Claims & Evidence Registrar v2 · in review

One record per semantic claim, comparator row, retired statement or open problem, every label as printed in the suite of record (Rev33.1_S369 (PDF sha256 b64ddcd9e16a6dcd…)), 336 of 357 records carry a suite quote and every one of those is machine-checked against its PDF page — the other 21 declare none and say so; every number carries its digit source. Generated from one canonical file (library_v2.jsonl, sha256 01d1a5873ede42f5b2c5f4fdcee3a4a74c09a14b99a0deea86a60ebd9c821033); the March library (v1) and the index that used to stand at the site’s Library tab are frozen in the Pasture (the archived March index; the Library tab itself is under construction by PI ruling S313); the 68 RETIRED records below are also listed there as the Retired Claims pen.

Counts, with denominators

records built (accepted at parse)357
of which CLAIM / COMPARATOR / RETIRED / OPEN / dispositions (NOT_AN_ENTRY)202 / 30 / 68 / 19 / 38
records blocked at parse (reasons)0
frozen candidates covered by an accepted record208 / 208
review stateIN_REVIEW 77, PUBLISHED 280
adjudicated by the house (internal)280 of 357. This is an internal decision by this programme about its own records.
reviewed outside this programme0. No record here has been peer-reviewed, and nothing has been published outside this programme. These are two different questions and this table keeps them apart.

Two label axes, printed side by side (no conversion)

The suite carries a mathematical status (Proved · Certified · Structural · Input · Historical) and an orthogonal physical attachment (Derived-attachment · Conditional-readout · Loaded-correspondence · Fitted · External-input) — suite p.8; the scorecard prints a tier word per row. Each record shows all three as printed at its locator; the house converts nothing (Certified is not Theorem, Input is not Axiom). The table below is the co-occurrence of the printed labels in this build — data, not a mapping rule; the suite's own crosswalk is queued (REV32.9_PENDING S304.5).

math status (as printed)attachment (as printed)scorecard tier word (as printed)records
NOT_PRINTEDNOT_PRINTEDnone printed204
StructuralNOT_PRINTEDStructural6
NOT_PRINTEDNOT_PRINTEDDerived-conditional3
NOT_PRINTEDNOT_PRINTEDLoaded3
ProvedNOT_PRINTEDnone printed3
InputNOT_PRINTEDnone printed2
StructuralLoaded-correspondencenone printed2
StructuralNOT_PRINTEDnone printed2
CertifiedNOT_PRINTEDnone printed1
NOT_PRINTEDLoaded-correspondencenone printed1
NOT_PRINTEDNOT_PRINTEDCoincidence-class1
NOT_PRINTEDNOT_PRINTEDREFUTED1
StructuralLoaded-correspondenceLoaded-correspondence1

Topic hubs (navigation, never claims)

All records

idclasstitlemath status / attachment / tier word (as printed)hubreview
LIB2-001CLAIMRoute-B admissible-gap classificationNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-002CLAIMPhysical atmospheric registration of the internal 7/16 mismatchNOT_PRINTED / Loaded-correspondence / noneH04PUBLISHED
LIB2-003COMPARATORSL-25: NuFIT 6.1 lower-octant atmospheric comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-004RETIREDRetired house atmospheric assertion: sin²θ₂₃ = 4/7— / — / noneH09PUBLISHED
LIB2-005OPENJoint basepoint and microscopic observation-map constructionNOT_PRINTED / NOT_PRINTED / noneH10IN_REVIEW
LIB2-006CLAIMThe registered symplectic exceptional substrateNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-007CLAIMThe identity-anchored complementary scalar sectorNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-008CLAIMThe Jordan-visible scalar plane fails the Lie-triple criterionNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-009CLAIMThe complementary tangent plane closes as a Lie-triple systemNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-010CLAIMThe algebra generated by the complementary tangent planeNOT_PRINTED / NOT_PRINTED / noneH01IN_REVIEW
LIB2-011CLAIMThe cubic Jordan slice is a Lagrangian boundary of the FTSNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-012CLAIMThe Albert-to-shell polarized-cubic solderNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-013CLAIMLocal positive paired-shell polarization at the transported pointNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-014CLAIMThe active braid carrier consists of twelve Clifford-module copiesNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-015CLAIMThe golden braid-word square root on the frozen carrierNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-016CLAIMThe physical-vector ten and selector ten are isomorphic modulesNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-017CLAIMThe boundary and selector tens have no equivariant linear intertwinerNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-018CLAIMDET-7 is a structural postulate in the algebraic selectorNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-019CLAIMRoute A selects the positive golden spectrum under its stated hypothesesNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-020CLAIMRoute B selects the positive golden-unit triple under DET-7NOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-021CLAIMThe finite loaded-profile parent action has its stated stable minimumNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-022CLAIMThe finite selector closure retains the stated boundary and coupling priceNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-023CLAIMThe grammar detector selects the dark rayNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-024CLAIMThe selector law and clock commutator share one structure constantNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-025CLAIMThe loaded-plane defect algebra determines the selector eigenspacesNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-026CLAIMA rank-character action represents the selector HessianCertified / NOT_PRINTED / noneH02PUBLISHED
