Complete note archive
Every maintained scientific note appears once. Priority measures current retrieval importance, not proof quality or novelty. Source notes govern later corrections.
Greppable catalog · Dependency paths · Obstruction map
Newton/action
- PDFA bounded Alpoge–Sussman peek: what returns to Newton in 0+1
A pinned selected-source peek motivates an exact quartic connected-response test: m4-3m2^2=-(b/hbar)(m2 m6-m4^2)<0. The equal-cell cumulant is asymptotic to -3 lambda hbar^3 T^5/(256m^4), while A_hbar fourth derivative divided by w tends to 6 lambda. A full Gaussian exponential-observable reflection test admits the zero-action member.
- PDFTime blocking, Newton polygons and explicit quantum action
For arbitrary unequal time grids, the exact Dirichlet Green row sum gives a contraction factor Lambda T squared over 8, polygon convergence and a uniform inverse-Hessian/source-response bound. Gaussian fluctuation widths retain an explicit hbar factor.
- PDFConstructing Newton motion: refinement, continuation and regularity
Arbitrary positive partitions and mixed kick/drift orders construct global-Lipschitz Newton motion with explicit mesh error. Conservative energy gives local continuation and magnetic global examples; exact logarithmic arrival criterion has threshold beta=2, vanishing annular action and local WKB residual. Unbounded slope is not a full-state merger; no action floor follows.
- PDFCanonical averaging and the Gaussian sector of Newton preparations
Copy-index symplectic mixers and weak or W2 closure admit a Gaussian with each admissible covariance; a positive infimum determines the entire Gaussian sector. The older density ceiling fails a two-copy mixer. A supplied entropy floor supports actual cusp transport and mixing with W2 closure but fails weak closure and, as a subsequent note proves, selective Gaussian-meter closure.
- PDFClassical fluctuation laws and conditional action universality
One nonnegative additive-function theorem controls mass-only independent fluctuation composition, including continuous Brownian free paths and Green-Kubo plateaus. A finite-rate reference supplies positivity; matched-scale ordered streams retain a zero plateau. Additive force-independent Brownian noise gives the sharp pinned-path record floor; symmetric Levy laws obey phi(m,k)=m Gamma(k/m).
- PDFQuantum preparations select continuations at a bounded Newton cusp
Two Gaussian families have identical position densities and the same limiting incoming trajectory, yet converge to reflection or transmission through the C1 cusp; their superpositions yield any mixture of the two outgoing branches.
- PDFRefinement action: cut energy, quantum phase and Gaussian information
One canonical Dirichlet action treatment: orthogonal arbitrary-cut hat energies and mesh exhaustion; exact Gaussian bridge KL/testing and sharp finite-grid invariant mark information; Weyl polygon phase, positive ordering holonomy and partition identity. General force bound retains one-sign attainability. Historical Mohist/Archimedes sources and conditional Opticks fit-count proof distinguish source reading from quantum assumptions. No floor, Weyl law or universal physical hbar is derived from fits.
- PDFA Gaussian meter breaks the classical entropy-floor witness
A single classical Gaussian meter with a supplied minimum-action pointer takes an entropy-floor input to arbitrarily small posterior action on a positive-probability coarse record. A Gaussian-mixture repair preserves the record and copy mixers but fails a nonlinear canonical shear. corrects: central-limit-canonical-gaussian-sector.
- PDFLeibniz's law of continuity, read on records, selects a positive action floor for motions
In the non-adaptive Gaussian mark model with preparation-invariant tests, optimal force discrimination is continuous at zero force iff κ>0; finite schedules realize spent cut action/κ. Historical passages support an explicitly modern record-level reading of continuity.
- PDFLifting a Lipschitz Newton certificate to quantum mechanics
Defines the universal constructive lifting conjecture with fixed certificate schema, noncommutative target, toolkit and joint observable limit; Koopman unitarity alone is insufficient. Proves the conservative global-Lipschitz C1,1 instance using graph estimates and Nelson: fixed-hbar product convergence and sharp mesh-uniform sqrt(hbar) classical recovery. Universal lifting, singular completion and positive-action necessity remain open.
