Where the programme puts what it no longer prints — kept whole, dated, and one click from what replaced it. Nothing here is current; everything here is how it stood. Build S371a · 2026-09-26 22:53Z.
What replaced what: every v2 record names its March antecedents under History; a retired March statement appears in the Retired Claims pen with the decision that retired it.
| id | retired statement | where it stood | retiring decision | what the suite prints now | successors |
|---|---|---|---|---|---|
| LIB2-004 | Retired house atmospheric assertion: sin²θ₂₃ = 4/7 sin²θ₂₃ = 4/7 — atmospheric mixing angle; STATUS: Y3 — DERIVED (math + 1 ODP-type postulate) | LIBRARY_V2_CANDIDATE_LIST_S304.csv, C2-169: L-Sin2Theta23_atmospheric_mixing.md (header and S173 flag) | S173 SUPERSEDED flag reproduced in C2-169; no explicit sentence naming the retired fraction located in the supplied suite. | The current physical θ23 row is therefore Loaded-correspondence; the number and the internal theorem do not move.PDF p.59 | LIB2-002 |
| LIB2-233 | Retired blanket zero-parameter observable headline [Group G: Precision Tests and Anomalies] TIER A-STAR OBSERVABLES — ZERO PARAMETER SUMMARY | LIBRARY_V1_GROK_ARCHIVE_S304.md, L71; pre-Rev29 blanket observable summary | S112 claim-language enforcement, carried in Rev32.7 Paper 0 p.8; Rev29 row-by-row re-tiering | Phrasings such as “100/100,” “all green,” “zero free parameters” (for the suite as a whole), “closed,” and “emergence” are retired except where a Proved-tier theorem licenses them.PDF p.8 | LIB2-060, LIB2-063, LIB2-124 |
| LIB2-234 | Retired 20/20 Standard-Model completion headline P72: m_s from J₁₃ Peirce Sector D_IV(4) — 20/20 SM Observables (gap 0.46%) — completion clause only. | LIBRARY_V1_GROK_ARCHIVE_S304.md, P72, 20/20 completion clause | Rev29 scope re-tiering as carried by Rev32.7 Paper 0 p.8 and Paper 3 §5.4; individual old production chronology not supplied | Two physical rows sit at derived-conditional, each with its premise printed beside it rather than PMNS and δ buried: θ12 CP .PDF p.59 | LIB2-060, LIB2-062, LIB2-129 |
| LIB2-235 | Superseded three-of-eight mixing tally and pending atmospheric hold The v1.3 mixing summary mirrored the theta23 CONTESTED hold with the 3/8 tally retained pending PI ruling. | LIBRARY_V2_CANDIDATE_LIST_S304.csv, C2-098; Track-2 v1.3 G-MIX-01 | A1566/D1244 atmospheric retype, Rev32.6; current Rev32.7 Paper 3 §5.4 | Two physical rows sit at derived-conditional, each with its premise printed beside it rather than PMNS and δ buried: θ12 CP .PDF p.59 | LIB2-002, LIB2-060, LIB2-062 |
| LIB2-236 | Retired Wyler bounded-domain derivation of alpha The alpha_em conjecture was marked CLOSED, and the Wyler D_IV(5) formula was presented as an alpha_em derivation proof. | Library v1 L103, L148, L271, P5, P56; C2-137/C2-153/C2-175 Wyler-programme headers | Appendix N §1.1, s256/S165; S174 RETIRED — WYLER PROGRAM flags reproduced in the three candidate rows | The bounded-domain programme is retired as a derivation of α.PDF p.252 | — |
| LIB2-237 | Retired exact-framework Cabibbo correction 0.225247 The exact-framework readout is |Vus| = 0.225247; the accompanying angle correction was 33.4877°. | Rev32.5 Paper 3 correction; Track-2 v1.3 D-MIX-05, candidate C2-062 | Rev32.6 correction from s1162, A1572, recorded in Rev32.7 Paper 3 §2 p.47 | current value is |Vus | = 0.225256 (the exact framework angle arctan( 3/ϕ2 ) = 33.4880◦ , printed from the kernel line s1162;PDF p.47 | LIB2-063 |