LIB2-027CLAIMThe declared action-completion class retains nonlinear-shape freedomNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-028CLAIMThe action-shape principle is adopted rather than intrinsically selectedNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-029CLAIMThe conditional selector for occupied golden mass-ladder rungsNOT_PRINTED / NOT_PRINTED / Derived-conditionalH02PUBLISHED
LIB2-030CLAIMTarget-triviality is forced in the minimal H2 classNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-031CLAIMThe minimal H2 rank and coefficient price are predeclaredNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-032CLAIMThe frozen H2 conditions do not select the coefficient mapNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-033CLAIMThe banked refined-condition inventory does not select ΦdiagNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-034CLAIMCasimir-naturality excludes the adopted action-shape targetNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-035CLAIMThe banked non-degenerate stability conditions leave an interiorNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-036CLAIMAn action depending only on the registered Gram map cannot select a coset pointNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-037CLAIMThe declared frame-free invariant class has no nonzero dark responseNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-038CLAIMThe transported selector consumes a source without selecting its rayNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-039CLAIMA fixed-grade cubic/current law cannot detect both dark directionsNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-040CLAIMAn RB-even action cannot select the horizontal-orbit signNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-041CLAIMA frame-free invariant does not select the ordered Peirce frameNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-042CLAIMA norm-only action leaves the regular norm-level directions flatNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-043CLAIMUnshifted quadratic Kempf–Ness potentials fail the selector-rank testNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-044CLAIMA beat-invariant potential in the declared KN class cannot isolate the dark rayNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-045CLAIMThe braid/trace grammar cannot select the boundary source datumNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-046CLAIMThe golden spectrum obeys the reciprocal-square identityNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-047CLAIMThe working golden vacuum has unit Jordan determinantNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-048CLAIMThe selected Jordan vacuum pair has Gram determinant sevenNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-049CLAIMThe octonion-dimension to Jordan-rank ratio is an internal identityNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-050CLAIMThe Peirce first-row weight factors into trace and generation normalizationsNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-051CLAIMThe registered half-weight generator has fixed octonionic coefficientNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-052CLAIMThe fixed Peirce sector has the registered unique invariant generatorNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-053CLAIMFrobenius compatibility fixes the finite trace ratioNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-054CLAIMThe finite tick has an additive mirror-reversing gradingNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-055CLAIMThe finite carrier fails the cylinder-condition countNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-056CLAIMThe selected winding symmetry model has one scale classNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-057CLAIMThe retained PSL class-algebra coefficientsNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-058CLAIMThe cubic scaling model has a constant homogeneity derivativeNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-059CLAIMThe cubic coupling is relevant by the stated power countNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-060CLAIMThe solar-angle readout is conditional on ordering and the propagation interfaceNOT_PRINTED / NOT_PRINTED / Derived-conditionalH04PUBLISHED
LIB2-061CLAIMThe reactor-angle formula retains an unforced round-trip readoutStructural / NOT_PRINTED / StructuralH04PUBLISHED
LIB2-062CLAIMThe leptonic Dirac-phase readout remains conditionalNOT_PRINTED / NOT_PRINTED / Derived-conditionalH04IN_REVIEW
LIB2-063CLAIMThe framework-angle Route-B readout gives the corrected Cabibbo valueNOT_PRINTED / NOT_PRINTED / LoadedH04PUBLISHED
LIB2-064CLAIMThe measured-angle Cabibbo diagnostic is a different readout objectNOT_PRINTED / NOT_PRINTED / noneH04IN_REVIEW
LIB2-065CLAIMThe loaded first row determines its displayed Vud magnitudeNOT_PRINTED / NOT_PRINTED / LoadedH04PUBLISHED
LIB2-066CLAIMThe Vcb formula retains its loaded physical attachmentStructural / Loaded-correspondence / Loaded-correspondenceH04PUBLISHED
LIB2-067CLAIMThe Vub hierarchy relation inherits the loaded Route-B chainNOT_PRINTED / NOT_PRINTED / LoadedH04PUBLISHED
LIB2-068CLAIMThe retained CKM-phase construction remains coincidence-classNOT_PRINTED / NOT_PRINTED / Coincidence-classH04PUBLISHED
LIB2-069CLAIMThe retained CKM numeral has the printed global-phase comparisonNOT_PRINTED / NOT_PRINTED / noneH04PUBLISHED