- PDFMarking Newton's comparison: classical widths and quantum probe costs
Classical independent-box protocols obey the 9/36 conditional bounds, while Gaussian invariant tests have sharp constant 48. Supplied quantum probes give the standard-deviation cost hbar/2; correlations and non-Gaussian probes qualify it. Body-independent-noise classification and unread Gaussian channels are integrated. is superseded by: record-distance-path-length.
- PDFRadiation, reservoirs and the action-scale question
Normalized radiation spectrum defines an action unit under explicit scale and integrability assumptions, not universal quantum structure. Cross-field thermal extension remains conjectural. Reversible two-pointer records defeat a prior density cap; exact Rutherford, regulated radiation-response, pumped-depot and thermodynamic-work countertests retain their distinct hypotheses. Lorentz spectral form and any Planck calibration are conditional; work lower bounds are not attainable optima.
- PDFCompeting time-cell branches: a conditional positive-action bound
A double-well time-cell response ceiling gives a uniform positive lower bound on the supplied action multiplier using an exact variance identity. The small-action source transition has a tanh profile. A specified global-minimum zero extension is discontinuous, while classical branch memory and a thermal weight are explicit controls.
- PDFThe Newton cusp: classical histories, conditional floors and records
Bounded C1 cusp potential has full point-state mergers and global classical solutions. Conditional positive covariance floors follow either reversible instantaneous phase evolution plus canonical/weak closure, or actual Gaussian cusp transport plus W2 copying/continuity. Full-trajectory group is a distinct zero-floor classical completion; Gaussian branch limits have nonuniform zero-width continuity. Sharp density-cap witness 1/(4piM), entropy witness and fine joint-record contradiction delimit claims. Quantum dynamics at supplied hbar and quantum identification are separate.
- PDFNewton indeterminacy routes: the physical premise a record floor needs
A conditional classical statistical-speed theorem reproduces the exact sagitta/impulse disturbance bound; Gaussian ensembles with affine generators satisfy its premise with h*=2ζ. Background and Newton inflexion candidates leave record closure and scale matching open.
- PDFNewton's comparison: areas, action defects and controlled reunion
Canonical Galileo/Newton geometry, source paragraph map, matched-endpoint action and arbitrary-partition defect, receding-centre correction and exact controlled F,−F,F reunion. Conditional copy thresholds are kept separate from action quantization.
- PDFA nonlinear Newton time cell: controlled fluctuations and induced stiffness
Convex Euclidean one-vertex integration has normalized tail, variance and curvature bounds; quartic integration generates positive stiffness at supplied hbar while minimization has zero central quadratic curvature. Retains finite constants, one-halving bad-event bound and precise Dimock/Balaban source evidence: noisy block average, generated terms, large fields and earned locality do not follow from a density-tower identity.
- PDFThe cost of a mark: Newton's vanishing sagitta and a floor of order ℏ
Integrated mathematical and historical manuscript: conditional Gaussian and quantum disturbance bounds, exact polygon phases and the source-based Newton comparison. Historical M3 is an interpretation; operator spreads, hard widths and posterior inference are distinguished.
- PDFA fifth postulate for the Principia: joint determinacy of place and motion
Added covariance classifies the Moyal algebraic route and a Gaussian state-restriction route, both retaining an unselected zero branch.
- PDFQuantum record bounds: aperture, disturbance and retained resources
One Bures-angle proof gives supplied-hbar aperture, general-disturbance and recoil-only bounds, with explicit hybrid-state envelopes and distinct preparation quantifiers. Separated packets and modular grid probes retain the resource counterexamples; force-split minimization needs envelopes uniform over splits. corrects: mark-cost-and-statistical-floor.
