The whole book Contents and reading orders
- Part 0 Entrance — how to read this book
- 0-01 How to read this book
- 0-02 One picture
- 0-03 Reading the problem statement word by word
- 0-04 Four dimensions in mathematics and four dimensions in physics
- Part 1 Mathematical preparation
- 1-01 Vector spaces and linear maps
- 1-02 What a group is
- 1-03 Lie groups and Lie algebras
- 1-04 SU(2) and SU(3)
- 1-05 Manifolds and tangent spaces
- 1-06 Differential forms and the exterior derivative
- 1-07 Vector bundles and connections
- 1-08 Probability and measure
- 1-09 Probability in infinite dimensions
- 1-10 Hilbert spaces and self-adjoint operators
- 1-11 Fourier analysis and distributions
- 1-12 Detour: what happens only in four dimensions
- Part 2 Physical preparation
- 2-01 Lagrangians and the action
- 2-02 The idea of a field
- 2-03 Electromagnetism is a gauge theory
- 2-04 Special relativity and spacetime
- 2-05 The bones of quantum mechanics
- 2-06 The harmonic oscillator and creation and annihilation
- 2-07 The idea of the path integral
- 2-08 Statistical mechanics and phase transitions
- 2-09 Detour: the gap and the correlation length in the Ising model
- 2-10 The relaxation time and the dynamical exponent z
- Part 3 Yang–Mills theory (classical)
- 3-01 The gauge principle
- 3-02 Non-abelian gauge fields
- 3-03 The action and the equations
- 3-04 Gauge theory as geometry
- 3-05 Instantons and topology
- 3-06 Detour: Donaldson and exotic R⁴
- 3-07 Yang–Mills inside the Standard Model
- Part 4 Quantisation
- 4-01 Canonical quantisation and the Hamiltonian
- 4-02 The path integral and Euclideanisation
- 4-03 Perturbation theory and Feynman diagrams
- 4-04 Divergences and renormalisation
- 4-05 The algebra of divergences
- 4-06 Asymptotic freedom
- 4-07 Dimensional transmutation and Λ
- 4-08 Gauge fixing and Faddeev–Popov
- 4-09 The axioms of quantum field theory
- 4-10 The Osterwalder–Schrader axioms and reconstruction
- 4-11 The definition of the mass gap
- 4-12 Detour: the perturbation series diverges
- Part 5 Lattice gauge theory
- 5-01 Wilson's lattice
- 5-02 The strong-coupling expansion
- 5-03 Reflection positivity and the transfer matrix
- 5-04 The infinite-volume limit and the cluster expansion
- 5-05 Weak coupling and the continuum limit
- 5-06 How U(1) differs from the non-abelian case
- 5-07 The Monte Carlo method
- 5-08 Measuring glueballs and the string tension
- 5-09 What to hold fixed when taking the limit
- 5-10 Lattice gauge theory with finite groups
- 5-11 Detour: Bakry–Émery and one-link integration
- Part 6 Constructive field theory
- 6-01 What constructive field theory is
- 6-02 Solvability in two dimensions and the Yang–Mills measure
- 6-03 Constructing scalar fields
- 6-04 The cluster expansion
- 6-05 The sequence of renormalisation group steps
- 6-06 Ultraviolet stability of three-dimensional Yang–Mills
- 6-07 Four dimensions
- 6-08 Triviality of φ⁴ in four dimensions
- 6-09 Stochastic quantisation and regularity structures
- 6-10 Where four dimensions stops
- 6-11 Obstacles other than divergence
- 6-12 Detour: "if 1/0 is given a symbol"
- Part 7 From the side of physics
- 7-01 How physics sees it
- 7-02 Mechanisms of confinement
- 7-03 The string picture
- 7-04 Large N
- 7-05 String theory and extra dimensions
- 7-06 How extra dimensions become invisible
- 7-07 Where gauge fields come from
- 7-08 Holography
- 7-09 The mass gap becomes geometry
- 7-10 Back to four dimensions
- 7-11 Supersymmetry and Seiberg–Witten
- 7-12 The sentence that plays the role of an equivalence principle
- 7-13 Where the way physics digs parts from mathematics
- Part 8 A dictionary of two languages — the physical and the mathematical view
- 8-01 How to read the dictionary
- 8-02 Dictionary A
- 8-03 Dictionary B
- 8-04 Dictionary C
- 8-05 The physical counterparts of our assumptions
- Part 9 Where things stand, and open tasks
- 9-01 How far the world has come
- 9-02 Where the two ways of digging part
- 9-03 Candidates for new concepts
- 9-04 The list of open tasks
- 9-05 Common misconceptions
- Part 10 Towards a proof of the mass gap — building the first step of the staircase
- 10-00 Entrance — the staircase, and the random walk, the ruler and the clock
- 10-01 The line of construction and Assumption H
- 10-02 Roads tried on the four-dimensional lattice, and walls
- 10-03 The four steps of the staircase — why we start from 0+1 dimensions
- 10-04 The path measure of the double well, and kinks
- 10-05 The statement of the first step — four conditions and Proposition 4.5
- 10-06 (H1) Local Poincaré within a phase
- 10-07 The map of (H2) — seven routes and the seam of the ring
- 10-08 What computer-assisted means — the conditions on the chain inside the window
- 10-09 The sector framework and the three strands of route 5
- 10-10 The list of detour plans — types of breakage
- 10-11 (H3)(H4) and the constant of the core
- 10-12 The integrated table and the dependency graph
- 10-13 Lean statements and the limits of machine checking
- 10-14 Reconciliation — the numbers of the record and the known numbers
- 10-15 What remains and its cost — the distance to a theorem
- 10-16 What is not claimed
- 10-17 Insights and small questions
- Part 11 Further considerations — beyond Assumption H, and other views
- 11-00 Further considerations — entrance
- 11-01 One form that obstructs H — a nearly conserved global quantity
- 11-02 Choosing the ruler and the coordinates again — the length at which conservation breaks
- 11-03 Two ways to repair H — the sector H and the local H
- 11-04 Which H the one-sided bridge needs
- 11-05 Making time continuous — the Hamiltonian lattice and the vacuum measure
- 11-06 Paying with rarity instead of convexity — renormalisation on groups and log-Sobolev
- 11-07 Because it is four dimensions — the dimensionless coupling and topology
- 11-08 Questions, and what is not claimed
- 11-A1 Table of notation for Part 11
- Appendices
- A-01 Table of notation
- A-02 Glossary
- A-03 Guide to the literature
- A-04 Lean and machine checking
- A-05 How this book was made
- A-06 Index of assumptions
The integrated table and the dependency graph
What this chapter shows — For the four conditions (H1)–(H4) of the first step, we put every row of the tables of the five grades of 10-05, 10-06, 10-07, 10-09 and 10-11 into one table, and renumber the five dependency graphs and join them into one. We put it in a form in which readers can check by the rule of numbering (the number of a premise is smaller than the number of a conclusion) that there is no circle, and we see in figures where the computer-assisted rows lie on the road to the conclusion, and that there is still no at which all rows are in place together.
Prerequisite chapters — 10-05 §07 (the format of the dependency graph), 10-06 §05, 10-07 §05, 10-09 §07, 10-11 §08 (the table of each condition), 10-00 §01 (the labels of the five grades).
Said first — The level is [Y3]. The integrated table is a map of "how far things are shown, and where assumption begins"; it is not a ruler for measuring progress. This part places Assumption H at the axis of the study, and this chapter lays out on one sheet the whole construction of its first step.