LIB2-070CLAIMThe retained CKM numeral has a distinct direct-angle comparisonNOT_PRINTED / NOT_PRINTED / noneH04PUBLISHED
LIB2-071CLAIMCKM unitarity holds by construction in the chosen parametrisationNOT_PRINTED / NOT_PRINTED / noneH04PUBLISHED
LIB2-072CLAIMThe two CKM beta readouts remain internally inconsistentNOT_PRINTED / NOT_PRINTED / noneH04PUBLISHED
LIB2-073CLAIMThe first-row weight is not a universal Peirce-block functorNOT_PRINTED / NOT_PRINTED / noneH04PUBLISHED
LIB2-074CLAIMPMNS unitarity is exact within its standard-form constructionProved / NOT_PRINTED / noneH04PUBLISHED
LIB2-075CLAIMThe uncorrected golden argument is closer on both named CKM comparisonsNOT_PRINTED / NOT_PRINTED / noneH04IN_REVIEW
LIB2-076CLAIMThe enumerated compact embeddings fail the simultaneous-adjoint testNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-077CLAIMThe unitary matter-colour class has no image-compatible adjointNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-078CLAIMThe frame-free real 56 has no invariant rank-one Higgs projectorNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-079CLAIMThe scanned dyonic completion hosts a classical algebra-type shadowNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-080CLAIMThe shadow family cannot reproduce the registered matter multisetNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-081CLAIMThe compact-completion result is conditional and enumeration-boundedNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-082CLAIMThe extra compact Cartan is the B−L charge directionNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-083CLAIMThe loaded local matter action has a correlated Z6 kernelNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-084CLAIMThe mirror ladder reproduces an NS/R parity pattern, not a spin structureNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-085CLAIMThe finite signatures require an internal structure or its equivalent proxyNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-086CLAIMThe reflected cone metric is colour-blind at tree level within each Peirce sectorNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-087CLAIMSchur block structure does not force a zero triplet eigenvalueNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-088CLAIMGeneric cross-block Yukawa loops are not yet covered by an Artin generator censusNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-089CLAIMThe physical-to-boundary quadratic bridge space is one-dimensionalNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-090CLAIMThe boundary-to-physical quadratic bridge space is two-dimensionalNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-091CLAIMThe declared invariant-connection class cannot cancel the holonomy obstructionNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-092CLAIMNear-137 golden formulas carry no selection evidence under the stated density testNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-093CLAIMGolden-torus robustness does not select the coupling in the tested dissipative modelNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-094CLAIMA continuous Reynolds offset does not supply the discrete rung selectorNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-095CLAIMThe registered radial vacuum-decay route supplies no scale for alphaNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-096CLAIMThe available compact part is too small for compact colourNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-097CLAIMThe tested translators do not extract a common line per clock weightNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-098CLAIMThe bare Freudenthal carrier does not select the electroweak framing packageNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-099CLAIMThe orphan-doublet ruling is class-relative and the finite subgate is not the full rowNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-100CLAIMThe registered octant construction does not exclude the mirror registrationNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-101CLAIMThe registered ladder and phase census contains no selected complex rung ratioNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-102CLAIMThe registered Jordan-scaling centralizer has the printed dimension and signatureNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-103CLAIMThe registered grading centralizer has the printed dimension and signatureNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-104CLAIMThe bare quartic is not stationary at the registered golden boundary pointNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-105CLAIMThe stated split-G2 involution family yields no positive equivariant polarizationNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-106CLAIMThe exact single-chi additive ratio completion fails on the registered supportNOT_PRINTED / NOT_PRINTED / REFUTEDH05PUBLISHED
LIB2-107CLAIMThe signed metric-weighted residue cannot supply the positive seven countNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-108CLAIMThe explicit B-map fixes a loaded one-generation field dictionaryProved / NOT_PRINTED / noneH06PUBLISHED
LIB2-109CLAIMThe loaded one-generation dictionary cancels the stated anomaliesProved / NOT_PRINTED / noneH06PUBLISHED