| LIB2-238 | Superseded rounded-angle Cabibbo value as the canonical readout The canonical |Vus| display through Rev32.4 was 0.225268, from the rounded 33.49° solar angle. | Through-Rev32.4 Cabibbo display, described in Rev32.7 Paper 3 §2 p.47; stale C2-009 body | Rev32.6 exact-framework replacement from s1162, A1572, carried at Rev32.7 | current value is |Vus | = 0.225256 (the exact framework angle arctan( 3/ϕ2 ) = 33.4880◦ , printed from the kernel line s1162;PDF p.47 | LIB2-063 |
| LIB2-239 | Deprecated house Cabibbo-comparator route L-CabDisc — Cabibbo Angle / V_us from Algebraic Structure; STATUS: CF2 ROUTE B — GREEN (D188b/A333, 3-AI consensus, 2026-04-10); ⚠ NOT HOMED — ROUTE DEPRECATED (S270, item 7.3); The deprecated Cabibbo-comparator route i… | LIBRARY_V2_CANDIDATE_LIST_S304.csv, C2-147: L-CabDisc_Cabibbo_angle_discrete.md | S270 item 7.3 ROUTE DEPRECATED flag in C2-147; the specific old Cabibbo-comparator statement is not located in the supplied suite | The first row is Loaded: Route B was selected after comparison with kaon data.PDF p.47 | LIB2-063 |
| LIB2-240 | Retired Shilov atmospheric-angle derivation θ₂₃(PMNS) = arctan(1 + 1/(2π)) Shilov Derivation [CLOSED, 0.03%]. | LIBRARY_V1_GROK_ARCHIVE_S304.md, L255; C2-168, L-Shilov23_Shilov_boundary_factor.md | S174 RETIRED — WYLER PROGRAM + STALE θ23 flag; current replacement in Paper 7 p.116 and Paper 3 p.59 | The current framework value is the mismatch-geometry branch sin2 θ23 = 7/16, rather than the older higher-octant phenomenological placeholder — printed since Rev32.6 as the sharp loaded lower-branch target of the selected corre- spondence (A1566: the octant r…PDF p.116 | LIB2-002 |
| LIB2-241 | Retired claim that the chirality interface selected the atmospheric octant Rev32.5: “selector built”, “locked to εQ” and “free bits 2 → 1”. | Rev32.5 octant-selection assertions, quoted in Rev32.7 Appendix N §6 p.257 | A1566/D1244, Rev32.6; s501 retyped after the s1156 countermap test | The current physical θ23 row is therefore Loaded-correspondence; the number and the internal theorem do not move.PDF p.59 | LIB2-002, LIB2-100 |
| LIB2-242 | Superseded trimaximal cosine-phase correction apparatus L-D115Erratum — cos δ_TM1 Correction; STATUS: ERRATUM (corrects D115 ChatGPT); ⚠ SUPERSEDED (flagged S173, lost-sheep sweep): Part of the retired TM1/trimaximal apparatus (0 hits in the suite); cos δ_TM1 ≈ +0.25 at exac… | LIBRARY_V2_CANDIDATE_LIST_S304.csv, C2-152: L-D115Erratum_cosδ_TM1_correction.md | S173 SUPERSEDED flag for the retired TM1/trimaximal apparatus; not located in suite | δCP = −2π/ 5 = −160.997◦PDF p.84 | LIB2-062 |
| LIB2-243 | Superseded trimaximal condition and rho-modulus apparatus L-TM1rho — TM1 Condition and ρ Modulus; STATUS: INDEPENDENT — TM1 requires 1 extra postulate. NOT derived from J₃(𝕆ₛ). | LIBRARY_V2_CANDIDATE_LIST_S304.csv, C2-173: L-TM1rho_TM1_condition.md | S173 SUPERSEDED flag for the TM1/trimaximal apparatus; not located in suite | δCP = −2π/ 5 = −160.997◦PDF p.84 | LIB2-060, LIB2-061, LIB2-062 |
| LIB2-244 | Superseded hybrid leptonic-phase formula δ_CP=arg(ω₇·e^{iπ/5})≈−160.9°; STATUS: Y1 — SIGN DERIVED (D161 ★★★★), k=1 PROPOSED (D147, naturalness) | LIBRARY_V2_CANDIDATE_LIST_S304.csv, C2-159: L-HybridDelta_hybrid_CP_phase.md | S173 SUPERSEDED flag in C2-159; replacement V3 phase readout in Paper 5 §3 p.84 | δCP = −2π/ 5 = −160.997◦PDF p.84 | LIB2-062 |
| LIB2-245 | Retired physical use of the PSL class-algebra sign argument The class-algebra sign argument left −arccos(−1/3) − 2π/7 = −160.900° as the only allowed phase sign. | Paper 8 §2 p.118, old chirality application; C2-172 L-StructConst_PSL27_structure_constants.md | Application deprecated in Paper 8 §2; S174 APPLICATION SUPERSEDED flag; class algebra itself retained | That application is deprecated. The authoritative CP phase is δCP = −2π/ 5 = −160.997◦ from the V3 rotation theorem (⋆100; Paper 5, Appendix C), which does not involve PSL(2, 7) at all;PDF p.118 | LIB2-062 |
