Machine-checked substrate

Formalization in Lean 4 / Mathlib

The modular and relative-entropy calculus underlying the regional cost functional χR\chi_R is machine-verified for the free-field coherent-state sector. The development carries no sorry and, as reported by #print axioms, depends only on the standard classical foundations of Lean/Mathlib (propext, Classical.choice, Quot.sound). At present the corpus spans roughly ~515 files and over 5,000 theorems (over 5,700 declarations including definitions) with a verified axiom budget of 0 (every project-specific interface axiom has been discharged to a concrete proof or a typeclass instance; what remains is carried as explicit, clearly-labelled hypotheses, never as Lean axioms).

Scope. The verified, axiom-free corpus now covers both the borrowed mathematics (Tomita–Takesaki modular theory and Araki = CGP relative entropy, free-field coherent sector) and the program’s own results: the covariant σ-additive consistent Born measure on the record net, the Born-from-typicality reduction (to a state-supervenience premise, with a no-go), λ’s covariance/contextuality structure, and the metaselector layer — a machine-checked no-go trilogy (neither capacity, nor symmetry, nor the state Φ selects the record framework) with the positive answer (einselection, Zurek’s commutativity criterion), plus a category-error-proof record/area “contract” resting on Born-from-projectors. A second, self-contained thread formalizes emergent gravity — Jacobson’s “Einstein equation of state” route to the Einstein field equations, with the thermodynamic input grounded in QIQT-H’s own capacity bound, as a conditional axiom-free chain (see below). What it does not establish: the holographic axiom (FQ), λ’s dynamical law, or the continuum (Type III₁); and the gravity thread is conditional on three clearly-labelled physics inputs (it is not “general relativity from nothing”). It does not close the open problems. (The original Macroscopic Definiteness Conjecture is retired as a category error, not a pending verification target.)

The headline result

The coherent-state Araki relative entropy equals the one-particle Casini–Grillo–Pontello entropy, as a literal machine-checked derivative theorem:

ddt0Ω, ΔW(f)ΩΩitΩ=iSCGP(f),\frac{d}{dt}\Big|_{0}\,\big\langle\Omega,\ \Delta_{W(f)\Omega\,\mid\,\Omega}^{\,it}\,\Omega\big\rangle = -\,i\,S_{\mathrm{CGP}}(f),

so that

SAraki(ωW(f)ΩωΩ)=SCGP(f)0.S_{\mathrm{Araki}}\big(\omega_{W(f)\Omega}\,\Vert\,\omega_\Omega\big) = S_{\mathrm{CGP}}(f) \ge 0.

The free-field modular-energy bound (the honest core of “deriving holography”)

A related, self-contained axiom-free development formalizes the modular-energy bound — the derivable content of the JLMS route to the area law. Along this modular route the A/4GA/4G area term is not free-field-derivable (the free scalar has no Newton constant GG, no geometric area operator, a scheme-dependent cutoff coefficient, and the δA/4G=2π ⁣ ⁣δTkk\delta A/4G = 2\pi\!\int\!\delta T_{kk} step needs the Einstein equations) — so here the A/4GA/4G identification stays a gravitational input, not a theorem. (This concerns the JLMS modular route only: the Bekenstein–Hawking 1/4\mathbf{1/4} ratio is derived — as a machine-checked theorem — but through the separate Sakharov / induced-gravity bridge, SakharovRatio.sakharov_ratio (the P4-MICRO story) — a re-derivation of the standard induced-gravity ratio, not unique to finiteness (any local relativistic QFT with the same UV coefficient yields it); what neither derives is the numerical value of GG — though that frontier has since narrowed: the induced-Newton 1/(12π)1/(12\pi) normalization’s π-content is now derived (HeatKernelDDim: the (4πt)d/2(4\pi t)^{-d/2} prefactor and the d=4d{=}4 assembly to 1/(12π)1/(12\pi)), and the a₁ Seeley–DeWitt 2tR2t\cdot R contraction machinery is machine-checked (HeatKernelA1). The flat-space analysis is now exhausted; only the curved-space κ=1/6\kappa=1/6 coefficient stays cited — it needs the covariant heat-kernel expansion Mathlib lacks — so there is still no numerical GG.) What is machine-checked (QIQTH/ModularEnergyBound.lean) is that the entropy variation is controlled by the modular-energy variation, which under one-particle Bisognano–Wichmann Kσ=2πBboostK_\sigma = 2\pi B_{\rm boost} is the Unruh bound ΔS2πΔBboost\Delta S \le 2\pi\,\Delta\langle B_{\rm boost}\rangle:

theoremstatement
modular_relEnt_identityUmegaki: D(ρσ)=(KσρKσσ)(S(ρ)S(σ))D(\rho\Vert\sigma) = (\langle K_\sigma\rangle_\rho-\langle K_\sigma\rangle_\sigma) - (S(\rho)-S(\sigma)), Kσ=logσK_\sigma=-\log\sigma
modular_casini_boundS(ρ)S(σ)KσρKσσS(\rho)-S(\sigma) \le \langle K_\sigma\rangle_\rho-\langle K_\sigma\rangle_\sigma (from Klein positivity)
finiteCorner_wedge_Casini_BWwith Kσ=2πKboost+cK_\sigma=2\pi K_{\rm boost}+c (BW identification, explicit hypothesis): ΔS2πΔKboost\Delta S \le 2\pi\,\Delta\langle K_{\rm boost}\rangle
finiteCorner_firstLawthe first law δS=δKσ\delta S = \delta\langle K_\sigma\rangle at the reference (relative-entropy stationarity)
finiteCorner_firstLaw_boostEnergythe explicit first law δS=2πδKboost\delta S = 2\pi\,\delta\langle K_{\rm boost}\rangle
finiteCorner_wedge_saturation_BWrigidity: ΔS=2πΔKboost    ρ=σ\Delta S = 2\pi\,\Delta\langle K_{\rm boost}\rangle \iff \rho=\sigma (tight only at the reference)
freeField_modularEnergyBound_finiteCorner_BWcapstone: bound \wedge exact deficit 2πΔKboostΔS=D(ρσ)2\pi\Delta\langle K_{\rm boost}\rangle-\Delta S=D(\rho\Vert\sigma) \wedge rigidity

This upgrades the modular pieces of the carried Phase5Master hypothesis from an assumption to derived results. It is formalized modular QFT — not a derivation of the holographic A/4GA/4G bound; the continuum Type III1 ⁣_1\!\toII crossed-product dual-weight trace where A/4GA/4G would live remains a multi-year cited frontier.

Two 2026-07 extensions push further into that frontier. Field-level Bisognano–Wichmann is now unconditional (freeField_secondQuant_BW_unconditional): the second-quantized wedge modular automorphism acts on the whole free-field Weyl algebra as the geometric boost, σt(W(u))=W(boost(2πt)u)\sigma_t(W(u)) = W(\mathrm{boost}(2\pi t)\,u) conjugated — with no carried BW hypothesis — lifting modular-flow == boost from one particle to the full field algebra. And the continuum one-particle map jj_\hbar is now built (Lp/Fock bricks 4–10, axiom-free): the positive-frequency map H1/2 ⁣H1/2 ⁣L2H^{1/2}\!\oplus H^{-1/2}\!\to L^2 with a weighted-L2L^2 isometry (ω\sqrt\omega bounded on the right domain), the canonical symplectic normalization σ=2Im,\sigma = 2\hbar\,\mathrm{Im}\langle\cdot,\cdot\rangle, and boost-covariance of σ\sigma — embedding into the pre-existing continuum Fock tower. That is genuine progress into the Type III1_1 continuum (not its resolution: the A/4GA/4G dual-weight trace stays the cited wall).