LIB2-110CLAIMThe loaded split-octonion cubic has a nonzero invariant trilinearNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-111CLAIMThe loaded hypercharge projection gives the four Yukawa tensorsNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-112CLAIMExactly half of the raw trilinear norm lies in forbidden mirror sectorsNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-113CLAIMReynolds preservation of the registered raw coefficient rayNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-114CLAIMThe registered compensator candidates do not produce the hierarchyNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-115CLAIMThe unrestricted residue map can reproduce any positive Yukawa quartetNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-116CLAIMThe displayed one-loop trajectory produces only an order-one spreadNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-117CLAIMThe edge-uniform parent metric has zero relative Yukawa rankNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-118CLAIMThe banked parent does not determine the within-generation hierarchyNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-119CLAIMThe same-block Peirce contraction extracts the unit middle weightNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-120CLAIMW01 declares the Planck-scale top-Yukawa attachmentNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-121CLAIMThe top tree estimate retains a status-ineligible cross-scheme offsetStructural / NOT_PRINTED / StructuralH06PUBLISHED
LIB2-122CLAIMThe muon-to-tau formula is a loaded reproduced ratioStructural / Loaded-correspondence / noneH06PUBLISHED
LIB2-123CLAIMThe muon-ratio residual is the multiplicative coefficient gapNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-124CLAIMThe mass-formula chains retain three named dimensional anchorsNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-125CLAIMThe tau-anchored muon tree estimate inherits the loaded ratioStructural / Loaded-correspondence / noneH06PUBLISHED
LIB2-126CLAIMThe separate QED matching step gives the displayed physical muon massNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-127CLAIMThe electron value is the light Koide root under an external empirical ruleNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-128CLAIMThe light-quark constituent proxy uses the fitted hadronic anchorStructural / NOT_PRINTED / StructuralH06PUBLISHED
LIB2-129CLAIMThe strange constituent proxy carries the printed Casimir modifierStructural / NOT_PRINTED / StructuralH06PUBLISHED
LIB2-130CLAIMThe bottom bridge retains its tau anchor and cross-scheme offsetStructural / NOT_PRINTED / StructuralH06PUBLISHED
LIB2-131CLAIMThe charm bridge remains constituent-anchored and cross-schemeStructural / NOT_PRINTED / StructuralH06PUBLISHED
LIB2-132CLAIMThe tested untuned running and matching readings do not remove the heavy-quark offsetsNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-133CLAIMThe outer-mirror charged-lepton fit consumes two free gapsInput / NOT_PRINTED / noneH06PUBLISHED
LIB2-134CLAIMThe literal Jordan-adjoint neutrino mass reading fails its splitting-ratio testNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-135CLAIMThe spectral-gap model imposes its self-consistency through the lifted cone traceNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-136CLAIMThe baryonic cubic channel is distinct from the cancelled quadratic channelNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-137CLAIMThe cone expansion uses a spectral background rather than stationarity of the cubicNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-138CLAIMThe compact two-scale Gram class excludes its previously priced half-ratioNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-139CLAIMThe declared top-Yukawa boundary has a separately reported running valueNOT_PRINTED / NOT_PRINTED / noneH06PUBLISHED
LIB2-140CLAIMThe selected neutrino rung is a below-floor edge target, not a mass relationStructural / NOT_PRINTED / noneH07IN_REVIEW
LIB2-141CLAIMThe neutrino depth assignment is post-hoc and receives no blind creditNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-142CLAIMThe lightest-mass boundary has mass-sum and beta-decay corollariesNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-143CLAIMThe exhibited winding-to-Fibonacci functor defines the finite cluster imageNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-144CLAIMThe cluster-ledger interface is the declared weight-to-energy mapNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-145CLAIMThe small-nucleus kernel is triangularly saturatedNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-146CLAIMThe closed alpha-cell typing gives the A = 5 gapNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-147CLAIMThe two-alpha typing gives a negative first correction at A = 8NOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-148CLAIMThe composition ladder is a finite trace invariantNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-149CLAIMThe residual-circulation weights obey the printed piecewise ruleNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-150CLAIMThe suite reports a sealed pentagon-weight matchNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-151CLAIMThe suite reports a sealed ninth-weight matchNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-152CLAIMThe Hoyle excitation passes the source's frozen barNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-153CLAIMThe freeze-state ledger records sharp passes and a separately typed obstructionNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-154CLAIMThe silicon residual passed its original bar and took the typed-obstruction branchNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-155CLAIMThe charge-magnitude ledger retains two exposed proton-separation defectsNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-156CLAIMThe direct Markov-second-moment repair has the wrong signNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-157CLAIMThe connected second moment does not switch off at the later cellsNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-158CLAIMThe tested perturbative annular attachment does not explain the deficit windowNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-159CLAIMThe separate silicon readout remains a three-way forkNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-160CLAIMThe fixed-Z isospin coefficient is selected rather than derivedNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-161CLAIMThe registered up–down operation is a parity, not a derived isospin actionNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-162CLAIMThe registered breathing weight is mirror-even and charge-blindNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-163CLAIMThe separation-energy rule uses the refined daughter ledgerNOT_PRINTED / NOT_PRINTED / noneH07IN_REVIEW
LIB2-164CLAIMThe draft glueball pair falls in the two printed frozen bandsNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-165CLAIMThe finite Gaussian OS subgate is reported as a conditional checkpointNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-166CLAIMThe toy resolvent remains a finite conditional checkpointNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-167CLAIMThe motivated clock seed is extra structure, not an energy order of tensor layersNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-168CLAIMThe trace-built MacDowell–Mansouri action is a signature-sector candidateNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-169CLAIMThe Euclidean MM/EH action has the stated conformal instabilityNOT_PRINTED / NOT_PRINTED / noneH07IN_REVIEW
LIB2-170CLAIMA reflection-positive Cartan state exists at finite regulatorNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-171CLAIMThe pure MacDowell–Mansouri quadratic form is not a positive covarianceNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-172CLAIMThe positive completion cone has a strict coefficient domainNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-173CLAIMThe ordered state pair supplies the additive relative modular scoreNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-174CLAIMThe record-quotient observation composite is unique under its seven premisesNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-175CLAIMThe supported MOS quotient has rank three and relative rank twoNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-176CLAIMHistory, character and boundary record are one registered record typeNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-177CLAIMThe realized history is sample data rather than a value selected by its lawNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-178CLAIMThe locked basepoint census has no qualifying intrinsic datumNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-179CLAIMThe registered stabilizer has no nonzero invariant odd covectorNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-180CLAIMThe transported A689 grading has trivial rather than alternating characterNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-181CLAIMThe local covariant odd response is one orbit with an unselected torsorNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-182CLAIMThe MOS channel family permits a range of odd-response amplitudesNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-183CLAIMThe reversal-covariant score solder bounds the product responseNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-184CLAIMThe registered normalization census contains no forcing rowNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-185CLAIMThe rank-two support certificate excludes a rank-five extension at the MOS tierNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-186CLAIMThe unit grade-four response is a declared premiseNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-187CLAIMThe unadopted response alternatives retain distinct meaningsNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-188CLAIMThe registered free quaternionic fermion determinant is non-negativeNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-189CLAIMThe anisotropic heat-kernel family has nonlinear OS positivity in its coneNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-190CLAIMNo positive path in the declared heat-kernel family reaches pure MM/EHNOT_PRINTED / NOT_PRINTED / noneH07IN_REVIEW
LIB2-191CLAIMThe stated bivector simplicity condition cannot be imposed by a linear projectorNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-192CLAIMA soft positive simplicity weight exists at finite regulatorNOT_PRINTED / NOT_PRINTED / noneH07IN_REVIEW
LIB2-193CLAIMThe registered Clifford construction has a one-particle bare gapNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-194CLAIMThe frozen Clifford law makes every registered carrier-map Gram isotropicNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-195CLAIMThe frozen symplectic braid representation has a nonscalar centreNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-196CLAIMThe specified classical vacuum spectrum is reproduced by CSS charge sumsNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-197CLAIMThe positive congruence dressing stays inside the registered E7 groupNOT_PRINTED / NOT_PRINTED / noneH01PUBLISHED
LIB2-198CLAIMThe MRSS Higgs parity is unique only under the loaded scalar spectrumNOT_PRINTED / NOT_PRINTED / noneH05PUBLISHED
LIB2-199CLAIMThe weak-angle value remains a structural target on a scheme-dependent curveStructural / NOT_PRINTED / noneH04PUBLISHED