- How the integrated table is made — the rules for putting five tables on one sheet, how identical rows are merged, the meaning of the columns
- The integrated table — every row of the first step (Table 1), and the number of rows per grade (Table 2)
- The dependency graph — the trunk (Figure 1) and the whole, how to check that there is no circle, and that the assumption rows do not contain the quantity of the conclusion
- The family of bridges — Proposition L (one-dimensional version) and Proposition B (multi-dimensional version)
- The position of the computer-assisted rows — what is on the road to the conclusion and what is not
- There is no at which all rows are in place — bands of the range (Figure 2, Table 4), and what is needed to bring them into line
- The rows needed to reach the power form of H — two ways of supporting the row of the core (Table 5)
- A note on how to read it — a map, not a fraction
How the integrated table is made — putting five tables on one sheet
The claim of the first step is Proposition 4.5 (10-05 §04): on conditions (H1)–(H4) and the premise rows, , and hence the power form of H, . Each of the four conditions is written in its own chapter as a table of rows in the five grades (Proved here, Cited, Computer-assisted, Reading, Assumption) and as a dependency graph of numbered nodes. In this chapter we put them on one sheet by the following rules.
- Count by rows. The unit is each row of the tables, not the name of a condition (whether (H1) is "closed"). This is because it is usual for rows with proofs and assumption rows to be mixed within one condition.
- Make identical rows one. When the same statement appears in two chapters, we make it one row and write the nodes of both chapters in the source column. For example, [14] of 10-05 and [19] of 10-11 are both Proposition H3, and row LSW of 10-07 and [06] of 10-09 are both the remaining single proposition (LSW♭). Row (T0′P) of 10-05 ([04]) is supported in 10-11 by the pair of Proposition CORE3 and the local term, and in 10-07 and 10-09 by the lower bound of the core on the sector side, so we made it one node with an "or" of the two ways of support.
- Rows left out. The rows of the list of detour plans (10-10) are not included, because none of them is a premise of any conclusion of the present construction. Of the rows of 10-04, the uniqueness of the measure is included in the common premise row P0, and the remaining spectrum of the fluctuation operator (of Pöschl–Teller type) is included as a single explanatory row.
- Line up the family of bridges. Proposition L (10-04 §04) and Proposition B (10-01 §06) are the one-dimensional and multi-dimensional versions of the same bridge, "the relaxation time of the path measure is at least the square of the correlation length", so we included them as a family of adjacent nodes (§04). The other rows of Table 8 of 10-01 (H↑, H↓ and the rereading of mass, the chain, the version with discrete time, the step of infinite volume) do not enter the road to the conclusion of the first step, so they stay in the graph of 10-01.
The columns of Table 1 are as follows. No. is the number of the node in the dependency graph of §03; Symbol is the short name of the row; Grade is the label of the five grades; Range of is what the row speaks about (nodes, window, three points, independent of , , or "—" for not shown at any ); Condition is which condition the row belongs to; Premise of which conclusion gives the numbers of the nodes that take the row as a direct premise, and whether following the edges of implication reaches the final conclusion (the power form of H); Source gives the tables and graph nodes of each chapter. Machine checking (Lean theorem names and assumptions) is placed under each row of the graph in §03.
The integrated table — every row of the first step
Table 1 is divided into five blocks by grade (within a block, in the order of the graph numbers). The smaller the number, the more it is a leaf (Assumption, Cited, Computer-assisted, Reading); the larger, the more it is a step of the construction; the last, [111], is the power form of H.
| No. | Symbol | Content (one line) | Grade | Range of ħ | Condition | Premise of which conclusion | Source (chapter nodes) |
|---|---|---|---|---|---|---|---|
| Assumption Assumption rows (put without proof) (30 rows) | |||||||
| [001] | P0 | Uniqueness of the measure at T=∞, Markov property, extension from local functions, the limit step, regularity | Assumption | — | Common | [071][073][077][081][106]. To the power form of H: reaches | 10-05 [01], 10-11 [01], 10-04 §01 |
| [002] | TUBE | (H2tube) Poincaré for the tube, uniform in tube length ≤ Cξ | Assumption | — | (H2) | [075]. To the power form of H: reaches | 10-05 [03], 10-11 [04] |
| [003] | KG | (KG) The box gap of the reduced kink gas is of the Glauber type | Assumption | — | (H4) | [075]. To the power form of H: reaches | 10-05 [05], 10-11 [05] |
| [004] | GLA | Closed formula for the gap of the Glauber box with fixed ends (original source bibliographic only) | Assumption | — | (H4) | Premise of no node. Part of the content of (KG) (a reading not made an independent node in the graph) | 10-11 Table 6 GLA |
| [005] | X | (X) Cross term ℰ_Y(E[f|Y]) ≤ (1+χ)ℰ(f), χ uniform | Assumption | — | (H4) | [075]. To the power form of H: reaches | 10-05 [06], 10-11 [06] |
| [006] | MXA | (MIX_alt) The alternating maximal correlation between boxes c_alt < 1 is uniform | Assumption | — | (H3) | [072]. To the power form of H: reaches | 10-05 [07], 10-11 [02] |
| [007] | MXC | (MIX_core) Upper bound for the alternating maximal correlation in the core c̄ < 1 (k ≥ 15) | Assumption | — | (H2) | [082]. To the power form of H: reaches | 10-11 [07] |
| [008] | DSC | (ΔS_core) C_P ≤ c ħ^(−p) e^(ΔS/ħ) for core and window | Assumption | — | (H2) | [084]. To the power form of H: reaches | 10-11 [08] |
| [009] | A5 | Continuous version of Holley's comparison (the tail lemma) | Assumption | Six nodes | (H1) | [061]. To the power form of H: reaches | 10-06 [05] |
| [010] | A10 | The Poincaré–Miranda theorem (covering by boxes) | Assumption | (0,0.2] | (H1) | [063]. To the power form of H: reaches | 10-06 [08] |
| [011] | A15 | (T5) Regularity and density of the functions used | Assumption | — | (H1) | [060]. To the power form of H: reaches | 10-06 [10] |
| [012] | B1 | (T1b) Neighbour and end values > 2.5 | Assumption | — | (H1) | [068]. To the power form of H: reaches | 10-06 Table 2 B1 |
| [013] | B2 | (T1c) ħ between the nodes (in uniform form) | Assumption | Outside the nodes | (H1) | [068]. To the power form of H: reaches | 10-06 Table 2 B2 |
| [014] | B3 | (T1c) ħ < 0.005 (in uniform form) | Assumption | — | (H1) | [068]. To the power form of H: reaches | 10-06 Table 2 B3 |
| [015] | B4 | (T3d) End values of the two sites > 4 | Assumption | — | (H1) | [068]. To the power form of H: reaches | 10-06 Table 2 B4 |
| [016] | B5 | Transfer from the ring to scraps (with end values) | Assumption | — | (H1) | [068]. To the power form of H: reaches | 10-06 Table 2 B5 |
| [017] | IA | Premises of interval arithmetic (IEEE correct rounding, errors of sums, our own exp) | Assumption | — | (H2) | [042][043]. To the power form of H: does not reach | 10-07 [01], 10-08 §03 |
| [018] | LIM | (lim), (END_rand), regularity at the seam of the ring | Assumption | — | (H2) | [043][099][103]. To the power form of H: reaches | 10-07 [02] |
| [019] | SM | The small assumptions of route 4 (inputs to the sectors) | Assumption | — | (H2) | [099]. To the power form of H: reaches | 10-07 [04] |