Relatedly, InducedNewtonConstant.lean (the granularity reframing) delivers G = 1/(N Λ_s²)G promoted from carried to derived (the relation; the numerical value still needs the species accounting) — and HolographicBridge.lean machine-checks the correspondence that, with this induced G, the AdS/CFT boundary Cardy microstate count of a BTZ horizon equals QIQT-H’s bulk capacity exponent (A/4)N Λ_s² (btz_cardy_eq_qiqth_capacity; the AdS radius cancels). This is a correspondence (the two holographic bookkeepings agree under the shared G), not an import of a boundary CFT, the Cardy formula, or AdS/CFT’s cross-check — QIQT-H’s capacity stays postulated/granularity-reframed.

Emergent gravity: the Einstein equations as a machine-checked equation of state

A second, self-contained axiom-free development formalizes Jacobson’s “Einstein equation of state” route to general relativity — with the thermodynamic input now grounded in QIQT-H rather than assumed. The result is a single conditional theorem:

qiqt_gr_from_wedge_kms — the Einstein field equations aTμν=Gμν+Λgμνa\,T_{\mu\nu} = G_{\mu\nu} + \Lambda\,g_{\mu\nu} (with a genuine Einstein tensor and a constant Λ\Lambda) follow from QIQT-H’s holographic capacity bound SηAS \le \eta A together with Klein positivity S(ρσ)0S(\rho\Vert\sigma)\ge 0, modulo exactly three clearly-labelled, well-motivated physics inputs: the wedge KMS property, matter conservation μTμν=0\nabla^\mu T_{\mu\nu}=0, and standard structural regularity.

What is genuinely derived inside the chain (no hypothesis smuggles in the conclusion):

theoremstatement
qiqt_gr_from_wedge_kmsaT=G+Λga\,T = G + \Lambda g from the QIQT-H capacity bound + Klein, modulo three labelled inputs
differential_area_law_of_relEntropyδS=ηδA\delta S = \eta\,\delta A derived from the bound + saturation + Klein positivity
oneParticleBW_wedgethe wedge modular flow equals the geometric Lorentz boost (one-particle Bisognano–Wichmann)
hasDerivAt_inner_boostUnitary_imaginarythe boost-charge derivative is ii\cdot(boost energy) — boost generator + unitarity
raychaudhuri_focusing_at_equilibriumRaychaudhuri dθ/dλ=Rkk\Rightarrow \mathrm{d}\theta/\mathrm{d}\lambda=-R_{kk} at a stationary horizon
einsteinTensor_divergence_zeroμGμν=0\nabla^\mu G_{\mu\nu}=0 (twice-contracted Bianchi)
jacobson_einstein_equation_of_statethe null-cone tensor relation \Rightarrow Einstein’s equations with constant Λ\Lambda

The instantiated showcase — the floor laid bare

The development since has been drained further: the chain is now machine-checked for an explicit free Klein–Gordon field on a curved pp-wave spacetime, the one-particle Bisognano–Wichmann theorem is now a fully unconditional Lean theorem (no longer a cited input), matter conservation μTμν=0\nabla^\mu T_{\mu\nu}=0 is derived for the KG stress tensor, and the entropy/area derivatives are derived from smoothness of the record law. The capstone of that effort is a single theorem that discharges every geometric and analytic premise and exhibits exactly what GR rests on:

qiqt_gr_ppwave_showcase — the Einstein field equations aTμν=Gμν+Λgμνa\,T_{\mu\nu}=G_{\mu\nu}+\Lambda g_{\mu\nu} for the explicit pp-wave spacetime, with the metric/tetrad, the area derivative (Raychaudhuri area-rate, via an expansion-free congruence), and the entropy bound SηAS\le\eta A (Shannon’s maximum at the holographic capacity) all discharged inside the theorem — leaving as hypotheses exactly the irreducible floor.

what the showcase dischargeshow
pp-wave metric + tetrad (symmetry, inverse, smoothness, frame congruence)the explicit pp-wave geometry
hA — the area derivativearea_hasDerivAt_of_covConst: an expansion-free congruence has zero expansion \Rightarrow constant area
hbound — the entropy bound SηAS\le\eta Ashannon_le_log_card: the area is set to the holographic capacity ηc=logR\eta\,c=\log\lvert R\rvert
what it carries — exactly the floormeaning
hKGthe matter equation of motion (Klein–Gordon on the pp-wave background)
hcap (ηc=logR\eta\,c=\log\lvert R\rvert)the finite-capacity input (P4-MICRO: finiteness is the postulate, from which the area floor SvNQRS_{\rm vN}\le Q_R is a derived theorem; the area form QR=A/4P2Q_R=A/4\ell_P^2 is conditionally derived via the Sakharov bridge, and GG is carried — its relation G=1/(NΛs2)G=1/(N\Lambda_s^2) derived under the granularity reframing, InducedNewtonConstant, only the numerical value carried)
hS, hKthe localization map — the field-coupled record law whose entropy rate equals the stress flux 2π/Tkk2\pi/\hbar\cdot T_{kk}

The localization map is provably not dischargeable by analysis: at the uniform reference the Shannon entropy is stationary (p=0\sum p'=0), so the value of the heat rate is forced to be the stress flux — i.e. the field-coupled record law, the irreducible Gap-2 input. So the showcase is the cleanest honest statement of the result: the Einstein equations for the pp-wave spacetime follow from the matter equation of motion + the holographic capacity (P4) + the localization map — every geometric, curvature, area-kinematic, and entropy-bound step machine-checked and discharged.

Honest scope — a conditional formalization milestone, not “GR from nothing.” This is a rigorous, axiom-free, conditional derivation: the chain rests on labelled inputs kept as explicit hypotheses and never as Lean axioms. For the explicit free Klein–Gordon showcase these reduce to three: the matter equation of motion (Klein–Gordon on the background), the holographic capacity (P4, QR=A/4P2Q_R=A/4\ell_P^2), and the localization map (the field-coupled record law — Gap 2). The wedge-modular-flow==boost story is no longer among them: the one-particle Bisognano–Wichmann is now a fully unconditional Lean theorem, Raychaudhuri focusing is a theorem, and matter conservation μTμν=0\nabla^\mu T_{\mu\nu}=0 is derived for the KG stress tensor — the modular and geometric content has been drained into theorems for the free field. (The algebraic wedge-KMS package — KMS-uniqueness, the strip property, standardness — remains cited rather than formalized only for the general interacting algebra, where a Lean proof would require operator-algebra infrastructure — unbounded Tomita–Takesaki theory, Hardy-strip methods — that Mathlib does not yet have; a substantial separate undertaking, not an impossibility.) What QIQT-H supplies as theorems is the inequality side of the area law; what makes the output general relativity is Jacobson’s argument, here machine-checked end to end. It is a verified formalization result — not a new physical prediction, and it does not by itself establish that our universe’s gravity is emergent.