LIB2-200CLAIMThe AX6 polarization postulate gives its readout without selecting itselfNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-201CLAIMThe parked moment model records a traversal with sixty winding ticksNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-202CLAIMThe specified constant set cannot supply a duration in secondsNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-203CLAIMThe parked Gogberashvili splice imports an external time axisNOT_PRINTED / NOT_PRINTED / noneH07PUBLISHED
LIB2-204COMPARATORSL-01: NuFIT solar mass-squared splitting comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-205COMPARATORSL-02: NuFIT atmospheric splitting with SK-ATMNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-206COMPARATORSL-03: NuFIT atmospheric splitting without SK-ATM— / — / noneH08IN_REVIEW
LIB2-207COMPARATORSL-04: DESI baseline neutrino-mass-sum upper boundNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-208COMPARATORSL-05: DESI Feldman–Cousins neutrino-mass-sum upper boundNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-209COMPARATORSL-06: MS-bar weak-angle comparator at the Z scaleNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-210COMPARATORSL-07: MS-bar strange Yukawa comparator— / — / noneH08IN_REVIEW
LIB2-211COMPARATORSL-08: MS-bar bottom Yukawa comparator— / — / noneH08IN_REVIEW
LIB2-212COMPARATORSL-09: Global-fit CKM Dirac phase in radiansNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-213COMPARATORSL-10: Global-fit Jarlskog invariant comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-214COMPARATORSL-11: First-row Cabibbo-magnitude comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-215COMPARATORSL-12: Retained PDG |Vub| comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-216COMPARATORSL-13: Retained PDG |Vcb| comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-217COMPARATORSL-14: First-row |Vud| comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-218COMPARATORSL-15: MS-bar charm mass at its self-scaleNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-219COMPARATORSL-16: MS-bar bottom mass at its self-scaleNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-220COMPARATORSL-17: Direct/MC top-mass comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-221COMPARATORSL-18: Measured tau-mass anchorInput / NOT_PRINTED / noneH08PUBLISHED
LIB2-222COMPARATORSL-19: Global-fit CKM Dirac phase in degreesNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-223COMPARATORSL-20: Direct unitarity-triangle angle comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-224COMPARATORSL-21: On-shell weak-angle comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-225COMPARATORSL-22: Effective-leptonic weak-angle comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-226COMPARATORSL-23: NuFIT squared-sine reactor-angle comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-227COMPARATORSL-24: NuFIT solar angle in degreesNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-228COMPARATORSL-26: NuFIT reactor angle in degreesNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-229COMPARATORSL-27: House-computed candidate coefficient diagnosticNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-230COMPARATORSL-28: Historical PDG |Vcb| comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-231COMPARATORSL-29: Historical PDG |Vub| comparatorNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-232COMPARATORSL-30: Global-fit Jarlskog comparator in the printed scaled unitsNOT_PRINTED / NOT_PRINTED / noneH08PUBLISHED
LIB2-233RETIREDRetired blanket zero-parameter observable headline— / — / noneH09PUBLISHED
LIB2-234RETIREDRetired 20/20 Standard-Model completion headline— / — / noneH09PUBLISHED
LIB2-235RETIREDSuperseded three-of-eight mixing tally and pending atmospheric hold— / — / noneH09PUBLISHED
LIB2-236RETIREDRetired Wyler bounded-domain derivation of alpha— / — / noneH09PUBLISHED
LIB2-237RETIREDRetired exact-framework Cabibbo correction 0.225247— / — / noneH09PUBLISHED
LIB2-238RETIREDSuperseded rounded-angle Cabibbo value as the canonical readout— / — / noneH09PUBLISHED
LIB2-239RETIREDDeprecated house Cabibbo-comparator route— / — / noneH09PUBLISHED
LIB2-240RETIREDRetired Shilov atmospheric-angle derivation— / — / noneH09PUBLISHED
LIB2-241RETIREDRetired claim that the chirality interface selected the atmospheric octant— / — / noneH09PUBLISHED
LIB2-242RETIREDSuperseded trimaximal cosine-phase correction apparatus— / — / noneH09IN_REVIEW
LIB2-243RETIREDSuperseded trimaximal condition and rho-modulus apparatus— / — / noneH09IN_REVIEW
LIB2-244RETIREDSuperseded hybrid leptonic-phase formula— / — / noneH09IN_REVIEW
LIB2-245RETIREDRetired physical use of the PSL class-algebra sign argument— / — / noneH09IN_REVIEW
LIB2-246RETIREDRetired legacy baryon-to-meson mass ratio— / — / noneH09PUBLISHED
LIB2-247RETIREDWithdrawn proof and zero-parameter status of the muon-to-tau ratio— / — / noneH09PUBLISHED
LIB2-248RETIREDWithdrawn universal two-parameter mass-completion no-go— / — / noneH09PUBLISHED
LIB2-249RETIREDRetired Det-squared selection of the polarization postulate— / — / noneH09PUBLISHED
LIB2-250RETIREDWithdrawn Schur-only proof of vanishing triplet masses— / — / noneH09PUBLISHED
LIB2-251RETIREDScoped withdrawal of blanket Artin protection for Yukawa loops— / — / noneH09PUBLISHED
LIB2-252RETIREDWithdrawn canonical reactor half-angle from the moment law— / — / noneH09PUBLISHED
LIB2-253RETIREDRetired structural derivation rating of the CKM phase construction— / — / noneH09PUBLISHED
LIB2-254RETIREDWithdrawn universal claim that inequality conditions cannot reduce dimension— / — / noneH09PUBLISHED