| [020] | PROD | Proposition LSσ_W (construction of the upper bound for A_W of the product form) | Assumption | — | (H2) | [102]. To the power form of H: does not reach | 10-07 [05] |
| [021] | LSWin | Input (LS_W) (the form of LSI for the marginals of site windows) | Assumption | — | (H2) | [087]. To the power form of H: reaches | 10-09 [01] |
| [022] | PF | (PF_seg) (locality of volume on the bridge) | Assumption | — | (H2) | [089]. To the power form of H: reaches | 10-09 [02] |
| [023] | BAR | Barta's row κ = 3/1000, b = 493/1000 | Assumption | Independent of ħ | (H2) | [092]. To the power form of H: reaches | 10-09 [03] |
| [024] | REG | The boundary term of Bochner and regularity of eigenfunctions | Assumption | — | (H2) | [090][092]. To the power form of H: reaches | 10-09 [04] |
| [025] | PROX | The provisional rows of Proposition P5 (lifting assumption, Spec and others) | Assumption | — | (H2) | [096]. To the power form of H: does not reach | 10-09 [05] |
| [026] | LSWb | (LS_W♭) A_W < A_max(ħ): the remaining single proposition of route 5 | Assumption | — | (H2) | [099]. To the power form of H: reaches | 10-09 [06], 10-07 [03] |
| [027] | K3 | The next eigenvalue 3/4 of the fluctuation operator (of Pöschl–Teller type) | Assumption | Independent of ħ | Explanation | Premise of no node. An explanatory row that does not enter the premises of the conclusion of the first step | 10-04 Table 3 K3 |
| [028] | SPEC1 | (A1) Discreteness of the spectrum, simplicity and positivity of the ground state (finite spatial lattice) | Assumption | — | Bridge | [107][108]. To the power form of H: does not reach | 10-01 [06] |
| [029] | KU | (A3) κ uniform in β (the graduation of the multi-dimensional version) | Assumption | — | Bridge | [109]. To the power form of H: does not reach | 10-01 [08] |
| [096] | P5 | Proposition P5 (the lower end of the window, with a table of assumptions) | Assumption | 8 nodes | (H2) | Premise of no node. A candidate to support the remaining single proposition (LS_W♭), with no edge of implication | 10-09 [21] |
| Cited Rows citing an original source (10 rows) | |||||||
| [030] | MOB | Mobility of a single kink D = ħ/S₀ (at the level of the process) | Cited | ħ→0 | (H4) | [075][105]. To the power form of H: reaches | 10-05 [08], 10-11 [09] |
| [031] | BE | Bakry–Émery on convex domains (Kolesnikov–Milman) | Cited | Independent of ħ | (H2) | [076]. To the power form of H: reaches | 10-11 [10] |
| [032] | A3 | Muckenhoupt's bracket B ≤ C_P ≤ 4B | Cited | Independent of ħ | (H1) | [061]. To the power form of H: reaches | 10-06 [03] |
| [033] | A4 | Correlation inequality for MTP₂ (monotonicity of e, ħκ ≥ 0) | Cited | Independent of ħ | (H1) | [061]. To the power form of H: reaches | 10-06 [04] |
| [034] | A6 | Poincaré version of Helffer's criterion (Ledoux Proposition 3.1) | Cited | Independent of ħ | (H1) | [062]. To the power form of H: reaches | 10-06 [06] |
| [035] | A12 | Brascamp–Lieb (the cross κ_f, (T4)) | Cited | Independent of ħ | (H1) | [063][064]. To the power form of H: reaches | 10-06 [09] |
| [036] | BOC | Integral form of Bochner's formula (Ledoux Proposition 1.3) | Cited | Independent of ħ | (H2) | [090][092]. To the power form of H: reaches | 10-09 [07] |
| [037] | SV | Singular-value representation of maximal correlation (Witsenhausen) | Cited | — | (H2) | Premise of no node. A representation used for how the reading values of Stage 2 are obtained | 10-11 Table 6 SV |
| [038] | KR | For Gaussians, maximal correlation = linear canonical correlation (Kolmogorov–Rozanov) | Cited | — | (H2) | Premise of no node. Used for reading Proposition G | 10-11 Table 6 KR |
| [039] | CORR | (A2) Formula for correlations of the stationary path measure | Cited | T=∞ | Bridge | [108]. To the power form of H: does not reach | 10-01 [07] |
| Computer-assisted Computer-assisted rows (4 rows) | |||||||
| [040] | A1 | (T1a) Margin ħρ − 2ħκ ≥ 0.067 (neighbour and end in [0,2.5]²) | Computer-assisted | Six nodes | (H1) | [061]. To the power form of H: reaches (only by the road on which it joins the Assumptions B1–B5 at [068]) | 10-06 [01] |
| [041] | A9 | (T3) λ_c ≥ 1.3×10⁻⁴ (ends in [0,4]²) | Computer-assisted | (0,0.2] | (H1) | [063][064]. To the power form of H: reaches (only by the road on which it joins the Assumptions B1–B5 at [068]) | 10-06 [07] |
| [042] | QF | q_free ≤ 0.998854904 (the chain outside the window) | Computer-assisted | Window | (H2) | [100]. To the power form of H: does not reach | 10-07 [09] |
| [043] | QO | q_out ≤ 0.998888530 (the outer chain of the ring, pin ≤ 0) | Computer-assisted | Window | (H2) | [101]. To the power form of H: does not reach | 10-07 [10] |
| Reading Reading rows (19 rows) | |||||||
| [044] | XI | ln ξ ≥ s/ħ (ξ ∝ ħ^½ e^(S₀/ħ)), the size of D/(Cξ)² | Reading | Three points, leading term | Conclusion | [084][111]. To the power form of H: reaches | 10-05 [09], 10-11 [11] |
| [045] | CAL | c_alt = 0.731 / 0.410 / 0.138 (C = 2 / 4 / 8) | Reading | Model | (H3) | Premise of no node | 10-11 [12] |
| [046] | MC2 | Two-point maximal correlation of Stage 2 and B₂ (22.1 / 30.5 / 66.4) | Reading | Three points | (H2) | [082]. To the power form of H: reaches | 10-11 [13] |
| [047] | CB | c̄_(≥15) ≤ 0.535 (measurement of a lower bound) | Reading | Three points | (H2) | [082]. To the power form of H: reaches | 10-11 [14] |
| [048] | BIS | Bistability of the core on the box side, the fibres of the binary of the bump | Reading | Three points | (H2) | Premise of no node | 10-11 [15] |
| [049] | CTL | Positive controls for Proposition H3 (pure Gaussian, Ising) | Reading | — | (H3) | Premise of no node | 10-11 Table 6 CTL |
| [050] | KV | K ≈ 2.76 / 1.43 (C = 2), 1.78 (C = 4), and c_ff for free ends | Reading | Model | (H4) | Premise of no node | 10-05 Kv, 10-11 CFF |
| [051] | DSV | ΔS⁰_* ≤ 1.4·10⁻² (ratio to 2S₀ ≤ 1.05·10⁻²) | Reading | ħ = 0 | (H2) | Premise of no node | 10-11 Table 6 DSV |
| [052] | N2 | The constants of route 2 π_*, Λ, C_1D, gap_W, the inner chain of the bridge | Reading | Three points | (H2) | [102]. To the power form of H: does not reach | 10-07 [06] |
| [053] | QIN | The inner chain of the ring q_in ≈ 1.24–1.28 | Reading | Four points | (H2) | [101]. To the power form of H: does not reach | 10-07 [07] |
| [054] | EDGE | The boundary stage q ≈ 1.004–1.045 | Reading | Four points | (H2) | [101]. To the power form of H: does not reach | 10-07 [08] |
| [055] | ELL | ℓ_min = 38.3 / 121.9 / 406.8 | Reading | Three points | (H2) | [089][094]. To the power form of H: reaches | 10-09 [08] |
| [056] | AWV | Upper bound of A_W 1857 / 2794 / 9106, lower bound 1.71 / 1.74 / 2.59 | Reading | Three points | (H2) | Premise of no node | 10-09 [09] |
| [057] | ST3 | How far strand 3 got (reading 0.54 times, paper upper bound 10³ times) | Reading | Two points | (H2) | Premise of no node | 10-09 [23] |
| [067] | A18 | C ≤ 658 (numerical input) | Reading | Six nodes | (H1) | Premise of no node | 10-06 Table 2 A18 |
| [089] | S4 | (Σ.4) ℓ_min does not depend on k | Reading | Three points | (H2) | [092]. To the power form of H: reaches | 10-09 [14] |
| [094] | AM2 | Needed value 25.1 / 90.3 / 312.3 | Reading | Three points | (H2) | [097]. To the power form of H: does not reach | 10-09 [19] |
| [097] | ST1 | How far strand 1 got (1.4–5.5 times the needed value) | Reading | Three points | (H2) | Premise of no node | 10-09 [22] |
| [102] | AV | A_W of the product form ≈ 2.5·10⁶–4.7·10⁷ | Reading | Three points | (H2) | Premise of no node | 10-07 [14] |