- PDFRivero's consistency conjecture: quartic paths and central-force angles
Constructive quartic and angular-phase tests retain zero-action sequences despite valid refinement and cycle consistency.
- PDFComposition and action normalization: reciprocal mechanics, rotations and spin phases
Reciprocal spring responses fix compatible inertia ratios through a connected-graph cycle test. Newton derivation compatibility and mechanical rotation closure equate constituent algebra constants, admitting zero. A supplied spin phase imposes 2s/K integrality while common normalization and arbitrarily small local cap actions remain free.
- PDFScore-constrained ensembles: action, records and the controller
Shared-score preparation and canonical copies lead to a restricted Fisher action, explicit positive forward orbit and switching representation. Terminal conjugate records and ordinary transport fail the restriction; branch controllers preserve unread energy while closure selects no kappa.
- PDFClassical recording: complete memories, refinement and nonlinear limits
Canonical classical recording treatment: regulated common-bath readout escape, terminal Gaussian closure, complete-record adaptive information, physical copy/refinement and continuum recoil, nonlinear-copy failures, and local phase/unread-energy tests.
- PDFCoulomb completion and its classical limit: domains, collisions and preparation
Classical Kepler collision flow is incomplete while non-relativistic Coulomb dynamics is global for every h>0. The October 2 written derivation proves (L)=O(h^(3/2)) and position/momentum centroid errors O(sqrt(h)) on fixed collision-free intervals. Proposition 2 gives selection-dependent Dirac and Klein–Gordon h-sets, with explicit endpoint rules.
- PDFCoherence, resolution and the classical zero-branch limit
Coherent finite-partition point records converge iff every nonzero action-frequency sum vanishes; equality to the classical value additionally requires cancellation of equal-action cross terms. Gaussian record laws vary continuously with the supplied action, and incoherent narrowing packets recover the classical swarm for quadratic forces. Includes local visibility, two-ended imprecision, free-fold and radial-angle constructions. The radial-angle model requires signed interval widths: positive Kepler action gradients compress before folding; T²/DeltaT is a dephasing scale, not an unconditional first wrapping time. corrects: score-constrained-ensemble.
- PDFClassical action selection: units, symmetries and orbital thresholds
Dimensional and similarity tests distinguish action units from floors. Sharp excitation and singular-Coulomb bounds retain their premises; the integrated C130 radial-action calculation gives the supplied-quantization Sommerfeld energy correspondence.
- PDFBounded-force records: reachability, minimax recovery and composition
Exact force lenses and clipped-cut areas, a symmetric-fibre minimax theorem, all three finite-horizon phase-risk regimes, independent composition and shared/block budget laws are proved in one information model.
- PDFGalileo's comparison as two-path interference
Endpoint-matched constant-force and impulsive propagators differ by the scalar phase Kτ/ε, yielding an exact independent-copy discrimination law. Refinement erases the signal; classical-first coherence oscillates, while relative-resolution averaging or calibrated attenuation gives specified noncommuting limits.
- PDFTopology, size stabilization and action normalization
Actual two-dimensional degree-one sigma solutions keep energy 4πrho while their radius-crossing action vanishes. A three-dimensional quadratic/quartic trial family fixes radius but exposes the supplied action coefficient b/c and a free common stiffness normalization.
- PDFA sharp mechanical cost for a finite-duration reversal
A return with endpoint velocities ±u and acceleration ceiling a exists iff T≥2u/a and has unique minimum kinetic action mu³/(3a). Chord-action defect is bounded sharply by ma²T|π|²/24.
- PDFOperational spin states, reversible interaction and finite closure
An affine-test orientation ball and its minimal composite have finite operational capacity, but a complete reversible spin interaction fails moment descent and admits no finite bounded-observable repair for all Borel preparations. Source reconstruction premises and the verified seven-dimensional generator restriction are integrated.