Prior published work — QIQT-H as its independent machine-verified formalization (2026). Dorau & Much (From Quantum Relative Entropy to the Semiclassical Einstein Equations, Phys. Rev. Lett. 136, 091602 (2026); arXiv:2510.24491, public October 2025) derived the semiclassical Einstein equations from the Araki–Uhlmann relative entropy of coherent states on a local Rindler (bifurcate Killing) horizon — a QFT extension of Jacobson. Their derivation is, step for step, the free-field chain machine-checked here: modular flow == boost (Fock.OneParticleBW); coherent-state relative entropy == horizon energy flux (ModularEnergyBound, the first law ΔS=2πΔBboost\Delta S = 2\pi\,\Delta\langle B_{\rm boost}\rangle); area variation via Raychaudhuri focusing (DifferentialAreaLaw); and the Einstein equations by stress-energy conservation (qiqt_gr_from_wedge_kms / the claim card). Where they assume Srel=δA/4S^{\rm rel}=\delta A/4 to fix the 8π8\pi, QIQT-H additionally re-derives the 1/41/4 (SakharovRatio). Their peer-reviewed Letter — public in October 2025, before QIQT-H’s GR chain was formalized (mid-2026) — establishes this relative-entropy → modular-theory → Jacobson route in a peer-reviewed venue. QIQT-H claims no priority; it independently and subsequently machine-verifies the same chain, with every physical input in an explicit ledger. Both meet the same honest frontier: their closing caveat — higher-order corrections on a curved horizon, “technically demanding, especially regarding the modular data” — is precisely our cited curved-correction / Riemannian-heat-kernel (Seeley–DeWitt) frontier. See the full equation-by-equation mapping (PRL step → Lean theorem).

The quantized graviton and the linearized bridge

Two further axiom-free developments (2026-07) extend the substrate from the scalar field to gravity’s own quantum and assemble the entanglement → linearized-Einstein bridge from machine-checked parts.

The free graviton, end to end

The linearized graviton is now formalized from kinematics through canonical quantization — standard free-field physics, machine-checked (every theorem axiom-free, standard 3):

theoremstatement
tt_decomposition + polarizations_not_gaugethe physical polarization space (TT modulo gauge) is exactly 2-dimensional — the D(D3)/2=2D(D-3)/2=2 count via the explicit gauge quotient
eR_helicity / eL_helicitythe circular polarizations e±=e+±ie×e_\pm = e_+ \pm i e_\times are eigenvectors of rotation with eigenvalue e2iθe^{\mp 2i\theta}helicity ±2 as explicit eigenvalues
kUp_null, physProj_*masslessness k2=0k^2=0 and the physical-state projector (the harmonic-gauge propagator numerator: idempotent, kills gauge and trace, extracts the helicity content)
graviton_null_wavenull profiles f(tz)f(t-z) solve the wave equation t2h=z2h\partial_t^2 h = \partial_z^2 h — the graviton propagates at cc (genuine calculus)
ccrcanonical quantization: [ai,aj]=δij[a_i, a_j^\dagger]=\delta_{ij} for the two helicity modes on the Bargmann–Fock space C[X0,X1]\mathbb{C}[X_0,X_1]
numberOp_pow, hamiltonian_vacuumbosonic occupation spectrum N\mathbb{N}; the Hamiltonian ω(N0+N1+1)\omega(N_0+N_1+1) with zero-point energy $H\lvert 0
angle=\omega\lvert 0
angle$
helicityOp_plus/minus, annih_coherent, twoPointone-graviton states carry helicity ±2; coherent states $a\lvertlpha
angle=lpha\lvertlpha
angle(theclassicalbridge);thetwopointfunction(the classical bridge); the two-point function\langle 0 ert a_i a_j^\dagger ert 0
angle=\delta_{ij}$ (the propagator residue)

The bridge: entanglement first law ⟺ linearized Einstein, assembled from real parts

The FGHMVR/Jacobson template (entanglement first law at every ball ⟺ linearized Einstein) is assembled in nine increments — every derived step a theorem, every physical input an explicit hypothesis (never a Lean axiom):

theoremstatement
graviton_solves_linearized_einstein, einstein_iff_dispersionthe quantized graviton’s polarization content solves linearized vacuum Einstein — and conversely δG=0k2=0\delta G = 0 \Leftrightarrow k^2 = 0: Einstein forces light-cone propagation
bianchi_einsteinSymbolthe linearized Bianchi identity $k^\mu(\delta G)_{\mu
u}=0$, identically
couple_gauge_invariant_iff_conservedgauge invariance of the matter coupling $\int h_{\mu
u}T^{\mu
u}$ stress-energy conservation
soft_gauge_invariant_iff_ward, equivalence_principlelongitudinal decoupling of the soft graviton ⟺ the Weinberg sum rule; for generic momenta all couplings equal — the equivalence principle at the algebraic level
boost_flux_unique, ball_flux_uniquethe wedge and per-ball Clausius data $\delta\langle K
angle = -\delta S$ are forced (given the carried BW/CHM identifications), riding the derived modular flow
chmWeight_edge_slope, cke_*the CHM ball kernel meets the entangling surface with unit slope (the wedge↔ball 2π2\pi consistency) and generates a conformal symmetry (Killing equation by real calculus)
area_probes_separategeometric area probes separate symmetric perturbations — the separating-family hypothesis of the skeleton becomes a theorem
bridge_firstLaw_iff_einstein, bridge_conditionalthe capstone: given the carried Clausius/area law δS=δA/4G\delta S = \delta A/4G, Iyer–Wald, and BW/CHM, the first law at every probe the emergent perturbation satisfies linearized vacuum Einstein

Honest scope. The graviton development is standard free-field QFT (linearized, flat background, no interactions), machine-checked — not a claim of quantum gravity. The bridge is a conditional linearized assembly: the Clausius/area law δS=δA/4G\delta S=\delta A/4G, the Iyer–Wald identity, the Bisognano–Wichmann/CHM identifications, scattering genericity, and the value of GG are carried as explicit hypotheses. Background independence, the nonlinear completion, and the area law from microstate counting remain the cited open frontier — the quantum-gravity problem itself.

The microtheory earns its gravity (E1–E5)

A follow-on campaign of joins between held theorems upgrades the bridge from assembled to earned in-model (all axiom-free, standard 3):

theoremstatement
freeFieldWedgePackage, freeField_clausius_unconditionalBW discharged: the wedge Clausius datum δ⟨K⟩ = −δS forced with no external Bisognano–Wichmann premise (wired from the unconditional one-particle BW theorem; free field)
reconstruct, reconstruct_areaVarthe metric is a function of the code’s own area data — the explicit decoder hii = 2A(ei), hij = A(ei+ej)−A(ei)−A(ej) inverts the emergence map (pointwise, basis-level, symmetric sector)
calibrated_entanglement_cut_area_law, uniform_realizes_area_lawcount = induced area / 4G: with the area induced from the calibrated entanglement cut (no separate area label), log #microstates = screenArea/(4G) under the single named calibration log De = wEnt(e), realized exactly by the maximum-entropy record
rayFamily_firstLaw, code_equilibrium_einsteincode equilibrium ⟹ Einstein: per-ray relative-entropy stationarity forces the first law at every probe, hence linearized vacuum Einstein — Jacobson’s equation of state with the state the code’s equilibrium (explicit K ↦ −K sign adapter)
gravStress_conserved, deser_selfcoupling_consistentthe Deser rung: the graviton’s own radiation stress is conserved on-shell (masslessness ⟹ conservation), so its self-coupling is gauge-consistent — bootstrap order one toward nonlinear GR

Honest scope. Every derived step is a theorem; every physical input is a named carried hypothesis — the calibration log De = wEnt(e) (the physics of the area law), the per-ray BW/analytic data, Iyer–Wald, and G. The full Deser iteration, the continuum Type II trace, background independence, and the value of G remain the open walls — this is the strongest in-model statement of emergent gravity, not quantum gravity.