| Proved here Rows with proofs (elementary proofs, algebra on named premises) (48 rows) | |||||||
| [058] | A2 | Lemma K2 (second-order Taylor of the tilt and the Hölder remainder) | Proved here | Independent of ħ | (H1) | [061]. To the power form of H: reaches | 10-06 [02] |
| [059] | A8 | (T2) The marginal of the kept sites is a nearest-neighbour chain | Proved here | Independent of ħ | (H1) | [062]. To the power form of H: reaches | 10-06 [11] |
| [060] | A14 | (T5) Decomposition of the variance | Proved here | Independent of ħ | (H1) | [065]. To the power form of H: reaches | 10-06 [12] |
| [061] | MARG | The continuum statement of the margin λ | Proved here | Six nodes | (H1) | [062]. To the power form of H: reaches | 10-06 [13] |
| [062] | A7 | Gap on the coarse side ≥ λ (Gershgorin on the ring) | Proved here | Six nodes | (H1) | [065]. To the power form of H: reaches | 10-06 [14] |
| [063] | A11 | Nesting λ_S ≥ 2.3×10⁻⁵ | Proved here | (0,0.2] | (H1) | [065]. To the power form of H: reaches | 10-06 [15] |
| [064] | A13 | (T4) v/ħ ≤ 5888 | Proved here | (0,0.2] | (H1) | [065]. To the power form of H: reaches | 10-06 [16] |
| [065] | A16 | Algebra of rates C_P ≤ ε/t | Proved here | Six nodes | (H1) | [066][067]. To the power form of H: reaches | 10-06 [17] |
| [066] | A17 | Proposition H1: C ≤ 1.6×10¹⁰ (ring version) | Proved here | Six nodes | (H1) | [068]. To the power form of H: reaches | 10-06 [18] |
| [068] | SEG | Conditions (H1), (H1seg): assembly when the B rows hold in uniform form | Proved here | (0,0.2] | (H1) | [075]. To the power form of H: reaches | 10-05 [02], 10-11 [03], 10-06 §07 |
| [069] | TP | Lemma TP (two projections) | Proved here | Independent of ħ | (H3) | [072][078][081]. To the power form of H: reaches | 10-05 [10], 10-11 [16] |
| [070] | ESP | Efron–Stein for product measures (martingale differences and Jensen) | Proved here | Independent of ħ | (H3) | [071][075][081]. To the power form of H: reaches | 10-11 [17] |
| [071] | BOX | Product inequality for boxes (conditional independence of even boxes) | Proved here | Independent of ħ | (H3) | [072]. To the power form of H: reaches | 10-05 [11], 10-11 [18] |
| [072] | H3 | Proposition H3: C_P ≤ (1+1/n)C_box/(1−c_alt) | Proved here | Independent of ħ | (H3) | [105]. To the power form of H: reaches | 10-05 [14], 10-11 [19] |
| [073] | DEC | Decomposition of the variance and splitting into a product on the fast side | Proved here | Independent of ħ | (H4) | [075]. To the power form of H: reaches | 10-05 [12], 10-11 [20] |
| [074] | KGC | c_kg = C²+π² (algebra of the limit of the closed formula) | Proved here | Independent of ħ | (H4) | [075]. To the power form of H: reaches | 10-05 [13], 10-11 [21] |
| [075] | H4 | Proposition H4: C_box ≤ C_loc + (1+χ)C_kg | Proved here | Independent of ħ | (H4) | [104]. To the power form of H: reaches | 10-05 [15], 10-11 [31] |
| [076] | BV | Lemma BV (convexity for k ≤ 7) | Proved here | Independent of ħ | (H2) | [078][081][082]. To the power form of H: reaches | 10-11 [22] |
| [077] | MR | Lemma MR (reduction to the ends) | Proved here | Independent of ħ | (H2) | [078]. To the power form of H: reaches | 10-11 [23] |
| [078] | TB | Lemma TB (two blocks for 8 ≤ k ≤ 14) | Proved here | Independent of ħ | (H2) | [082]. To the power form of H: reaches | 10-11 [24] |
| [079] | G | The ratio of Proposition G (geometric series) | Proved here | Independent of ħ | (H2) | Premise of no node | 10-11 [25] |
| [080] | RR | Example in which two-point quantities cannot bound the alternating maximal correlation | Proved here | Independent of ħ | (H2) | Premise of no node | 10-11 [26] |
| [081] | BET | Inequality of form (β) (k ≥ 15) | Proved here | Independent of ħ | (H2) | [082]. To the power form of H: reaches | 10-11 [27] |
| [082] | CORE3 | Proposition CORE3: three stages for the constant of the core | Proved here | Three points | (H2) | [103]. To the power form of H: reaches | 10-11 [28] |
| [083] | PHY | The ends of the core of the sector framework are only on the side of the well | Proved here | Independent of ħ | (H2) | Premise of no node | 10-11 [29] |
| [084] | CLOC | The local term vanishes as ħ→0 | Proved here | ħ→0 | (H2) | [103]. To the power form of H: reaches | 10-11 [30] |
| [085] | S1 | (Σ.1) Sum over sectors | Proved here | Independent of ħ | (H2) | [087]. To the power form of H: reaches | 10-09 [10] |
| [086] | S2 | (Σ.2) Gibbs variational inequality | Proved here | Independent of ħ | (H2) | [087]. To the power form of H: reaches | 10-09 [11] |
| [087] | S3 | (Σ.3) Localisation component by component | Proved here | Independent of ħ | (H2) | [092]. To the power form of H: reaches | 10-09 [12] |
| [088] | SK | The scalar form is not uniform in k | Proved here | Independent of ħ | (H2) | Premise of no node | 10-09 [13] |
| [090] | R1 | Localised Bochner | Proved here | Independent of ħ | (H2) | [094]. To the power form of H: does not reach | 10-09 [15] |
| [091] | R2 | Optimisation of the Gibbs tilt | Proved here | Independent of ħ | (H2) | [094]. To the power form of H: does not reach | 10-09 [16] |
| [092] | S5 | (Σ.5) Composition and the closing condition | Proved here | Independent of ħ | (H2) | [093][099]. To the power form of H: reaches | 10-09 [17], 10-07 [11] |
| [093] | AMX | The formula for the needed value A_max | Proved here | Independent of ħ | (H2) | [094]. To the power form of H: does not reach | 10-09 [18] |
| [095] | THR | If the thresholds disagree, ℓ = 0 | Proved here | Independent of ħ | (H2) | Premise of no node | 10-09 [20] |
| [098] | WALL | At the single site at the top, diagonal dominance fails by ¼ | Proved here | Independent of ħ | (H2) | Premise of no node | 10-09 [24], 10-07 W |
| [099] | COREP | A positive lower bound for the gap of the core, uniform in k (sector side) | Proved here | — | (H2) | [103]. To the power form of H: reaches | 10-09 [25], 10-07 [15] |
| [100] | SWB | S_W of the bridge ≤ 1779.6 | Proved here | Window | (H2) | [102]. To the power form of H: does not reach | 10-07 [12] |
| [101] | SWR | S_W of the ring ≤ 122745 | Proved here | Window | (H2) | Premise of no node | 10-07 [13] |
| [103] | T0P | Row (T0′P): Poincaré for the core, uniform in core length and end values | Proved here | — | (H2) | [104]. To the power form of H: reaches | 10-05 [04], 10-07 [16], 10-11 [28][30] |
| [104] | K4 | K₄ does not depend on ħ | Proved here | ħ→0 | (H4) | [105]. To the power form of H: reaches | 10-11 [32] |
| [105] | P45 | Proposition 4.5: C_P ≤ Kξ²S₀/ħ | Proved here | ħ→0 | Conclusion | [110]. To the power form of H: reaches | 10-05 [16], 10-11 [33] |
| [106] | BL | Family of bridges, one-dimensional version: Proposition L (R ≥ 1) | Proved here | Every ħ | Bridge | [110]. To the power form of H: reaches | 10-05 [17], 10-04 §04 |
| [107] | GS | Identity of the ground-state transformation | Proved here | Finite spatial lattice | Bridge | [108]. To the power form of H: does not reach | 10-01 [11] |
| [108] | BB | Family of bridges, multi-dimensional version: Proposition B (C_P ≥ κξ²) | Proved here | Continuous time, T=∞ | Bridge | [109]. To the power form of H: does not reach | 10-01 [12] |
| [109] | LH | The lower half of the power for the multi-dimensional version | Proved here | ξ > 1 | Bridge | Premise of no node | 10-01 [17] |
| [110] | RB | 1 ≤ R ≤ K′/ħ | Proved here | ħ→0 | Conclusion | [111]. To the power form of H: reaches | 10-05 [18] |
| [111] | PH | The power form of H: ln C_P / ln ξ → 2 | Proved here | ħ→0 | Conclusion | The final conclusion | 10-05 [19] |
Counting the rows by grade gives Table 2.