- PDFContinuous spin in Galilei mechanics: a transverse boost moment
The zero-mass continuous-spin label is a transverse boost moment, realized by a signed-mass dipole; elementary orbit curves have fixed physical time, and nonzero momentum precludes an energy lower bound. A supplied Poincaré energy gap gives a boost–momentum uncertainty floor proportional to ℏΔ/c², while a positive continuous-spin label still permits energy approaching zero.
- PDFMechanical interference measures phase without fixing an action unit
An explicit ideal string network produces mechanical work fringes whose normalized autocorrelation survives attenuation, while energy and canonical action shrink quadratically. The finite-pulse construction distinguishes canonical action from the traveling wave’s zero Lagrangian action.
- PDFIndependent settings test shared readiness, while leaving action units free
CHSH bounds arbitrary shared-readiness local models under setting independence but cannot select an action normalization.
- PDFSuperdeterminism lives below every resolution; a floor gives it a lifetime
Exponential mixing of a connected Anosov setting device bounds hidden-variable/setting correlations for Lipschitz-resolved conditional preparations, with a logarithmic resolution-dependent onset.
- PDFClassical detector records: thresholds, reliability and coincidence bounds
Fixed-split conditionally independent monotone receivers obey the sharp coincidence-product bound. Passive barriers, exact capped-Arrhenius retention/deadline optimization and shared-release countermodels retain their separate premises, energy accounting and causal timing. None selects a universal physical action.
Yang–Mills/gauge
- PDFFour-dimensional composition: exact Gaussian blocking and one-loop matching
Exact directional Gaussian composition preserves harmonic flux normalization but sharp blocked covariance grows with depth. Internally checked determinant-jet estimates and conditional telescoping give universal average running; §7 supplies formal finite one-step vertices/matching constants.
- PDFFour-dimensional parallel insertions: one-loop shifts and the logarithm
Computes formal one-step four-dimensional anisotropic shifts and conditionally recovers the universal inverse-coupling change −2b₀ log 2 from matched background determinants. Exact generated-action recursion retains every induced interaction.
- PDFGaussian product blocking: the tree-level coupling never moves
Exact Gaussian product blocking multiplies the small-momentum heat-time coefficient by 2^(4−D), preserving it in four dimensions at every finite depth. Centred nearest-plaquette input retains an O(K²) error.
- PDFLow-dimensional gauge gaps: matrix confinement, conditional floors and scales
Scalar and SU(2) bosonic matrix oscillator bounds prove compact resolvent, a simple ground state and a supplied-hbar gap with exact hbar^(4/3)g^(2/3) scaling. Classical area restrictions instead bound sublevels and their volume; the Weyl leading count and semiclassical channel levels remain distinct. Includes field-unit conversion, torus/invariant-sector limits, free/compact/2D flux and corrected singular-domain examples.
- PDFConditional gauge-gap transfer: multiscale control, mixing and certification
H1 multiscale fluctuation/quasi-local Gibbs control and H2 neighborhood mixing imply a volume-uniform Wilson-transfer gap, with continuum transfer conditional on existence and dense observables. Finite certificates, gauge marginal reduction, interaction robustness and numerical bands retain their distinct burdens.
- PDFGauge spectral limits: finite lattices, coupling sets and the continuum target
One canonical lattice-to-continuum spectral treatment contains T1 finite compact-resolvent positivity, strong-coupling and Wilson/KS distinctions, finite-volume analytic coupling dependence, conditional limiting spectral thresholds and lost-weight counterexample. Integrates former position map and exact Wilson sufficient constants. All-coupling positivity/phase equivalences, large-field rarity, relative flow truncation and exhaustive route closures remain unproved; continuum construction and physical spectral transfer stay separate.
- PDFSeries and parallel: where the gauge insertion law stops closing
Directional heat-kernel halving closes in series but leaves an exactly defined coupled mid-plane parallel theory.