The wall: the Type II dual-weight trace on the crossed-product core (W1–W4)

The Chandrasekaran–Penington–Witten dual-weight trace — the object whose renormalized entropy underlies the Type II capacity story — constructed on an honest algebraic core with its three defining laws exact (all axiom-free, standard 3):

theoremstatement
dualAction_matter, dualAction_clockthe Takesaki dual action θs on the crossed product: fixes the matter π(a), phases the clock θst) = eistλt — the vector-valued Weyl relation
Iexp_dualShiftthe log-clock density scales exactly: Iexp(f(·+s)) = e−s·Iexp(f) — the τ∘θs = e−sτ mechanism (density on the log-clock variable, the verifier’s binding correction)
zWeight_shift_quasiInvariant, zWeight_dualCircle_invariantthe ℤ-clock regression: the e−1 scaling belongs to the shift; the true dual (circle) action leaves the weight invariant — the distinction machine-checked
tauMonomial_dualthe trace on normal-ordered monomials π(a)λtf(L): τ₀∘θs = e−s·τ₀ exactly, no regularization
eigen_tau_tracetraciality τ₀(xy) = τ₀(yx): the matter KMS factor eκ cancels exactly against the ∫ex change of variables — a KMS state becomes a trace under the log-clock dressing, the Type II mechanism as a theorem
eigen_tau_star_mul_nonnegpositivity τ₀(xx) ≥ 0 — the xx symbol collapses to a pointwise norm-square
phase5_from_core_trace, traceCapacity_from_corethe capacity interfaces instantiated by the constructed trace: the JLMS remainder realized as τ₀(r*r), the bound Sren ≤ Q proven rather than assumed

Honest scope — the wall is not crossed. The trace exists with exact laws on the algebraic core; the matter-side KMS-eigen and positivity inputs are carried (provable for the finite corner); the von Neumann closure is the carried DualWeightTraceExtension typeclass (normal weights/affiliated operators — the genuine remaining frontier, a named hypothesis, never an axiom); the continuum count and black-hole matching remain cited. Not quantum gravity.

Index of machine-checked results

For the exact theorem statements, machine-translated from the Lean source to readable math (notation only, content verbatim), see the machine-rendered statements page.

Toolchain leanprover/lean4:v4.30.0 · verified in QIQTH/AxiomAudit.lean.

Finite Araki relative entropy

theoremstatement
arakiEntropy_eq_relEntropySAraki(ρσ)=trρ(logρlogσ)S_{\mathrm{Araki}}(\rho\Vert\sigma)=\operatorname{tr}\rho(\log\rho-\log\sigma) (Umegaki)

Operator convexity → Lieb’s concavity → DPI → strong subadditivity

A complete, axiom-free, finite-dimensional formalization of the Carlen DPI–Lieb tower — operator-convexity machinery that Mathlib does not have — built bottom-up, every result standard-3. This is an independently-useful contribution to formalized mathematics, and it is what discharged the program’s former entropy-interface axioms (Donald, DPI, ArakiInterface, EntropyBridge) outright.

theoremstatement
peierls_inequalityPeierls (Carlen 2.9): jf(Bjj)trf(B)\sum_j f(B_{jj}) \le \operatorname{tr} f(B), convex ff
trace_function_convexAtrf(A)A \mapsto \operatorname{tr} f(A) convex for convex ff (2.10)
matrix_sqrt_le_sqrtLöwner–Heinz: 0ABAB0\le A\le B \Rightarrow \sqrt A\le\sqrt B
star_inv_subadditiveAndo’s joint convexity of (A,B)BA1B(A,B)\mapsto B^\ast A^{-1}B
gmean_superadditivejoint concavity of the operator geometric mean A#BA\#B
lieb_superadditiveLieb’s concavity theorem(A,B)tr(KA1tKBt)(A,B)\mapsto\operatorname{tr}(K^\ast A^{1-t}K\,B^t) jointly concave
relEntropy_subadditivejoint convexity of quantum relative entropy
dpi_mixed_unitary, partial_trace_dpithe data-processing inequality D(ΦρΦσ)D(ρσ)D(\Phi\rho\Vert\Phi\sigma)\le D(\rho\Vert\sigma)
strong_subadditivitystrong subadditivity S(ρABC)+S(ρB)S(ρAB)+S(ρBC)S(\rho_{ABC})+S(\rho_B)\le S(\rho_{AB})+S(\rho_{BC})
condMutualInfo_nonnegconditional mutual information I(A:CB)0I(A{:}C\mid B)\ge 0

Bounded Tomita–Takesaki (standard subspace)

theoremstatement
modConj_rvdRC_modConjJRJ=2RJRJ=2-R
modConj_rvdT_of_mem_KJ(Tξ)=(2R)ξJ(T\xi)=(2-R)\xi for ξK\xi\in\mathcal{K}
modUnitaryΔit\Delta^{it}: group law, unitarity, strong continuity

One-particle CGP relative entropy

theoremstatement
cgpEntropyS(ξ)= ⁣log((2r)/r)dμξRS(\xi)=-\!\int\log((2-r)/r)\,d\mu^R_\xi
rvdSpec_balancethe CGP spectral balance
cgpEntropy_nonnegS(ξ)0S(\xi)\ge 0 for localized ξK\xi\in\mathcal{K}

Free-field (Fock) modular flow

theoremstatement
secondQuantModFlowHΓ(Δit)\Gamma(\Delta^{it}): one-parameter group, vacuum-fixing, strongly continuous on coherent vectors
secondQuantModFlowH_weylHσt(W(u))=W(Δitu)\sigma_t(W(u))=W(\Delta^{it}u)

Coherent-state relative modular operator and reduction

theoremstatement
relModFlowHΔW(f)ΩΩit=W(f)Γ(Δit)W(f)\Delta^{it}_{W(f)\Omega\mid\Omega}=W(f)\,\Gamma(\Delta^{it})\,W(f)^{*}
connesCocycleH_chain[DωW(f)Ω:DωΩ]t=W(f)W(Δitf)[D\omega_{W(f)\Omega}:D\omega_\Omega]_t=W(f)W(-\Delta^{it}f) + chain rule
hasDerivAt_relModFlow_vacuumSAraki(ωW(f)ΩωΩ)=SCGP(f)S_{\mathrm{Araki}}(\omega_{W(f)\Omega}\Vert\omega_\Omega)=S_{\mathrm{CGP}}(f)

Free-field Born measure & decoherent-histories consistency

A genuine (non-deterministic) Born probability measure on the continuum free field, its Lorentz-covariance, and the decoherent-histories consistency (sum-rule) conditions. Born is the input weight μΦ(α)=CαΦ2\mu_\Phi(\alpha)=\lVert C_\alpha\Phi\rVert^2; these theorems establish that it is a consistent, σ\sigma-additive, covariant probability — not a derivation of Born.