LIB2-255RETIREDRetired use of one operator name for Wick chart and shell reversal— / — / noneH09PUBLISHED
LIB2-256RETIREDSuperseded nontrivial bundle reading of the signature sheets— / — / noneH09PUBLISHED
LIB2-257RETIREDRetired one-bit accounting of distinct gluing and observation structures— / — / noneH09PUBLISHED
LIB2-258RETIREDRetired finite-sign chamber-lift price computed on the wrong carrier— / — / noneH09PUBLISHED
LIB2-259RETIREDWithdrawn aggregate bit-and-dimension freedom headline— / — / noneH09PUBLISHED
LIB2-260RETIREDRetired microscopic selector-deriving status of the earlier parent action— / — / noneH09PUBLISHED
LIB2-261RETIREDRetired independent-channel source doorway— / — / noneH09PUBLISHED
LIB2-262RETIREDWithdrawn unconditional action preference for the root line— / — / noneH09PUBLISHED
LIB2-263RETIREDRetired depth-exclusion inference from commuting charge and mass— / — / noneH09PUBLISHED
LIB2-264RETIREDWithdrawn claim that the promotion functional was constructed and run— / — / noneH09PUBLISHED
LIB2-265RETIREDSuperseded Wyler-baseline route for the muon mass— / — / noneH09PUBLISHED
LIB2-266RETIREDSuperseded electromagnetic-power Wyler formula for the muon— / — / noneH09PUBLISHED
LIB2-267RETIREDSuperseded sub-Wyler route for the electron mass— / — / noneH09PUBLISHED
LIB2-268RETIREDSuperseded extended-Wyler route for the tau mass— / — / noneH09PUBLISHED
LIB2-269RETIREDSuperseded Peirce-cylinder proposal for the tau mass— / — / noneH09PUBLISHED
LIB2-270RETIREDSuperseded D-tower formula for the bottom mass— / — / noneH09PUBLISHED
LIB2-271RETIREDSuperseded pi-weighted prefactor formula for the bottom mass— / — / noneH09PUBLISHED
LIB2-272RETIREDSuperseded cylinder-prefactor proof prompt for the bottom mass— / — / noneH09PUBLISHED
LIB2-273RETIREDSuperseded D-tower formula for the charm mass— / — / noneH09PUBLISHED
LIB2-274RETIREDSuperseded triality log-geometric-mean charm formula— / — / noneH09PUBLISHED
LIB2-275RETIREDSuperseded cubic-to-tower triality bridge for the charm mass— / — / noneH09PUBLISHED
LIB2-276RETIREDSuperseded resummed-electromagnetic charm formula— / — / noneH09PUBLISHED
LIB2-277RETIREDSuperseded early cubic-phase ansatz for the leptonic Dirac phase— / — / noneH09IN_REVIEW
LIB2-278RETIREDSuperseded imaginary-correction prompt for the leptonic phase— / — / noneH09IN_REVIEW
LIB2-279RETIREDSuperseded determinant-imaginary-part route for the full leptonic phase— / — / noneH09IN_REVIEW
LIB2-280RETIREDSuperseded sum-rule and torsion-corrected reactor route to the leptonic phase— / — / noneH09IN_REVIEW
LIB2-281RETIREDSuperseded cylinder formula for the reactor angle— / — / noneH09PUBLISHED
LIB2-282RETIREDSuperseded torsion-corrected cylinder formula for the reactor angle— / — / noneH09PUBLISHED
LIB2-283RETIREDSuperseded torsion-corrected PMNS angle scheme— / — / noneH09PUBLISHED
LIB2-284RETIREDSuperseded Shilov-circle correction prompt for the atmospheric angle— / — / noneH09PUBLISHED
LIB2-285RETIREDSuperseded Peirce golden-power assignment for two CKM magnitudes— / — / noneH09PUBLISHED
LIB2-286RETIREDSuperseded additive correction prompt for Vcb— / — / noneH09PUBLISHED
LIB2-287RETIREDSuperseded golden-power ratio of CKM hierarchy magnitudes— / — / noneH09PUBLISHED
LIB2-288RETIREDSuperseded Cabibbo-squared formula for Vcb— / — / noneH09PUBLISHED
LIB2-289RETIREDSuperseded reciprocal weak-angle proposal— / — / noneH09PUBLISHED
LIB2-290RETIREDSuperseded logarithmic loop-correction prompt for the weak angle— / — / noneH09PUBLISHED
LIB2-291RETIREDSuperseded cylinder-running proof prompt for the weak angle— / — / noneH09PUBLISHED
LIB2-292RETIREDSuperseded electromagnetic-subtraction formula for the weak angle— / — / noneH09PUBLISHED
LIB2-293RETIREDSuperseded QLC-plus-cylinder correction for the Cabibbo angle— / — / noneH09PUBLISHED
LIB2-294RETIREDSuperseded torsion-corrected Cabibbo–Weinberg formula— / — / noneH09PUBLISHED
LIB2-295RETIREDSuperseded Cabibbo–Weinberg residual identity as a physical target— / — / noneH09PUBLISHED
LIB2-296RETIREDSuperseded singular-vacuum premise of the protection-and-bounce chain— / — / noneH09PUBLISHED
LIB2-297RETIREDRetired compact-colour subgroup claim in the split-G2 real form— / — / noneH09PUBLISHED
LIB2-298RETIREDWithdrawn physical-generation implication of the triality carrier cycle— / — / noneH09PUBLISHED
LIB2-299OPENDerive the anchor relations required by the physical one-input programme— / — / noneH10IN_REVIEW
LIB2-300OPENConstruct the missing continuum Yang–Mills functor— / — / noneH10IN_REVIEW
LIB2-301OPENTest Einstein universality of the finite-regulator gravity construction— / — / noneH10IN_REVIEW
LIB2-302OPENConstruct the normalized physical mass-response map— / — / noneH10IN_REVIEW
LIB2-303OPENConstruct the packing or coordination explanation of the deficit window— / — / noneH10IN_REVIEW
LIB2-304OPENDerive the configuration-dependent charge-magnitude mechanism— / — / noneH10IN_REVIEW
LIB2-305OPENSupply the missing QCD flip energy in the neutron–proton splitting— / — / noneH10IN_REVIEW
LIB2-306OPENResolve the parent breathing-mode accounting— / — / noneH10IN_REVIEW
LIB2-307OPENConstruct the interacting chiral determinant-line trivialization— / — / noneH10IN_REVIEW
LIB2-308OPENDerive the sign that selects the atmospheric-octant registration— / — / noneH10IN_REVIEW
LIB2-309OPENDerive one source law for the real ladder step and compact phase— / — / noneH10IN_REVIEW
LIB2-310OPENDerive the scheme-specific weak-angle matching bridge— / — / noneH10IN_REVIEW
LIB2-311OPENFind a non-residue physical realization of the finite index normalization— / — / noneH10IN_REVIEW