- PDFSU(2) on the full mid-plane: the relative-order-t halving defect
Formal full-plane one-loop coupling shifts have explicit signs and SU(N) scaling, with a separate finite-torus winding obstruction.
- PDFThe SU(2) mid-plane on its small-field set: bounds and the missing comparison
Covariant inverse decay, bridge tails and local convexity coexist with the flat-holonomy failure of the original normalized comparison. Exact barriered responses, large-field insertions and weak-recoupling dressed activities give (112)/(116); a centered quadratic moving-mean model gives (177), while nonlinear (113), physical recoupling and iteration stay open.
- PDFThe SU(2) bridge midpoint in closed form: the curvature term is exact
Exact bridge character formulas cover every spin; spin-½ is scalar, while internally checked spin-1 matrix entries retain axial anisotropy and explicit image bounds.
- PDFThe bridge midpoint on a compact group at any cut: windings and the centre
Exact single/multiple-cut character moments classify central image phases by q-torsion; SU(3) trisections see triality while halvings reach only the identity centre element. Fundamental trisection shells are explicit.
- PDFOne-loop torus valleys: local confinement, periodicity and spectral limits
The one-loop SU2 valley has bounded periodic full potential and an unbounded nonperiodic subtracted correction. For the declared flat 4pi holonomy operator, centre-odd and cubic-invariant trials give an explicit g^(8/3) exp(-c/g) upper gap, so local g^(2/3) spacing is not its global gap. corrects: weak-coupling-feshbach-reduction.
- PDFCompact U(1) under refinement: an explicit total-variation bound in three dimensions, and why it fails in four
Exact Villain monopole/flux decomposition gives a D=3 full-measure TV bound 2(L/a)³e^(−π²/(6λ₃a))/(1−e^(−π²/(2λ₃a))) and removes compact defects at fixed coupling and volume.
- PDFThe weak-coupling gap in a small box reduces to three inequalities through the Schur complement
Proves abstract Schur gap-transfer lemmas, including a constant-shift/relative-error version. Physical H1–H3, UV-uniform domains and bounds remain open, and H3 must identify the centre sector and observable algebra before a local matrix spacing can represent its compressed gap.
- PDFAn explicit strong-coupling gap for the Wilson transfer matrix: SU(3) is gapped for g² ≥ 1059, with Δ ≥ (ℏ c/a) 4log[1/(176(e6/g2-1))]
The all-representation activity rho=e^(6/g²)−1 yields a volume-uniform Wilson-transfer gap at the sufficient integer bound g²≥1059, with rate 4 log[1/(176 rho)] in units ℏc/a. Exact sufficient KP convergence uses rho≤21/(500e²); the unrounded rate is positive only at a strict margin.
- PDFBlocking and Schur bounds: the surface-to-gap obstruction
Surface-to-gap criteria scale unfavourably in specified regimes.
- PDFDobrushin's Wilson criterion: an explicit strong-coupling gap at g² > 444 and an open block test
Derives the explicit one-link Wilson sufficient criterion g²>444 for SU3 and its transfer-gap rate. The proposed single-link block-marginal test is empty in the gauge interior; a joint invariant certificate and weak-trajectory control remain additional obligations.
- PDFSpectral upper bounds: smeared susceptibilities and moment hierarchies
One variational and positive-spectral-measure treatment gives intensive susceptibility bounds, conditional moment ratios and exact spatially flowed Maxwell constants. Temporal-flow admissibility and infrared moments remain assumptions. All finite inverse moments can coexist with a zero edge; complete moment data may determine the observed channel, which need not be the global gap.
- PDFGauge flow: exact conjugation, Jacobian locality and spectral truncation
Finite-lattice flow preserves spectra and multiplication norms and has a local first-derivative path bound. Exact continuum variation distinguishes the true Jacobian from an auxiliary Gaussian propagator with an absolute tail budget. Landau growth is gB-k_parallel^2; inverse metrics and relative Hamiltonian truncation remain open.