theoremstatement
weylBit_typicalityMeasure_existsa σ\sigma-additive Born probability measure μ\mu_\infty exists (finite-fiber Kolmogorov extension; the finiteness is the capacity bound)
weylBit_typicality_lorentzBoost_invariantμ\mu_\infty is the same in every Lorentz frame (covariant as a law)
weak_decoherence_bitReD(α,β)=0\mathrm{Re}\,D(\alpha,\beta)=0 — weak decoherence / consistency (the Born sum-rule condition), exact
weak_decoherence_contextthe same for every single-bit coarse-graining: the whole projective family is a consistent set
bell_two_bit_strong_decoherencefor orthogonal records u,v=0\langle u,v\rangle=0, full D=0D=0 (incl. the maximally-different Bell pair)
bitOp_vac_expVec_cross_eqexact overlap correction 12ev2/2sinhv,w\tfrac12 e^{-\lVert v\rVert^2/2}\sinh\langle v,w\rangle; vanishes iff v,w=0\langle v,w\rangle=0
strong_decoherence_needs_orthogonalitywitnessed countermodel: overlapping records are not strongly decoherent
offdiagonal_tendsto_zeroSBS / Quantum-Darwinism: redundancy NN\to\infty drives the joint off-diagonal 0\to 0
realm_unique_of_einselectiongiven the einselected pointer family the realm is unique…
capacity_underdetermines_realm…but capacity alone does not pin it (a no-go: distinct capacity-maximal realms)

The metaselector — what fixes the record framework

The choice of abelian record framework {Pα}\{P_\alpha\} resolved as a no-go trilogy (neither capacity, nor symmetry, nor the state Φ\Phi selects it) plus a positive selector (einselection), with a category-error-proof record/area “contract.” Verified scaffold, not new physics: λ\lambda stays inert, so the scheme remains operationally Everett (an ontological reading, with no formal-content claim attached).

theoremstatement
SymmetryNoGo.unitary_invariant_score_constantthe unitary group acts transitively on frameworks (orthonormal bases), so any unitarily-invariant typicality score is constant — symmetry selects no framework
StateAloneNoGo.state_records_triviala single projection P=ΦΦP=\lvert\Phi\rangle\langle\Phi\rvert generates only the trivial framework {0,P,1P,1}\{0,P,1-P,1\} — the state alone selects nothing finer (Bub–Clifton)
MetaselectorSelection.pointer_commutesZurek’s criterion: a record commuting with the monitored AA commutes with the interaction ABA\otimes B — einselected (decoherence-free)
MetaselectorSelection.pointer_invariantan AA-eigenstate stays a product under the ABA\otimes B coupling: pointer states do not decohere
BornProjBridge.bornRecordLawBorn-from-projectors: for a finite orthogonal PVM and normalized Φ\Phi, μ(r)=PrΦ2=Φ,PrΦ\mu(r)=\lVert P_r\Phi\rVert^2=\langle\Phi,P_r\Phi\rangle is a genuine record law
RecordContract.shannon_le_log_cardthe record information bound H(R)logRH(R)\le\log\lvert R\rvert (Jensen) — the entropy/capacity bridges thread the postulated Bousso bound
MetaselectorSelection.finite_budget_forces_overlapa DD-dim record space cannot hold M>DM>D orthonormal records — a finite holographic budget forces a residual-interference floor

Terminology (Gell-Mann–Hartle). Re D = 0 is weak decoherence / consistency (it is what makes the Born weights obey the probability sum rules); full D = 0 is medium, and with orthogonal record states also strong. The Weyl-bit operators A(u,s) = (I + sW(u))/2 are effects, not projectors, so this is a generalized-measurement history; the projector/Boolean-record content is separate. These are exact algebraic consistency results for the free/coherent sector — not a proof of macroscopic classicality.

Born from typicality — the symmetry / state-supervenience reduction

The Born weights reduced from typicality to a single state-supervenience premise (with a no-go that some premise is unavoidable). Born is input, not derived; these establish what it reduces to.

theoremstatement
RedundancyCompressible.card_redundantCodewordsRR redundant copies of a record are distinguishable in X\lvert X\rvert ways, not XR\lvert X\rvert^R — redundancy is compressible (the category-error core)
RedundancyCompressible.naive_overcountsthe naive RlogXR\log\lvert X\rvert strictly exceeds the true logX\log\lvert X\rvert
EnvarianceJustification.envariance_swap_invariantthe system swap, undone by the environment counter-swap, fixes the state iff the swapped amplitudes are equal (Zurek envariance, proved not assumed)
BornEquiprobable.born_from_equiprobabilityfor an equal-amplitude orthonormal fine-graining, the Born weight == the equiprobable branch-count fraction (the amplitude→count bridge)
StateSupervenience.NaturalTypicality.envariance_equiprobnaturality ++ a state-fixing symmetry \Rightarrow equal-amplitude outcomes are equiprobable

λ’s selection schema: covariance & contextuality (OP3b)

theoremstatement
CovariantGluing.no_covariant_selectorno equivariant Φλ\Phi\mapsto\lambda selector when the symmetric state’s histories form a nontrivial orbit (the S² obstruction) — so λ\lambda is a symmetry-breaking sample of the covariant law, not a covariant function
ContextualitySafe.contextuality_safea quantum/record correlation >2>2 (Tsirelson) has no global value-map — assigning values only to the actual context is forced
Fock.bell_no_signaling_stateno-signaling is state-independent: for any (entangled) global state, summing Bob’s record outcome leaves Alice’s marginal independent of Bob’s setting

λ’s selection schema: the finite Takesaki criterion + modular invariance

The finite (Type I) shadow of λ’s kinematic-and-dynamical law. λ is Type-III-native — the records it selects come from a chosen abelian pointer subalgebra 𝔄 (which exists already inside a Type III₁ factor), and the Born weights are the algebraic state value ω(Pα)\omega(P_\alpha), needing no trace. These theorems make precise which 𝔄 is consistent, that the decoherence map is the conditional expectation onto it, and that the selection is stable under the modular dynamics.

theoremstatement
LambdaPointer.modAut_fixes_iff_commuteTakesaki criterion: the modular flow fixes a pointer projection σ(P)=P\sigma(P)=P iff [ρ,P]=0[\rho,P]=0 — i.e. iff the state has no coherence between pointer sectors (exact decoherence selects 𝔄)
LambdaPointer.bornWeights_sumthe algebraic Born weights ω(Pα)=tr(ρPα)\omega(P_\alpha)=\operatorname{tr}(\rho P_\alpha) of a resolution of unity sum to trρ\operatorname{tr}\rho — a genuine probability
LambdaPointer.dephase_preserves_statethe decoherence map E(x)=αPαxPαE(x)=\sum_\alpha P_\alpha x P_\alpha is the unital, ω\omega-preserving conditional expectation onto 𝔄 (exactly when the criterion holds)
LambdaPointer.dephase_sigmaDiag_commutemodular-invariance, t\forall t: EE commutes with the real-time modular flow σt(x)=ρitxρit\sigma_t(x)=\rho^{it}x\rho^{-it} — a consistency fact (the modular flow is not physical time, so this is not physical no-recoherence)
LambdaPointer.dephase_sigmaDiag_commute_diagonalin the einselected (density-eigenbasis) pointer basis the modular-invariance is unconditional for all tt
LambdaPointer.modAut_fixes_pointer / bornWeight_modAut_invarianteach selected record is a fixed point of the flow, and the Born weights are constants of the modular motion
SelectionEvent.selects_exists_uniquethe selection event: an inverse-CDF selector from an actuality seed s[0,1)s\in[0,1) picks exactly one record per seed (totality + uniqueness — single-world consistency)
SelectionEvent.volume_selectsthe uniform seed measure of record kk equals its Born weight pkp_k — the single-shot seed measure of record kk = its Born weight pkp_k (the seed is λ; an across-run frequency needs the separate LLN; the selector is order-dependent, not equivariant, as the no-covariant-selector result requires)