| Grade | Rows | Main content |
|---|---|---|
| Assumption | 30 | The common premise P0, (H2tube), (KG), (X), (MIXalt), (MIXcore), (ΔScore), B1–B5 extending (H1) beyond the nodes, the premises of interval arithmetic, the inputs to the sectors, the remaining single proposition (LSW♭), Proposition P5 (with a table of assumptions) and others |
| Cited | 10 | Mobility of kinks, Bakry–Émery on convex domains, Muckenhoupt, MTP2, Helffer's criterion, Brascamp–Lieb, Bochner, two representations of maximal correlation, the formula for stationary correlations |
| Computer-assisted | 4 | The margin of (H1) (six nodes), the gap of two sites, the chain outside the window, the outer chain of the ring |
| Reading | 19 | How the correlation length grows, maximal correlations and the values of the stages of the core, the constants of route 2, the inner chain, the rarity exponent, the needed value, the coefficient of the reduced model and others |
| Proved here | 48 | The assembly of Proposition H1, Lemma TP, the product over boxes, Proposition H3, Proposition H4, Proposition CORE3, the five stages of the sectors, Proposition 4.5, Proposition L, the algebra to the power form of H and others |
| Total | 111 | Breakdown by condition: (H1) 25, (H2) 57, (H3) 7, (H4) 9, common 1, family of bridges 7, conclusion 4, explanation 1 |
There are many (H2) rows in Table 2 because the row of the core of (H2) is built from two sides (the three stages on the box side and the five stages on the sector side); it does not mean that (H2) is further along than the others. Conversely, there are few (H3) rows because the construction of Proposition H3 is short and the remaining assumption rows are gathered into one, (MIXalt). The number of rows counts where there are proofs and where assumptions remain; it does not measure how many of the four conditions are done (§08).
The dependency graph — joining five graphs into one
We turn the 111 rows of Table 1 into a list of nodes in the same format as 10-05 §07. The numbers of the premises to the right of "⟸" are always smaller than the number of the conclusion on the left. There is just one node, [103] (row (T0′P)), for which either of two ways of support suffices, and there we write "(…) or (…)". The numbers in both brackets are smaller than [103], so the rule works in the same way.
The whole is long, so we first give Figure 1, which extracts only the trunk. The numbers in the trunk are the same as in the whole graph.
[001] ASM P0 common premise (uniqueness, Markov property, extension, limit, regularity) [002][003][005] ASM (H2tube), (KG), (X) [006] ASM (MIX_alt) [007][008] ASM (MIX_core), (ΔS_core) [012]–[016] ASM B1–B5 ((H1) beyond the nodes, beyond the ends, to scraps) [026] ASM (LS_W♭) the remaining single proposition [040][041] CMP margin of (H1), gap of two sites (six nodes, (0,0.2]) [044] RDG ln ξ ≥ s/ħ [066] PRV Proposition H1 (ring version, six nodes) ⟸ [065] (with [040][041] below it) [068] PRV condition (H1), (H1seg) ⟸ [066][012][013][014][015][016] [072] PRV Proposition H3 ⟸ [006][069][071] [075] PRV Proposition H4 ⟸ [068][002][003][005][030][070][073][074] [082] PRV Proposition CORE3 (core on the box side) ⟸ [007][046][047] … [084] PRV the local term vanishes ⟸ [008][044] [099] PRV lower bound of the core (sector side) ⟸ [026][092][019][018] [103] PRV row (T0′P) ⟸ ([082][084]) or ([099][018]) [104] PRV K₄ independent of ħ ⟸ [103][075] [105] PRV Proposition 4.5 ⟸ [030][072][104] [106] PRV family of bridges, Proposition L (one-dim. version) ⟸ [001] [108] Proposition B (multi-dim. version) [110] PRV 1 ≤ R ≤ K′/ħ ⟸ [105][106] [111] PRV power form of H ⟸ [044][110] (side road) [042][043] CMP chain outside the window, outer chain of the ring → [100][101] S_W → [102] RDG A_W of the product form (stops here)
Open the whole graph (111 nodes)
[001] ASM P0 uniqueness of the measure at T=∞, Markov property, extension from local functions, the limit step, regularity ħ: —
[002] ASM TUBE (H2tube) Poincaré for the tube, uniform in tube length ≤ Cξ ħ: —
[003] ASM KG (KG) box gap of the reduced kink gas is of the Glauber type ħ: —
[004] ASM GLA closed formula for the gap of the Glauber box with fixed ends (original source bibliographic only) ħ: —
[005] ASM X (X) cross term ℰ_Y(E[f|Y]) ≤ (1+χ)ℰ(f), χ uniform ħ: —
[006] ASM MXA (MIX_alt) alternating maximal correlation between boxes c_alt < 1 is uniform ħ: —
[007] ASM MXC (MIX_core) upper bound for the alternating maximal correlation in the core c̄ < 1 (k ≥ 15) ħ: —
[008] ASM DSC (ΔS_core) C_P ≤ c ħ^(−p) e^(ΔS/ħ) for core and window ħ: —
[009] ASM A5 continuous version of Holley's comparison (the tail lemma) ħ: six nodes
[010] ASM A10 the Poincaré–Miranda theorem (covering by boxes) ħ: (0,0.2]
[011] ASM A15 (T5) regularity and density of the functions used ħ: —
[012] ASM B1 (T1b) neighbour and end values > 2.5 ħ: —
[013] ASM B2 (T1c) ħ between the nodes (in uniform form) ħ: outside the nodes
[014] ASM B3 (T1c) ħ < 0.005 (in uniform form) ħ: —
[015] ASM B4 (T3d) end values of the two sites > 4 ħ: —
[016] ASM B5 transfer from the ring to scraps (with end values) ħ: —
[017] ASM IA premises of interval arithmetic (IEEE correct rounding, errors of sums, our own exp) ħ: —
[018] ASM LIM (lim), (END_rand), regularity at the seam of the ring ħ: —
[019] ASM SM the small assumptions of route 4 (inputs to the sectors) ħ: —
[020] ASM PROD Proposition LSσ_W (construction of the upper bound for A_W of the product form) ħ: —
[021] ASM LSWin input (LS_W) (the form of LSI for the marginals of site windows) ħ: —
[022] ASM PF (PF_seg) (locality of volume on the bridge) ħ: —
[023] ASM BAR Barta's row κ = 3/1000, b = 493/1000 ħ: independent of ħ
[024] ASM REG the boundary term of Bochner and regularity of eigenfunctions ħ: —
[025] ASM PROX the provisional rows of Proposition P5 (lifting assumption, Spec and others) ħ: —
[026] ASM LSWb (LS_W♭) A_W < A_max(ħ): the remaining single proposition of route 5 ħ: —
[027] ASM K3 the next eigenvalue 3/4 of the fluctuation operator (of Pöschl–Teller type) ħ: independent of ħ
[028] ASM SPEC1 (A1) discreteness of the spectrum, simplicity and positivity of the ground state (finite spatial lattice) ħ: —
[029] ASM KU (A3) κ uniform in β (the graduation of the multi-dimensional version) ħ: —
[030] CIT MOB mobility of a single kink D = ħ/S₀ (at the level of the process) ħ: ħ→0
[031] CIT BE Bakry–Émery on convex domains (Kolesnikov–Milman) ħ: independent of ħ
[032] CIT A3 Muckenhoupt's bracket B ≤ C_P ≤ 4B ħ: independent of ħ
[033] CIT A4 correlation inequality for MTP₂ (monotonicity of e, ħκ ≥ 0) ħ: independent of ħ