- PDFGauge vacuum estimates: global tails and conditional slice transfer
Exact magnetic Laplacian/gradient identities and variance sum rule feed finite-volume global Agmon tails with explicit all-path constants. Perron slab and anisotropic temporal limits conditionally identify ground-state slice probabilities; normalized local rarity and operator comparison remain separate.
- PDFLarge gauge fields: action cost, constrained minima and model entropy
Flowed-block continuum action floor eta_F^2/(4g^2) has exact equality accounting and no proved positive-threshold saturation. Bianchi failure defeats the old localized-constant example. Finite-regulator minimum need not have nonnegative tangent-cone Hessian. Charged-background phase-space and exact box counts retain real/complex SU3 multiplicities and norm-dependent cost ratios. Normalized rarity, entropy and polymer convergence remain unproved.
- PDFRare gauge configurations and signed operator comparisons
Exact positive-perturbation min-max bound and negative-well ground-state trial identity distinguish measure from signed spectral control. IMS coefficient 32pi^2 c0^2/3 requires extra link-response, pointwise-field and locality assumptions. Local energy excess and vacuum surface subtraction are unproved targets for a specified construction; no exhaustion of Hamiltonian methods or automatic Euclidean closure.
- PDFVariational lattice-gap bounds: plaquettes, electric trials and holonomies
The KS Feynman-Bijl identity gives plaquette strong-coupling order, an abelian structure-factor gaplessness test and an exact averaged-Polyakov susceptibility bound. Constant-colour electric trials vanish for semisimple gauge algebras; a universal string cost for all field-dependent dressed trials is unproved. An exact SU2 adjoint-loop bound targets the neutral centre sector; the one-patch fundamental variance is not a global vacuum variance.
- PDFA Lieb–Robinson bound for the Kogut–Susskind Hamiltonian, with velocity ∝ Nc/g²
The support-preserving interaction picture reduces commuting unbounded single-link electric terms to bounded plaquette locality, with volume-uniform coefficient of order Nc/g². Numerical prefactors, clustering lengths, physical propagation and stability need their separate hypotheses.
- PDFGaussian gauge blocking: exact covariance, decay and the nonlinear threshold
Exact linearized four-dimensional tube blocking gives the 4/9 constrained gap and Gaussian covariance. A distinct soft constraint has gap 2/9 and a coefficient-specific decay criterion. Correct two-link normalization and infinity-norm shell sum replace the old threshold table; nonlinear KP control remains conditional.
- PDFKogut–Susskind strong coupling: stability, finite-volume bounds and history estimates
Yarotsky stability gives an existential volume-uniform KS gap and a specified translation-invariant perturbed target region. Exact finite-volume electric-loop bounds, corrected all-root overlap obligations and restricted continuous-time counts share one proof structure; numerical uniform thresholds remain withdrawn.
- PDFThree-dimensional Yang–Mills: conditional scaling and the physical gap limit
Conditional physical 3D theory has gap E3 f(lambda3 L), with E3=hbar c lambda3 and lambda3=hbar g_cl². Exact SU2 constant-mode scaling and explicit nu=2 strong-coupling lattice constants control different regimes; nonzero-mode transport, construction and a positive finite spectral limit remain unproved.
- PDFGauge crossover mechanisms: spectral scope, comparison tools and source evidence
One gauge-mechanism comparison keeps curvature, centre deformation, three-dimensional scaling and valley lifting beside correlation inequalities and finite certification. A weak scaling trajectory needs less than all-coupling positivity; temporal operators, rank and physical-hbar limits remain distinct.
apparatus/reconstruction
- PDFA conservative receiver and the origin of a correlation scale
Finite conservative harmonic receivers have zero long-window response; the prepared increasing-chain plateau depends on limit order and closes under its hard speed-support condition. Exact two-body cut/reset and three-body elimination/observability proofs retain the missing classical memory.