λ’s selection schema in the continuum (free-field / standard-subspace sector)

The finite schema above, lifted onto the genuine continuum modular flow Δit\Delta^{it} (the Rieffel–Van Daele bounded modUnitary of a standard subspace) — axiom-free. The local algebra’s Type III₁-ness (Buchholz–Wichmann) is cited; the residual walls are the Haagerup natural-cone existence in Mathlib and the interacting case.

theoremstatement
ContinuumLambda.modAutOp_add / _mul / _starthe modular automorphism σt=Ad(Δit)\sigma_t=\mathrm{Ad}(\Delta^{it}) is a one-parameter group of unital \star-automorphisms
ContinuumLambda.modAutOp_fixes_iff_commutecontinuum Takesaki criterion: σt(A)=AA\sigma_t(A)=A \Leftrightarrow A commutes with Δit\Delta^{it}
ContinuumLambda.dephaseOp_specProj_commutecontinuum modular-invariance: the decoherence map commutes with σt\sigma_t for every tt (unconditional for spectral pointer projections) — a consistency fact, not physical persistence (modular flow ≠ physical time)
NaturalConeBorn.bornWeights_sumthe Type-independent algebraic Born rule: the scalar spectral measure of a finite pointer partition sums to ξ2\lVert\xi\rVert^2 (a genuine probability, no trace)
ContinuumSelection.continuum_selects_exists_uniquethe Type-blind selection event: exactly one record per actuality seed, driven by the continuum Born weights
ContinuumSelection.continuum_volume_selectsthe uniform seed measure of record kk equals its continuum Born weight — the single-shot seed measure = its continuum Born weight (across-run frequency needs the separate LLN)

And the whole schema lifted to the second-quantized free field: Γ(Δit)\Gamma(\Delta^{it}) as a unitary one-parameter group of bounded operators on the Fock Hilbert space, with the field-level automorphism, modular-invariance, Born rule (on the genuine Fock vacuum state) and selection event.

theoremstatement
secondQuantModCLM_unitaryΓ(Δit)\Gamma(\Delta^{it}) is unitary on the Fock Hilbert space (Γ=Γ(t)\Gamma^\star=\Gamma(-t)) — the free-field modular unitary group
dephaseFock_modAutFock_commutefield-level modular-invariance: the decoherence map commutes with σt=Ad(Γ(Δit))\sigma_t=\mathrm{Ad}(\Gamma(\Delta^{it})) for every tt (a consistency fact, not physical persistence)
vacuumState_povm_sum / vacuumState_weylBit_sumfield-level Born rule: vacuum-state weights of a POVM are a probability; the Weyl-bit record gives (1±eu2/2)/2(1\pm e^{-\lVert u\rVert^2/2})/2
field_selects_exists_unique / field_volume_selectsthe free-field selection event: exactly one Weyl-bit record per actuality seed, single-shot seed-measure = the Fock-vacuum-state Born weight

What these add (and don’t). They pin down λ’s selection schema, not a law: Born reduces to state-supervenience (not capacity, not a counting rule); the covariance + contextuality structure is verified (covariant measure, no covariant point-selector; no global value-map; state-independent no-signaling — operationally weaker than Bell local causality); the Takesaki criterion fixes which record context is consistent; and the dephasing map is modular-invariant. That last is a consistency fact, not physical persistence — the modular flow is not the physical Hamiltonian evolution. The inverse-CDF selection is a sampling representation (single-shot seed-measure = Born weight), not a mechanism or an across-run frequency. So the single outcome is λ’s by stipulation; the holographic bound is the finite record stage only; and the scheme is operationally equivalent to standard QM. The honest residual: the seed’s origin (a primitive), an across-run frequency theorem, a global decoherent-history selector, and the continuum walls (Haagerup natural-cone existence; interacting case).

The joins — hypothesis deletion (J1–J4)

A dedicated campaign shrinking the carried inputs of the landed results by connecting held theorems. The ledger, entry by entry (each says which named hypothesis became a theorem or shrank):

The Lorentz stress-test gates (CPSUV → diamond tip → state level)

Three falsification gates on the finite-capacity postulate itself — numerics validated against closed forms, the decisive constants and limits machine-checked (QIQTH/QG/CpsuvGate.lean, LatticeDispersionBound.lean, DiamondTipGate.lean, StateLevelLVGate.lean; scripts lorentz_stress_test.py, diamond_tip_test.py; results docs under docs/qg_roadmap/).

The arc’s verdict, honestly. Every regulator reading of QR = A/4ℓP² is dead — pixels pick a frame, diamond clocks leak, and averaging over the noncompact boost family is not a regulator. The entropy reading is provably frame-free and is exactly what the Lean core already formalizes (capacity = entropy, not a count). The dynamical-realization gap — what physical mechanism enforces the bound — is now also the sole remaining Lorentz door: LV re-enters iff the enforcer is non-equivariant. Consistent with the covariant-entropy-bound literature (Bousso, Casini, QNEC). The loop integrals are numerically validated (closed forms to ≤0.16%), not formalized; NOT quantum gravity.

The operator emergence map — “graviton = quantized area fluctuation,” theorem-shaped (Q1–Q5)

The classical area→metric decoder promoted to an operator map on the polynomial Bargmann–Fock carrier (Module.End of ℂ[X₀,X₁]; the completion is never used as an operator domain). Two honesty rules are machine-enforced by design: equal-time quantized areas commute (the naive noncommutativity claim was cut at consult time), and the finite code can never carry exact CCR (the trace obstruction) — the code join is expectation-level, permanently.

Honest scope. The carried residue is three named inputs: hJoin (the emergence-map identification, stated once), the calibration log De = wEnt(e), and the Bargmann-adjointness grounding of the coherent v-rule. The code Hilbert space is not Fock and never will be (the CCR-isometry obstruction is a theorem-level fact); fixed momentum, two polarizations, linearized, free. NOT quantum gravity — the genuine microstate count (deriving the calibration via the Type II trace) and the von Neumann closure remain the frontier.

The grounding campaign — carried hinges deleted at once (G1–G5)

Two files, four increments; every deletion names its residue.

The honest ledger after this campaign. Of the named carried inputs across the landed results, the following remain: hJoin + the calibration (the emergence-map identifications — deletable only by the genuine count via the vN closure), the massless wedge BW, the nonlinear Einstein coefficients, symbol-level Iyer–Wald (hDeficit), and the geometric carrier-conjugacy data. Everything else that was carried at the start of the joins/grounding arc is now a theorem. NOT quantum gravity; the von Neumann closure and the count remain the frontier. (Two later campaigns moved this ledger: the keystone delivered the count in the finite branch — the calibration is a theorem there for trace-defined weights — and the join instance below then deleted hJoin itself by construction, merging the code and graviton towers at the finite level; the vN closure and the continuum limit remain the named walls.)

The keystone — THE COUNT (K0–K6): the holographic count as a theorem in the finite branch

The campaign derives, rather than posits, that a diamond/screen algebra’s entropy against the constructed crossed-product trace τ₀ equals induced area/4G — deleting, in the finite branch, the Clausius input, the geometric input, the calibration log De = wEnt(e), and the emergence join at once (QIQTH/Keystone.lean, KeystoneOperator.lean; axiom-free, std-3).