LIB2-312OPENSupply a scheme-matched physical comparison for the top tree estimate— / — / noneH10IN_REVIEW
LIB2-313OPENDerive physical matching for the tau-anchored bottom bridge— / — / noneH10IN_REVIEW
LIB2-314OPENDerive the constituent-to-running-mass bridge for charm— / — / noneH10IN_REVIEW
LIB2-315OPENForce the reactor-angle readout rather than choose its normalization— / — / noneH10IN_REVIEW
LIB2-316OPENSelect the invariant required by the CKM-phase construction— / — / noneH10IN_REVIEW
LIB2-317NOT_AN_ENTRYReference metadata for imported Standard-Model running constants— / — / noneH00IN_REVIEW
LIB2-318NOT_AN_ENTRYSource hold on the Track-2 gauge-completeness gates— / — / noneH05IN_REVIEW
LIB2-319NOT_AN_ENTRYMerge the generic measured-scale statements as input metadata— / — / noneH00IN_REVIEW
LIB2-320NOT_AN_ENTRYProspective publication-test policy is not a scientific result— / — / noneH00IN_REVIEW
LIB2-321NOT_AN_ENTRYPublication-evidence availability belongs in release metadata— / — / noneH00IN_REVIEW
LIB2-322NOT_AN_ENTRYTaxonomy and validator descriptions are schema metadata— / — / noneH00IN_REVIEW
LIB2-323NOT_AN_ENTRYBoundary-condition-family ruling is premise metadata— / — / noneH00IN_REVIEW
LIB2-324NOT_AN_ENTRYSEL-27 declaration status is workflow metadata— / — / noneH00IN_REVIEW
LIB2-325NOT_AN_ENTRYThe basepoint subgroup symbol is a typed placeholder— / — / noneH00IN_REVIEW
LIB2-326NOT_AN_ENTRYSource inventory and resolver tools are provenance metadata— / — / noneH00IN_REVIEW
LIB2-327NOT_AN_ENTRYThe assumption-stack heading is programme-reference metadata— / — / noneH00IN_REVIEW
LIB2-328NOT_AN_ENTRYSource hold on the integral cubic coordinate map— / — / noneH01IN_REVIEW
LIB2-329NOT_AN_ENTRYSource hold on the Peirce–compact chirality-plane obstruction— / — / noneH05IN_REVIEW
LIB2-330NOT_AN_ENTRYSource hold on the Cayley-plus-triality frame conversion— / — / noneH01IN_REVIEW
LIB2-331NOT_AN_ENTRYSource hold on the primitive integral Lagrangian halves— / — / noneH01IN_REVIEW
LIB2-332NOT_AN_ENTRYSource hold on the grading-homogeneous magnetic section— / — / noneH01IN_REVIEW
LIB2-333NOT_AN_ENTRYSource hold on the Roman–clock finite-inventory comparison— / — / noneH05IN_REVIEW
LIB2-334NOT_AN_ENTRYRoman–clock orientation-parity interface remains a proposal— / — / noneH01IN_REVIEW
LIB2-335NOT_AN_ENTRYSource hold on the two distinct Hessian-trace quantities— / — / noneH07IN_REVIEW
LIB2-336NOT_AN_ENTRYSource-equivalence hold on the AX2-elimination header— / — / noneH02IN_REVIEW
LIB2-337NOT_AN_ENTRYSource-equivalence hold on the Jordan-boundary selector header— / — / noneH02IN_REVIEW
LIB2-338NOT_AN_ENTRYSource hold on the forced AdS base-manifold seed— / — / noneH07IN_REVIEW
LIB2-339NOT_AN_ENTRYSource hold on the CKM channel CP decomposition— / — / noneH04IN_REVIEW
LIB2-340NOT_AN_ENTRYSource hold on the CKM mixed-parity statement— / — / noneH04IN_REVIEW
LIB2-341NOT_AN_ENTRYSource hold on the universal mass-cascade assertion— / — / noneH06IN_REVIEW
LIB2-342NOT_AN_ENTRYCharge/gauge provenance terminal is a source-backed overview— / — / noneH00IN_REVIEW
LIB2-343NOT_AN_ENTRYSource hold on the house electroweak-loop scale— / — / noneH04IN_REVIEW
LIB2-344CLAIMThe generation-count forcing skeleton remains conditionalNOT_PRINTED / NOT_PRINTED / noneH02PUBLISHED
LIB2-345RETIREDSuperseded use of the first JUNO oscillation comparison— / — / noneH09PUBLISHED
LIB2-346NOT_AN_ENTRYSource hold on the Gate-B matter-functor construction— / — / noneH05IN_REVIEW
LIB2-347NOT_AN_ENTRYSource hold on the meson binding-ratio formula— / — / noneH07IN_REVIEW
LIB2-348NOT_AN_ENTRYSource hold on non-associativity as the source of hierarchy steepness— / — / noneH06IN_REVIEW
LIB2-349NOT_AN_ENTRYSource-equivalence hold on the octonionic democracy postulate— / — / noneH02IN_REVIEW
LIB2-350NOT_AN_ENTRYPeirce-block anti-error heading is reference metadata— / — / noneH00IN_REVIEW
LIB2-351NOT_AN_ENTRYSource hold on the earlier solar-angle obstruction— / — / noneH04IN_REVIEW
LIB2-352NOT_AN_ENTRYSource hold on the T-matrix versus propagator residue comparison— / — / noneH07IN_REVIEW
LIB2-353NOT_AN_ENTRYSource hold on the wall-contact operator and pairing-order map— / — / noneH07IN_REVIEW
LIB2-354NOT_AN_ENTRYSource hold on the indefinite partition-function divergence claim— / — / noneH07IN_REVIEW
LIB2-355NOT_AN_ENTRYThe charge-clock-knot tower remains on a source hold, not retired— / — / noneH07IN_REVIEW
LIB2-356CLAIMThe internal mismatch identity is distinct from atmospheric registrationNOT_PRINTED / NOT_PRINTED / noneH03PUBLISHED
LIB2-357NOT_AN_ENTRYUnidentified additional parity-lemma proposal is not an entry— / — / noneH00IN_REVIEW

For AI reviewers: how to check this library from the site

  1. Fetch /library-v2/index.json and print its count and build_sha as your first line. If you cannot fetch it, write NOT RUN and stop.
  2. For each entry you are asked to review, open /library-v2/<id>/ (or its index.json). Every quote names a PDF page; open the suite-text part linked beside it, find ===== PDF PAGE n / N ===== (N = the page count of the sealed PDF), and check the quote and the label words on that page.
  3. Return one text line per entry: id | PASS or FAIL(G1–G8) or NOT RUN | quote | PDF page | one sentence. Never propose a tier; never compute a σ; say what the page says.
  4. Machine surfaces: library_v2.jsonl (canonical), index.json (capsules), suite text, SOURCE_LEDGER_REV32.csv.

Generated from library_v2.jsonl. Declared volatile fields (R36): BUILD_STAMP.
BUILD_STAMP S371a · 2026-09-26T22:53Z · master 01d1a5873ede42f5 · cut 9dcc6ce9a8ee3e02