- PDFClassical apparatus: construction, complete records and stable recovery
One autonomous finite-mass Hamiltonian apparatus has vanishing-error/disturbance quiet-preparation limits; exact nonlinear calibration and complete pointer/clock records give bounded-domain recovery. Impulsive repeated-cut readout has separate growing-probe resources.
- PDFPreparation, calibration and exact-record fibres of a classical apparatus
A common inverse apparatus chart proves shell saturation, energy/calibration ambiguities, rank-controlled global recovery, matched tolerance/coupling crossover and directional calibration fibres. Signed-coupling symmetry cancels the proposed canonical tangent; finite-width quadratic quadratures retain a conditional curvature test.
historical/sources
- PDFClassical cuts: source evidence and information at an interface
Unifies Aristotle and Plutarch cut evidence with Indian contact, Avicennian, Chinese dissection/statics and cohesion witnesses, preserving editions and reading limits. Separates sampling, re-solving, marginalization and measurement, and retains fixed-time compatibility premises without an action-selection claim.
- Newton on discovery, demonstration and limiting ratios
Passage-level Newton Project audit separates retrospective analytical discovery from synthetic Principia demonstration and documents generated quantities, limiting ratios and priority/publication revisions.
refinement/comparison
- PDFConstructing a 0+1 field theory: the quartic oscillator and the Yang–Mills matrix model
Assembles the known quartic oscillator into a continuous full-time Euclidean process with a unique vacuum, positive gap, bounded-cylinder reflection positivity and a non-Gaussian one-time marginal; ground-state boundary-weighted lattice measures converge for arbitrary time partitions. The construction applies to the prior SU(2) matrix gap and its singlet sector.
- PDFQuantum wall dynamics: boundary choice, reflected packets and impulse
Imposed elastic bounce and quantum boundary choice are distinct. Explicit Dirichlet odd packet has uniform position recovery through impact, current recovery away, and positive boundary-force measure converging to 2|p0| delta. Full Neumann stress has same weak impulse; Robin phases and bound state retain boundary information absent from classical bounce. No self-adjoint half-line momentum is assumed.
- PDFTangent-groupoid scaling and the quantum construction of Newton motion
Exact interacting dilation commutes with kernel composition and normalized bridge marginalization. Matched hbar=epsilon S0 and time/distance epsilon give a local heat expansion with explicit second-order potential terms and a refinement-uniform Gaussian bridge limit. The shifted kernel product retains insertion centres lost at zero. Row-normalized harmonic transitions fail the semigroup law; well-resolving scaling differs. Retains the O(hbar+mesh) coherent-state field theorem, free zero-action control and bridge action defect.
- PDFGauge refinement: exact steps, scale dependence and the infrared obligations
Exact series/parallel operations, arbitrary cuts and group image sectors organized by dimension and scientific dependency. Retains exact circle/rotor identity and one-loop scaling, separates depth/volume uniformities, fine-measure construction and spectral visibility. Corrects unsupported renormalon identification and stable-quartic non-Borel claim. No scale-to-gap or confinement implication is assumed. is superseded by: mass-gap-openings.
- PDFQuantum-to-Newton results: literature and Lean verification targets
Precise classical, operator, packet, sharpness, wall, cusp, relativistic and Euclidean Lean targets with close prior art and a finite rational drift-kick versus kick-drift comparison for newtonlean; exact constant-force overlap exposes joint-limit ray separation and a variable-mass example shows factor-ordering ambiguity.
- PDFFrom multiscale quantum mechanics to Newton's initial-value problem
Normalized supplied-hbar Euclidean blocks and coherent unitary products construct the unique smooth Newton initial-value trajectory with O(hbar+mesh) mean error and O(sqrt(hbar)) widths. Projective Gaussian preparation, raw kinetic divergence and its scale estimator are integrated.