[034] CIT A6 Poincaré version of Helffer's criterion (Ledoux Proposition 3.1) ħ: independent of ħ
[035] CIT A12 Brascamp–Lieb (the cross κ_f, (T4)) ħ: independent of ħ
[036] CIT BOC integral form of Bochner's formula (Ledoux Proposition 1.3) ħ: independent of ħ
[037] CIT SV singular-value representation of maximal correlation (Witsenhausen) ħ: —
[038] CIT KR for Gaussians, maximal correlation = linear canonical correlation (Kolmogorov–Rozanov) ħ: —
[039] CIT CORR (A2) formula for correlations of the stationary path measure ħ: T=∞
[040] CMP A1 (T1a) margin ħρ − 2ħκ ≥ 0.067 (neighbour and end in [0,2.5]²) ħ: six nodes
Lean T1_margin_six_nodes (numbers), T1_node_margin (assumption: interval output)
[041] CMP A9 (T3) λ_c ≥ 1.3×10⁻⁴ (ends in [0,4]²) ħ: (0,0.2]
[042] CMP QF q_free ≤ 0.998854904 (the chain outside the window) ⟸ [017] ħ: window
Lean win_qfree_window_le_of_interval_table (assumption: the table of interval-arithmetic output)
[043] CMP QO q_out ≤ 0.998888530 (the outer chain of the ring, pin ≤ 0) ⟸ [017][018] ħ: window
Lean unc_window_lt_one_of_table (assumption: the table of interval-arithmetic output)
[044] RDG XI ln ξ ≥ s/ħ (ξ ∝ ħ^½ e^(S₀/ħ)), the size of D/(Cξ)² ħ: three points, leading term
[045] RDG CAL c_alt = 0.731 / 0.410 / 0.138 (C = 2 / 4 / 8) ħ: model
[046] RDG MC2 two-point maximal correlation of Stage 2 and B₂ (22.1 / 30.5 / 66.4) ħ: three points
[047] RDG CB c̄_(≥15) ≤ 0.535 (measurement of a lower bound) ħ: three points
[048] RDG BIS bistability of the core on the box side, the fibres of the binary of the bump ħ: three points
[049] RDG CTL positive controls for Proposition H3 (pure Gaussian, Ising) ħ: —
[050] RDG KV K ≈ 2.76 / 1.43 (C = 2), 1.78 (C = 4), and c_ff for free ends ħ: model
[051] RDG DSV ΔS⁰_* ≤ 1.4·10⁻² (ratio to 2S₀ ≤ 1.05·10⁻²) ħ: ħ = 0
[052] RDG N2 the constants of route 2 π_*, Λ, C_1D, gap_W, the inner chain of the bridge ħ: three points
[053] RDG QIN the inner chain of the ring q_in ≈ 1.24–1.28 ħ: four points
[054] RDG EDGE the boundary stage q ≈ 1.004–1.045 ħ: four points
[055] RDG ELL ℓ_min = 38.3 / 121.9 / 406.8 ħ: three points
[056] RDG AWV upper bound of A_W 1857 / 2794 / 9106, lower bound 1.71 / 1.74 / 2.59 ħ: three points
[057] RDG ST3 how far strand 3 got (reading 0.54 times, paper upper bound 10³ times) ħ: two points
[058] PRV A2 Lemma K2 (second-order Taylor of the tilt and the Hölder remainder) ħ: independent of ħ
[059] PRV A8 (T2) the marginal of the kept sites is a nearest-neighbour chain ħ: independent of ħ
[060] PRV A14 (T5) decomposition of the variance ⟸ [011] ħ: independent of ħ
[061] PRV MARG the continuum statement of the margin λ ⟸ [040][058][032][033][009] ħ: six nodes
Lean T1_margin_six_nodes, T1_node_margin
[062] PRV A7 gap on the coarse side ≥ λ (Gershgorin on the ring) ⟸ [034][059][061] ħ: six nodes
Lean ring_gershgorin (assumption: κ ≥ 0)
[063] PRV A11 nesting λ_S ≥ 2.3×10⁻⁵ ⟸ [041][010][035] ħ: (0,0.2]
[064] PRV A13 (T4) v/ħ ≤ 5888 ⟸ [041][035] ħ: (0,0.2]
Lean T4_paper_numeric (assumption: λ_c ≥ 1.3×10⁻⁴)
[065] PRV A16 algebra of rates C_P ≤ ε/t ⟸ [060][062][063][064] ħ: six nodes
Lean H1_assembly (assumptions: seven named ones)
[066] PRV A17 Proposition H1: C ≤ 1.6×10¹⁰ (ring version) ⟸ [065] ħ: six nodes
Lean H1_rate_paper_six_nodes (numbers)
[067] RDG A18 C ≤ 658 (numerical input) ⟸ [065] ħ: six nodes
Lean H1_rate_numeric_six_nodes (numbers)
[068] PRV SEG conditions (H1), (H1seg): assembly when the B rows hold in uniform form ⟸ [066][012][013][014][015][016] ħ: (0,0.2]
[069] PRV TP Lemma TP (two projections) ħ: independent of ħ
Lean two_proj_var (assumption: A+B ≤ (1+c)V)
[070] PRV ESP Efron–Stein for product measures (martingale differences and Jensen) ħ: independent of ħ
[071] PRV BOX product inequality for boxes (conditional independence of even boxes) ⟸ [001][070] ħ: independent of ħ
[072] PRV H3 Proposition H3: C_P ≤ (1+1/n)C_box/(1−c_alt) ⟸ [006][069][071] ħ: independent of ħ
Lean box_two_family, box_shift_average
[073] PRV DEC decomposition of the variance and splitting into a product on the fast side ⟸ [001] ħ: independent of ħ
[074] PRV KGC c_kg = C²+π² (algebra of the limit of the closed formula) ħ: independent of ħ
Lean kg_constant (assumption: Cξ ≠ 0)
[075] PRV H4 Proposition H4: C_box ≤ C_loc + (1+χ)C_kg ⟸ [068][002][003][005][030][070][073][074] ħ: independent of ħ
Lean H4_two_scale, H4_gap_form
[076] PRV BV Lemma BV (convexity for k ≤ 7) ⟸ [031] ħ: independent of ħ
Lean lemma_BV
[077] PRV MR Lemma MR (reduction to the ends) ⟸ [001] ħ: independent of ħ
[078] PRV TB Lemma TB (two blocks for 8 ≤ k ≤ 14) ⟸ [069][076][077] ħ: independent of ħ
Lean tb_far, tb_adjacent, tb_range
[079] PRV G the ratio of Proposition G (geometric series) ħ: independent of ħ
Lean gauss_mode0, one_sub_phi
[080] PRV RR example in which two-point quantities cannot bound the alternating maximal correlation ħ: independent of ħ
Lean rareR_pair, rareR_joint
[081] PRV BET inequality of form (β) (k ≥ 15) ⟸ [001][069][070][076] ħ: independent of ħ
Lean core_uniform_L5 (assumption: the measured c̄)
[082] PRV CORE3 Proposition CORE3: three stages for the constant of the core ⟸ [007][046][047][076][078][081] ħ: three points
Lean three_stage (assumption: the upper bound of each stage)
[083] PRV PHY the ends of the core of the sector framework are only on the side of the well ħ: independent of ħ
Lean p5_end_not_negative
[084] PRV CLOC the local term vanishes as ħ→0 ⟸ [008][044] ħ: ħ→0
Lean cloc_term_poly, cloc_term_vanishes
[085] PRV S1 (Σ.1) sum over sectors ħ: independent of ħ
Lean var_split_cells, cell_sum_sup
[086] PRV S2 (Σ.2) Gibbs variational inequality ħ: independent of ħ
Lean gibbs_ln2_cell
[087] PRV S3 (Σ.3) localisation component by component ⟸ [021][085][086] ħ: independent of ħ
Lean comp_sum_le
[088] PRV SK the scalar form is not uniform in k ħ: independent of ħ
Lean scalar_not_uniform (assumption: p > 0)
[089] RDG S4 (Σ.4) ℓ_min does not depend on k ⟸ [022][055] ħ: three points
[090] PRV R1 localised Bochner ⟸ [024][036] ħ: independent of ħ
Lean negw_le_localized, bochner_localized
[091] PRV R2 optimisation of the Gibbs tilt ħ: independent of ħ
Lean tilt_cost_le
[092] PRV S5 (Σ.5) composition and the closing condition ⟸ [023][024][036][087][089] ħ: independent of ħ
Lean comp_close (assumptions: Barta, (Σ.3), Bochner)
[093] PRV AMX the formula for the needed value A_max ⟸ [092] ħ: independent of ħ
[094] RDG AM2 needed value 25.1 / 90.3 / 312.3 ⟸ [055][090][091][093] ħ: three points
Lean judge_i_inside (assumption: the measured lower bound of ℓ)
[095] PRV THR if the thresholds disagree, ℓ = 0 ħ: independent of ħ
[096] ASM P5 Proposition P5 (the lower end of the window, with a table of assumptions) ⟸ [025] ħ: 8 nodes
