of the four steps, why the mathematics of the third step does not exist, physical mechanisms [Y3]11-01, 11-02, 10-03, 10-15, 4-07, 6-07
11-08Questions, and what is not claimedThe table of questions F1–F19, a list of candidate rules, the sixteen items that are not claimed [Y2]–[Y3]10-16
11-A1Table of notation for Part 11Symbols, where they are defined, units, correspondence with Part 10 (pages of reference)10-01, A-01

Appendices

Ch.TitleContentsPrereq.
A-01Table of notation—
A-02Glossary1–3 lines each, links to chapters—
A-03Guide to the literaturePrimary sources, reviews, textbooks (with their availability)—
A-04Lean and machine checkingA guide to `../lean-guide/`, and the labels used in this book—
A-05How this book was madeThe verification procedure (for readers; the internal history is not written)—
A-06Index of assumptionsH, H↑, H↓, H_band[normalised], (P), T(c,1), (S1)–(S8), the chains (i)(ii)(iii), η_dyn, θ, δ, κ, ℰ_ϑ / ℰ_A, in a table of symbol, one-line meaning, chapter where it is placed, and status (assumption / algebra closed in Lean / known). The table "eight readings of Assumption H" (10-03) is reproduced—

02

Reading orders — five of them

I want to know first what the problem is

0-02 One picture → 0-03 Reading the problem statement word by word → 0-04 Four dimensions in mathematics and four dimensions in physics → 9-02 The seven seams → 9-05 Common misconceptions. No tools are needed. By this point the "shape" of the problem is visible.

I want to dig from the mathematical side

Part 1 (only where needed) → Part 3 → 4-02, 4-10, 4-11 of Part 4 → Part 5 → Part 6 → 9-03 Candidates for new concepts. This follows the road of those who construct existence, in order from regularisation to the axioms.

I want to dig from the physical side

Part 2 (only where needed) → Part 3 → 4-06, 4-07 of Part 4 → 5-07, 5-08 of Part 5 → Part 7 → 9-02 The seven seams. The road of those who measure what exists, the limit that brings extra dimensions back to four, and as far as the sentence that plays the role of an equivalence principle.

I want to follow the study in Part 10

10-00 Entrance → 10-01 The line of construction and Assumption H → 10-03 The four steps of the staircase → 10-04 The double well → 10-05 The statement of the first step → 10-12 The integrated table → 10-15 What remains and its cost → 10-16 What is not claimed. With Assumption H as the axis, this splits the claim of the first step into conditions and follows it in order up to what remains and what is not claimed. The prerequisites are 2-05, 2-07, 2-10 of Part 2 and 4-11, 5-09, 5-11 of Parts 4 and 5.

I want to follow Part 11

11-00 Entrance → 11-01 A nearly conserved global quantity → 11-03 The sector H and the local H → 11-04 Which H the one-sided bridge needs → 11-05 The Hamiltonian lattice and the vacuum measure → 11-08 Questions, and what is not claimed. Reading 10-00 and 10-01 of Part 10 first makes the meaning of the received sentences clear.


03

Related articles

Revised 2026-09-26: first version. Set out the frame of the contents and the reading orders.
2026-10-09: Part 10 reorganised into eighteen chapters (the old 14 pages are kept as guide pages); added the nine chapters of Part 11 "Further considerations" and the table of notation. Added two reading orders.