- PDFInserting a point, subdividing a cell: how the limit is built
Exact constant-force elimination and supplied-action Gaussian composition accompany sharper harmonic insertion/mixed-kick bounds and an all-partition trajectory/force-law construction. Exact 2D gauge subdivision and a sufficient summable-defect law require different inputs from a classical initial-value theorem; higher-dimensional interactions and physical limits remain open. corrects: low-dimensional-mass-gap. corrects: three-dimensional-gap-one-function.
- PDFFrom quantum time slices to relativistic and Newtonian motion
Bounded third derivatives give O(h+mesh+c^-2) mean and smooth Weyl convergence to Newton for the positive-energy relativistic particle; fixed h has strong-resolvent convergence, and a separate spectral Dirichlet wall has uniform position convergence through impact.
- PDFWhat survives refinement: the pion, the Yang–Mills gap and Newton's action
Physical comparison retains a pure-SU3 gap, massless/massive two-flavour QCD pion channels and Newton record costs as different targets. Axial Ward/pole identity and two positive spectral-measure limit criteria include surviving weight and counterexample to eigenvalue-only convergence. Coherence, singular-domain selection and physical action necessity remain separate premises; chronological queue and repeated domain tables removed.
- PDFThe zero-spacing limit for any plaquette action and any dimension
Two-dimensional infinitesimal symmetric class-function refinement with finite representation exponents yields exactly central Lévy semigroups; a Lindeberg condition selects the Gaussian Yang–Mills member.
- PDFOne action scale, two rules for composing paths
An exactly unitary normalized checkerboard walk converges strongly on fixed L² wavepackets to Dirac evolution with supplied K; the corresponding real transition rule gives telegraph dynamics. Measuring direction every step yields a ballistic fixed-frequency limit.
- PDFWhen an action plateau controls a spectral gap
Complete observable frames with bounded total susceptibility lower-bound a finite reversible chain’s relaxation gap; one positive velocity plateau only upper-bounds it. Explicit hidden/weakly observed slow modes preserve the plateau while closing the gap.
- PDFA finite-speed return bridge: cuts and midpoint crossover
Exact elastic equal-mass receiver and sharp kappa_mid<=mT(u-|v|)^2 support benchmark precede the velocity-resolved telegraph return bridge. Count/simplex law includes midpoint atom, Beta law, arbitrary-cut action error, exact Bessel crossover and small-mass/window nonuniformity. Scalar convolution rigidity is kept in cut-paradox-two-faces. Speeds, reversal rate, apparatus and limits are supplied.
- Navier–Stokes and Yang–Mills: exact targets and conditional bridges
States the exact Clay data, forcing and quantifiers for fluid A–D and the axiomatic quantum Yang–Mills existence/finite-gap target. Derives scaling and dissipation identities, distinguishes physical from auxiliary clocks and states the obligations for each proposed bridge.
- PDFFinite propagation: scalar rigidity, internal states and record limits
Scalar ballistic-support probability convolution laws are deterministic drift, and scalar translation-invariant unitary groups with light-cone kernels are translations up to phase. Internal-state identities, the matrix conjecture, hidden slow mode and exact additive-readout double limit retain separate scope.
- PDFLocal entangling gates preserve an energy gap uniformly in chain length
A depth-two controlled-Z circuit conjugates independent spins to a local interacting cluster Hamiltonian with unique entangled ground state and exact volume-uniform energy gap J. Removing endpoint terms yields four ground states, with gap J above the ground space.
- PDFIsing relaxation, local parent Hamiltonians and clock normalization
The exact interacting heat-bath gap, its explicit positive three-site square-root Gibbs parent and logarithmic global mixing-time comparison are proved or source-matched together. Refresh-clock and supplied-action normalization remain independent of equilibrium weights.
- PDFHolography in the lowest dimensions: at d=0 it is the wave-function identity, at d=1 it is the Schwarzian
Exploratory dictionary compares Euclidean ground-state marginals and segment factorization with low-dimensional holography, then distinguishes gapless Schwarzian/SYK scales from a confining infrared cap.