Lean path5_conditional, p5_assembly
[097] RDG ST1 how far strand 1 got (1.4–5.5 times the needed value) ⟸ [094] ħ: three points
[098] PRV WALL at the single site at the top, diagonal dominance fails by ¼ ħ: independent of ħ
[099] PRV COREP a positive lower bound for the gap of the core, uniform in k (sector side) ⟸ [026][092][019][018] ħ: —
Lean comp_close
[100] PRV SWB S_W of the bridge ≤ 1779.6 ⟸ [042] ħ: window
[101] PRV SWR S_W of the ring ≤ 122745 ⟸ [053][054][043] ħ: window
Lean sw_inner_le (assumptions: q_in ≤ 13/10, q_out ≤ 0.998888530)
[102] RDG AV A_W of the product form ≈ 2.5·10⁶–4.7·10⁷ ⟸ [020][052][100] ħ: three points
[103] PRV T0P row (T0′P): Poincaré for the core, uniform in core length and end values ⟸ ([082][084]) or ([099][018]) ħ: —
[104] PRV K4 K₄ does not depend on ħ ⟸ [103][075] ħ: ħ→0
[105] PRV P45 Proposition 4.5: C_P ≤ Kξ²S₀/ħ ⟸ [030][072][104] ħ: ħ→0
Lean H3_H4_compose (assumptions: (8), (12), D = ħ/S₀, n, ħ, S₀ > 0, c_alt < 1)
[106] PRV BL family of bridges, one-dimensional version: Proposition L (R ≥ 1) ⟸ [001] ħ: every ħ
Lean local_rayleigh_ratio_le_one (skeleton of the finite sum)
[107] PRV GS identity of the ground-state transformation ⟸ [028] ħ: finite spatial lattice
[108] PRV BB family of bridges, multi-dimensional version: Proposition B (C_P ≥ κξ²) ⟸ [028][039][107] ħ: continuous time, T=∞
Lean cont_ratio_closed, one_sided_bridge
[109] PRV LH the lower half of the power for the multi-dimensional version ⟸ [029][108] ħ: ξ > 1
Lean power_lower_half_of_bridge
[110] PRV RB 1 ≤ R ≤ K′/ħ ⟸ [105][106] ħ: ħ→0
[111] PRV PH the power form of H: ln C_P / ln ξ → 2 ⟸ [044][110] ħ: ħ→0
Lean power_H_of_kink_ratio (assumptions: 0 < K, s, δ; 1 ≤ R ≤ K/ħ; s/ħ ≤ ln ξ)
How to check. There are three steps by which readers can check for themselves. (1) Look one by one at the rows of the whole graph that have "⟸", and check that the numbers on the right are all smaller than the number on the left. At [103], look at both brackets. (2) If this rule is kept in every row, the number strictly decreases each time a premise is followed, so you eventually reach a leaf (a row without "⟸") and never return to the original row. That is all there is to "there is no circle". (3) If even one edge is found that does not keep the rule, it is a candidate for a circle of dependence, and the text has to name which step takes the conclusion of which step as a premise. In the graph of this chapter there was no such edge (all edges of the 111 nodes were checked by comparing numbers).
The assumption rows do not contain the quantity of the conclusion. The rule of numbering does not prevent the form in which the conclusion has slipped into the content of an assumption row (the form that puts the conclusion as a premise). So we read the statements of the assumption rows one by one. The quantities of the conclusion are three: the Poincaré constant of the whole measure at , the ratio , and the power . The 30 assumption rows fall into (i) properties of the measure ([001], [011], [018], [024]), (ii) constants of partial measures (scraps, tubes, cores, site windows: [002], [008], [012]–[016], [021], [022], [026]), (iii) quantities of correlation ([006], [007]), (iv) reduced models and comparisons of forms ([003], [004], [005]), (v) premises of computation and citation ([009], [010], [017], [019], [020], [023], [025], [096]), and (vi) the multi-dimensional version and explanatory rows ([027], [028], [029]); none of them contains , or the power. The Poincaré constants contained in the rows of (ii) belong to the partial measures of scraps, tubes, cores and windows, not to the whole measure. This check is done by eye; machine checking does not replace it (10-13 §05).
The family of bridges — Proposition L and Proposition B
[106] Proposition L and [108] Proposition B are the one-dimensional and multi-dimensional versions of a sentence of the same form. Both say "for the path measure, the ceiling of the Rayleigh quotient of test functions local in time is the square of the correlation length", and from this come lower bounds for the relaxation time, (Proposition L) and (Proposition B).
| Version | Statement | Premises | Role in this part |
|---|---|---|---|
| One-dimensional version [106] | Proposition L: for the 0+1-dimensional double well | [001] (continuous time, ; proof in 10-04 §04) | The left inequality of (14). Gives the lower half of the power form of H without conditions |
| Multi-dimensional version [108] | Proposition B: on a finite spatial lattice | [028] assumption on the spectrum, [039] formula for correlations, [107] ground-state transformation (10-01 §06) | [109] the lower half of the power for the multi-dimensional version (with the uniformity of the graduation [029]). Does not enter the road to the conclusion [111] of the first step |
Putting the two side by side, one reads in the same form that the content of Assumption H is only "the upper half". The lower half is given automatically by the bridge (the one-dimensional version needs only the premise [001]; the multi-dimensional version needs [028][039] and the uniformity of the graduation [029]), and what conditions (H1)–(H4) take on is the upper half . For the multi-dimensional version to apply to the four-dimensional Wilson measure, the rows of discrete time, infinite volume and graduation remain ([08][09][10] of the graph of 10-01).
The position of the computer-assisted rows — what is on the road to the conclusion and what is not
For the four "Computer-assisted" rows of Table 1, we look at the road to the conclusion [111].
- [040] the margin, [041] the gap of two sites ((H1)). There is a road [061] the continuum statement of the margin → [062], [063], [064] → [065] the algebra of rates → [066] Proposition H1 → [068] condition (H1) → [075] Proposition H4 → … → [111]. But it is only the road on which they join the assumption rows B1–B5 ([012]–[016]) at [068]; there is no road that reaches the conclusion without passing through [068]. The computer assistance at the six nodes becomes a premise of the conclusion only when combined with the assumption rows extending it beyond the nodes, beyond the ends and to scraps.
- [042] the chain outside the window, [043] the outer chain of the ring ((H2), route 1 and route 6). [042] → [100] of the bridge → [102] of the product form (Reading) stops there, and [043] → [101] of the ring stops there. Neither is on the road to the conclusion. This is because the value of of the product form lies outside the needed value that the remaining single proposition [026] asks for (10-09 §03).