The K6 checkpoint — the two honest sentences. HAVE: “every finite code screen realized as a finite record corner of the constructed crossed-product core has Sτ₀ = log dimτ₀(𝒟C) = Σe log dimτ₀(Pe) = Aτ(C)/4G; in the code instance dimτ₀(Pe) = De, so the calibration is a theorem (trace-defined weight) and the count-built area operator gives the join by construction — no hClausius/hGeom/hCalib/hJoin carried in this branch.” HAVE NOT (Walls 1–5, named): continuum QFT diamond algebras ARE these corners; external geometric area = count-built area; Type III₁/II continuum structure in Lean; σ-weak/normal weights; the value of G. NOT quantum gravity solved; no wall crossed.

The join instance — hJoin deleted by construction (JI1–JI7): the two towers merged

The screen-code tower (the keystone count) and the graviton tower (Q1–Q5) joined into ONE object at the finite level: the dictionary instance — links = screen elements, code weights defined FROM the geometry — makes the Q5 carried hypothesis hJoin a theorem (QIQTH/JoinInstance.lean; axiom-free, std-3). Two-level construction per the consult verdict: generic-exact with REAL trace-dimensions; integer codes only under a named realizability datum.

The JI7 checkpoint — the two honest sentences. HAVE: “after JI1–JI6, hJoin is no longer a hypothesis for the constructed τ join or for nat-realizable finite-code joins, and the count normalization rewrites to (AJ/4)·N·Λs² with local capacity corollaries.” HAVE NOT: “no theorem says arbitrary external real geometry has exact natural link dimensions, no asymptotic approximation is included, and no canonical A₀ split is asserted beyond the named apportionment data/policy.” The CCR-isometry obstruction is permanent (the join is expectation-level forever); NOT quantum gravity solved; no wall crossed.

The embedding — the truncated field diamond IS a counted record corner (EM1–EM7): the finite-level bridge closed

The matter-side dictionary. The key observation is definitional: the keystone’s microstate space Micro = Π_k Fin(D_k) IS a multi-mode truncated Fock basis (joint occupation numbers nk < Dk) — no new Hilbert space is built; the campaign gives the already-counted diamond algebra its FIELD structure and the mode↔link semantics (QIQTH/Embedding.lean; axiom-free, std-3). With THE COUNT, THE JOIN INSTANCE, and THE EMBEDDING complete, the finite-level bridge is closed end to end: a truncated free field in a diamond IS a counted record corner, its records ARE occupation pointer states, its count IS the area over 4G, and that same number IS the graviton’s coherent area expectation — one object, one theorem chain.

The EM7 checkpoint — the two honest sentences. HAVE: “the N-mode truncated free-field diamond algebra IS a counted record corner — the occupation basis is Micro, the per-mode truncated oscillators embed with their honest defect ([a,a†] = 1 − D·Ptop), records are occupation projectors, the count S = Σ log Dk = A/4G reads as the truncated field diamond’s entropy, capacity bounds/saturates the cutoffs as a constraint, and the mode dictionary composes with the join instance end-to-end (field → corner → count → area → graviton expectation).” HAVE NOT: “no exact finite CCR (the truncation defect is permanent); no Type III₁ finite corner (the cutoff→continuum limit is THE wall, never claimed); no construction of continuum-localized modes from the standard subspace (mode membership is named finite data, at most CERTIFIED by a supplied localization witness); capacity is a constraint, not a generator.” NOT quantum gravity solved; no wall crossed.

The dynamics — the code’s time evolution, the independent cross-check, and the conjecture (DY1–DY7)

The microscopic side gets what a definition of a theory requires — a time evolution — and the campaign closes with the QIQT-H analogue of the Brown–Henneaux = Cardy check in its honest finite form, plus the sharp continuum conjecture stated (never assumed) in Lean (QIQTH/Dynamics.lean, CrossCheck.lean, Conjectures.lean; axiom-free, std-3).

The DY7 checkpoint — the two honest sentences. HAVE: “a finite, axiom-free diagonal code dynamics, explicit Gibbs/KMS states, product-mode reductions, and a saturated conditional induced-gravity cross-check whose proof does not use the trace/wEnt area calibration.” HAVE NOT: “a finite proof of a continuum one-loop heat-kernel area law or an equality between finite thermal entropy at arbitrary β and an induced geometric area; that remains the named continuum frontier/conjecture.” NOT quantum gravity solved; no wall crossed.

The decoupling shadow — the finite forced core of the dictionary (DS1–DS7)

Prompted by a primary-source re-reading of Maldacena (hep-th/9711200), whose deepest structural feature is that the dual sides are two SURVIVING DESCRIPTIONS of one parent construction under one limit: this campaign delivers the honest finite shadow of that structure — the word “constructed” is deleted from every part of QIQT-H’s dictionary where deleting it is mathematically true, and what remains is named parent data (QIQTH/Decoupling/, QIQTH/Rigidity/; axiom-free, std-3).

The DS7 checkpoint — the two honest sentences. HAVE: “The capacity-limit theorem forces the oscillator/free-field sector only in the bounded-occupation or positive-temperature sense; it does not force the screen geometry or Newton constant.” HAVE NOT: “The tower-rigidity theorem forces the logarithmic capacity weight only under monoidal, monotone refinement naturality; without those hypotheses there are explicit finite counterexamples.” NOT a full decoupling derivation — the join incidence geometry, the species/cell match, and the value of G remain parent data; NOT quantum gravity solved; no wall crossed.

The tower (T1–T8): the first machine-checked contact with the Type III₁ wall

Phase A of the continuum-definition attack, via the ITPFI/Araki–Woods route: the capacity code tower with its Gibbs product states IS Araki–Woods input data, and its arithmetic invariant is machine-verified to be the III₁ one — at the level of the wall’s fingerprint, never the wall itself (QIQTH/Tower/; axiom-free, std-3).

The T8 checkpoint — the two honest sentences. HAVE: “the machine-checked arithmetic content of the Araki–Woods III₁ criterion for the code’s Gibbs tower, including a hypothesis-free concrete instance, the Powers-guard separation, the σ-additive infinite-mode Gibbs measure with its non-atomicity, and the state-compatible modular-equivariant finite refinement tower; the inference to an actual III₁ factor is cited (Araki–Woods 1968; Connes 1973), never proved.” HAVE NOT: “the ITPFI von Neumann algebra, its ratio set, its type, any inductive limit or weak closure, any quantum state on the infinite system, or any continuum-limit completion — none are constructed or classified here.” NOT the continuum done; no wall crossed — this is the wall’s fingerprint.

The closure (C1–C11): the von Neumann double-commutant theorem

The convergent blocker of the continuum program — the missing lemma that four separately-named frontiers all reduce to — is now a machine-checked theorem, in Mathlib-styleable form: Mathlib defines VonNeumannAlgebra by the bicommutant property but has no bicommutant theorem; this campaign closes that gap (QIQTH/VonNeumann/; axiom-free, std-3; all eleven increments landed, the stretch included).