These two rows turn the contraction of the chains into inequalities over the whole window , and they stand as results of computer assistance within the window in their own right (10-08). But in the present construction they are not used as premises of the conclusion. They enter the road when an upper bound for not of the product form satisfies [026] and the ratio of the chain enters that upper bound (10-07 §06). Put the other way round, the number of computer-assisted rows does not show how close one is to the conclusion.
There is no at which all rows are in place
We overlay the range of of each row on one number line (Figure 2). Assumption rows whose range is "—" ([002], [003], [005], [006] and others, most of the 30 assumption rows) are rows not shown at any , so they are not drawn; only the rows that have a range are drawn.
There are three things to read from Figure 2. (a) The computer assistance for the margin of (H1) is at six nodes with , and the smallest node is larger than the upper end of the window (the "gap" between the vertical dotted lines in the figure). (b) Proposition P5 is point values at 8 nodes at the lower end of the window, , and a little beyond the two conditions can no longer hold together in the same window (the reading that they do not hold together at , 10-09 §05). (c) The six nodes of (H1) and the 8 nodes of P5 do not meet, and there is no node of (H1) inside the window. Moreover, the assumption rows whose range is "—" ((H2tube), (KG), (X), (MIXalt) and others) remain assumptions at every . Therefore there is still not a single at which all the rows of the four conditions are in place together.
| Kind | Range | Which rows | Grade |
|---|---|---|---|
| The nodes of (H1) | [040], [061]–[066] | Computer-assisted, Proved here (between the nodes and below , Assumption of [013][014]) | |
| The computer-assisted window | (25 subintervals) | [042], [043], [100], [101] | Computer-assisted, Proved here |
| The range of Proposition P5 | 8 nodes in (no enclosure between the nodes) | [096] | Assumption (a proposition with a table of assumptions) |
| The three points of reading | [044], [046], [047], [052]–[056] and others | Reading |
What is needed to bring them into line. To bring them into line over the same range of , one of the following is needed.
- Extend (H1) to . That is, show row [014] (). The type of computer assistance by subintervals cannot be used, because with a fixed ratio the number of subintervals, , grows without bound as ; a paper argument uniform as is needed ((H1-b) of 10-06 §07).
- Extend P5 to . This corresponds to route 7 (outside the window), a route decided to be outside the scope of this part (10-07 §02). The form of P5 itself also stops at .
Whichever is done, they only come into line over a fixed range. The power form of H is a statement about , so in the end every row has to be stated in a form uniform as , and computer assistance in the window alone cannot reach it. Outside the window, paper asymptotics are needed. The assumption rows whose range is "—" remain at the stage before ranges are brought into line: first being shown at a single .
The rows needed to reach the power form of H — two ways of supporting the row of the core
Following the graph from the conclusion [111] in the direction of the premises picks up all the leaves the conclusion needs. The only fork is the "or" at [103] (row (T0′P)), so there are two required sets of leaves (Table 5). This applies to the graph of the first step the way of thinking that counts the sets that reach the conclusion when the assumption rows are put as "provisionally true" (for the list of walls on the side of the four-dimensional lattice, see 10-02 §06).
| Grade of leaf | Support A: the core on the box side ([082] and [084]) | Support B: the core on the sector side ([099]) |
|---|---|---|
| Assumption | 15 rows: [001], [002], [003], [005], [006], [007], [008], [009], [010], [011], [012]–[016] | 20 rows: [001], [002], [003], [005], [006], [009], [010], [011], [012]–[016], [018], [019], [021], [022], [023], [024], [026] |
| Cited | [030], [031], [032], [033], [034], [035] | [030], [032], [033], [034], [035], [036] |
| Computer-assisted | [040], [041] | [040], [041] |
| Reading | [044], [046], [047] | [044], [055] (and [089], which depends on it) |
What to read from Table 5. (1) The assumption rows common to both ways of support are the common premise [001], the rows inside the box [002][003][005], [006] between boxes, and [009]–[016] extending (H1). These remain whichever road is taken. (2) Support A puts the alternating maximal correlation of the core [007] and the action barrier [008] as assumptions, and needs the readings of Stages 2 and 3, [046][047], to be replaced by upper bounds. Support B puts the remaining single proposition [026] and the inputs to the sectors [019], [021], [022], [024] and Barta's row [023] as assumptions. (3) Both sets still contain "Reading" rows. For the conclusion to become unconditional, every "Assumption" row has to be replaced by a proof, and every "Reading" row by an upper bound (Proved here, Cited or Computer-assisted).
A note on how to read it — a map, not a fraction
The integrated table is a map that shows where in the claim of the first step there are proofs and where assumptions remain. A proportion such as "48 of 111 rows are Proved here" does not show progress. There are two reasons. One is that the rows do not have equal weight (the single row [001] holds everything from the uniqueness of the measure to regularity, while the single row [074] is the algebra of a sum of two terms). The other is that many of the "Proved here" rows are algebra that takes assumption rows as input, and as long as one assumption row remains, the conclusion stays conditional (the same as the note after Table 2 of 10-05).
When reading it as a map, the following order helps. (a) Follow the trunk of Figure 1 from the conclusion [111], (b) look at the required set of leaves in Table 5, and (c) trace the "Assumption" rows in it from the source column of Table 1 to the text of each chapter. What remains and its cost are laid out row by row of this table in 10-15.
This part places Assumption H at the axis of the study, and has built the upper half of the first step by dividing it into four conditions. This map, which puts the whole on one sheet, is also a map within that way of dividing. Other viewpoints are taken up in Part 11.
What this chapter can say
| Can say | Cannot say |
|---|---|
| The integrated table putting the rows of the five chapters of the first step on one sheet (111 rows: Assumption 30, Cited 10, Computer-assisted 4, Reading 19, Proved here 48), and the dependency graph that keeps the rule of numbering on every edge (no circle) | Any of the 30 assumption rows. Hence the conclusion of Proposition 4.5 and the power form of H of the first step |
| That the statements of the assumption rows do not contain the quantities of the conclusion , or the power (a check by reading the statements) | That the assumption rows are compatible with each other, or that none of them is false |
| The position of the four computer-assisted rows: the two rows of (H1) become premises of the conclusion only on the road where they join B1–B5, and the two rows of (H2) are not on the road to the conclusion | Carrying the computer-assisted results outside the window or to |
| That there is no at which all rows are in place together (by comparing ranges), and the two things needed to bring them into line | Either of the two things to bring them into line. Rows in a form uniform as |
| That there are two required sets of leaves for the conclusion (Table 5) | Which of the two ways of support is easier |
Sources and reproduction
| Item | Kind | Source, tool |
|---|---|---|
| The statement, grade and range of each row of Table 1 | This book | 10-05 Table 2, 10-06 Table 2, 10-07 Table 4, 10-09 Table 5, 10-11 Table 6, 10-04 Table 3, 10-01 Table 8. The original sources of the cited theorems are in the source table of each chapter |
| Edges of the dependency graph | This book | The "⟸" of each chapter's dependency graph copied as it is, with identical rows merged (the rules of §01). The "or" at [103] comes from the notes on correspondence in 10-05, 10-07 and 10-11 |
| Checking the rule of numbering, counting the rows, the required set of leaves | Text processing | A small script that, from data copying out the rows and edges of the table, compares the numbers on every edge, counts rows by grade, and collects leaves from the conclusion in the direction of the premises (not a mathematical computation) |
| Lean theorem names and assumptions | Lean | Under each row of the graph. The list of statements and the limits of checking are in 10-13 |
Terms used in this chapter — integrated table, dependency graph, node, leaf, trunk, the rule of numbering, circle of dependence, the form that puts the conclusion as a premise, family of bridges, way of support, required set of leaves, bands of the range of (nodes, window, the range of P5, the three points of reading). Their meanings are in the A-02 glossary.
Next chapter: 10-13 Lean statements and the limits of machine checking — looks, through the list of bundles and examples, at what machine checking guarantees, "the conclusion follows from the propositions as written", and what it does not guarantee (the truth of the assumptions, the encoding of the objects, closing by putting the conclusion into a definition, circles of dependence).
← 10-11 (H3)(H4) and the constant of the coreContents10-13 Lean statements and the limits of machine checking →