The C11 checkpoint — the two honest sentences. HAVE: “We have the von Neumann double-commutant theorem as an axiom-free Lean theorem over current Mathlib — for every unital ⋆-subalgebra A of the bounded operators on a complex Hilbert space, the double centralizer A″ equals the set of operators approximable from A in norm on every finite tuple of vectors (and, in the shipped WOT increment, the weak-operator closure) — packaged as VonNeumannAlgebra.generatedBy with membership lemmas, and instantiated to present the project’s crossed-product representation and any commonly-represented refinement tower as genuine VonNeumannAlgebras.” HAVE NOT: “We do not have Kaplansky density, normal states, preduals or the σ-weak topology, type classification, or the inductive-limit (tower-GNS) Hilbert space — the ITPFI tower’s limit algebra is packaged only relative to a hypothesized common representation, and the crossed-product dual-weight trace is not claimed to extend from the algebraic core to the weak closure.” The gate to the continuum, not the wall crossed.

The representation (R1–R9): the tower’s limit von Neumann algebra exists

The GNS construction of the compatible Gibbs family: the corner tower — previously a family of finite matrix algebras related by embeddings — now acts on ONE Hilbert space, and its directed-union limit von Neumann algebra is an actual, named, axiom-free object (QIQTH/TowerGNS/; the first genuinely infinite-dimensional quantum object of the development).

The R9 checkpoint — the two honest sentences. HAVE: “One Hilbert space — the completion of the semidefinite Gibbs-GNS pre-space on the direct sum of all finite corners — carrying compatible unital ⋆-representations of every corner algebra (π_{C′} ∘ cornerEmbed = π_C for all C ⊆ C′), a unit cyclic vector Ω implementing every corner Gibbs state as a vector state (⟪Ω, π_C(a)Ω⟫ = φ_C(a)), and the directed-union limit von Neumann algebra towerLimitVN = limitVN of the representation images, with membership characterized by SOT-approximation from the finite stages — all axiom-free.” HAVE NOT: “The type of towerLimitVN is not classified — no factor, no ITPFI identification, no III₁ claim is made or proved (the T3 fingerprint stays arithmetic; Araki–Woods 1968 and Connes 1973 stay cited, never invoked); Ω is not shown separating, the modular theory of the limit state on the completion is not constructed, and the representations are not shown isometric.” The continuum is not done — but for the first time it has an inhabitant.

The transport + the accounting: dynamics for the limit algebra; the species form forced

Two tracks, one campaign (all axiom-free, std-3, budget 0).

The generator: the self-adjoint Hamiltonian of the limit dynamics, computed

towerGen := stoneGen (towerFlow) — the transported flow’s genuine self-adjoint unbounded generator (K = K†), instantiating the held Stone theorem with the five flow facts (two adapter lemmas; every increment green on first or second build). With it:

Honest scope (the checkpoint, verbatim). “towerGen is NOT constructed from, and NOT claimed equal to, a Tomita modular Hamiltonian log Δ of the limit state — no Δ, J, S, separating property, KMS-at-the-limit, or von Neumann type is claimed. No spectral resolution (PVM) of the unbounded towerGen is claimed, and no exponential-recovery identity towerFlow t = exp(it·towerGen) is claimed — the recovery wall is open by design and the campaign does not cross it.”

The separation: Ω is cyclic AND separating — the standard form

The limit algebra reaches the standard-form hypothesis pair of Tomita–Takesaki theory, axiom-free (RightMul.lean, Separation.lean):

Honest scope (checkpoint, verbatim). “No Tomita operator S₀, no modular operator Δ, no conjugation J, no KMS condition at the limit, and no type classification is constructed or claimed here — separation is the HYPOTHESIS for that theory, not the theory.”

The Tomita operator: S₀, computed and closable

Modular theory proper begins: towerTomita₀ — the Tomita operator of the tower limit state on its classical orbit domain, as a genuine conjugate-linear (σ-semilinear) partial operator:

Honest scope (checkpoint, verbatim). “The closure S̄ is not constructed as an object, and no polar decomposition, no modular operator Δ, no modular conjugation J, no KMS condition of the limit state, and no von Neumann type classification is constructed or claimed; Mathlib’s LinearPMap closure and adjoint theories cover only ℂ-linear (identity ring-hom) partial maps, and a conjugate-linear closure theory is not built here.”

The conjugate closure: S̄ as an object — and a new slice of Mathlib

The closure of the Tomita operator exists, built by the ℝ-reduction (a conjugate-linear map IS ℝ-linear; Mathlib’s closure theory applies verbatim through the global complexToReal instances — no local instances anywhere):

Honest scope (checkpoint, verbatim). “The modular operator Δ, the conjugation J, and the polar decomposition are not constructed (the documented Δ contract … is the named next campaign); no σ-semilinear graph or closure theory is contributed to Mathlib here (the ℝ-reduction sidesteps it; the σ-graph remains Mathlib’s own open TODO); no KMS condition of the limit state and no von Neumann type is claimed.”

The modular operator: Δ, computed as the modular automorphism

The campaign after the conjugate closure delivers Tomita–Takesaki’s central object for the tower limit state:

Honest scope (checkpoint, verbatim). “Full self-adjointness Δ† = Δ is not proved — it is von Neumann’s S̄*S̄ theorem, absent from Mathlib and named as the next target; no polar decomposition, no J, no Δ^{1/2} or Δ^{it} (no unbounded positive square-root or spectral theory for partial operators exists in the pin), no KMS condition of the limit state, and no von Neumann type is constructed or claimed.”

The von Neumann campaign: Δ† = Δ — and von Neumann’s theorem itself

One campaign later, the modular operator is genuinely self-adjoint (six increments in a single session, four consecutive first-try greens):

Honest scope (checkpoint, verbatim). “Δ^{1/2} and the polar decomposition S̄ = JΔ^{1/2} are not constructed (so J is still not an object); the spectral resolution of the unbounded Δ is not built; Δ^{it} and the KMS property of the limit state are not proved — in particular NO claim that the transported dynamics equals the modular flow of Δ; no Tomita theorem at the algebra level; no von Neumann type statement.”

The resolvent campaign: Δ^{it} exists

The modular unitary group of the tower limit state is constructed (seven increments, every one first-try green):

Honest scope (checkpoint, verbatim). “No claim that towerModUnitary equals the transported towerFlow (equivalently towerGen = log Δ): two strongly continuous unitary groups now coexist on the tower space and their identification — the exponential-recovery wall — is the named next campaign, not crossed here. No KMS condition of the limit state is proved; Tomita’s theorem is not proved — U_t is not shown to implement automorphisms of the limit algebra; Δ^{1/2}, J, and the polar decomposition are still not constructed; no von Neumann type statement.”

The identification: the exponential-recovery wall, crossed — and Tomita I

The campaign after the resolvent identifies the two unitary groups (five increments, every one first-try green):

Honest scope (checkpoint, verbatim). “J and the polar decomposition S̄ = JΔ^{1/2} are still not constructed (so JMJ = M′, the second half of Tomita’s theorem, stays open — the natural next campaign: J on matrix units is also explicit, so the same eigenbasis method applies); no analytic strip-KMS of the limit state (only the boundary identity); no von Neumann type classification; and everything remains the finite-stage Gibbs inductive-limit state — the free-field/Type-III continuum objects are untouched.”

Reproduce the verification

~/.elan/bin/lake build QIQTH
~/.elan/bin/lake build QIQTH.AxiomAudit   # emits #print axioms for every theorem

Each theorem reports depends on axioms: [propext, Classical.choice, Quot.sound]. The full statement-level index lives in the repository; a companion formalization paper is in preparation.

A note on wording: “no axioms” here means no project axioms. propext, Classical.choice, and Quot.sound are the standard classical foundations every ordinary Mathlib proof uses; we keep them and add nothing of our own.