| LIB2-246 | Retired legacy baryon-to-meson mass ratio M_B/M_M ≈ 6.7 matched the proton/pion value at one free coupling, with a stated ratio range 5–8 across perturbative couplings. | C2-142 L-BaryonMesonRatio_mass_ratio_from_algebra.md; historical S23–S24 calculation described in Paper 8 §4 p.121 | s284/S175 current-frame recompute; explicit numerical retirement in Paper 8 p.121 and Appendix I p.210 | The number is therefore retired — a legacy null-cone artifact superseded by the current frame, not a parked candidate.PDF p.121 | LIB2-136 |
| LIB2-247 | Withdrawn proof and zero-parameter status of the muon-to-tau ratio The muon-to-tau ratio was printed as Proved / zero-parameter / forced by algebra, no fit. | Through-Rev28 ratio classification, described in Paper 2 p.33 and Appendix X p.335; C2-018/C2-056 | Rev29 charged-lepton re-tiering, explicitly carried in Paper 2 §3.2 and Appendix X | The rows of this subsection therefore stand at Structural (mathematical tier), Loaded-correspondence (physical attachment) and Reproduced (numerical status): the ratio is reproduced, not derived.PDF p.33 | LIB2-122, LIB2-123, LIB2-125 |
| LIB2-248 | Withdrawn universal two-parameter mass-completion no-go ≤ 2-parameter completion is impossible. | Earlier mass-completion claim, quoted in Appendix O §5, Remark 5.2 p.261; Executive State Map casualty #6 | Withdrawal recorded in Appendix O Remark 5.2 after the fitted period-70 harmonic control; Executive State Map p.7 | The blanket “≤ 2-parameter completion is impossible” claim is therefore withdrawn; the honest statement is that surveyed one-parameter forms fail and no universal ≤ 2-parameter no-go is proved.PDF p.261 | LIB2-106 |
| LIB2-249 | Retired Det-squared selection of the polarization postulate The degree-six Det2 selector cos(6ψ) = 1/2, with its 50° branch, selected AX6pol and its weak-angle readout. | Former AX6/ψ-star identification, reconstructed as the explicitly withdrawn identification in Paper 4 §7 p.73; C2-125 | Rev32.2 two-object repair; A1549/s1135 and PI ruling S295, carried in Paper 4 §7 p.73 | The Det2 object is therefore retired as a selector of AX6pol ; A667 remains correct for the 50◦ object only and does not constrain AX6pol .PDF p.73 | LIB2-200 |
| LIB2-250 | Withdrawn Schur-only proof of vanishing triplet masses Schur block structure implies “zero entries for all triplet components at every loop order.” | Earlier Appendix A proof sketch, quoted and withdrawn in Rev32.1; retained withdrawal at Rev32.7 p.146 | A1538 F1, Rev32.1 Schur gauge-protection withdrawal; S290.4 falsifier-control note | the previous version of this sketch concluded “zero entries for all triplet components at every loop order” from the block structure; that inference is withdrawn — Schur permits a nonzero scalar on each triplet block,PDF p.146 | LIB2-087 |
| LIB2-251 | Scoped withdrawal of blanket Artin protection for Yukawa loops Standard Yukawa and gauge-coupling running is “fully protected” by Artin without establishing the internal two-generator containment of each diagram. | Earlier blanket Artin bridge, scoped in Rev32.1 Appendix A §A.7.8, Corollary 0.16; C2-114 | A1538 F5, Rev32.1 scope correction; Appendix A pp.147–148 | the blanket “fully protected” claim is scoped Rev32.1 pending the generator census (A1538 F5).PDF p.148 | LIB2-088 |
| LIB2-252 | Withdrawn canonical reactor half-angle from the moment law The half-angle π/8 is canonical because T2 = −1. | Earlier T-bridge wording, explicitly retracted in Appendix B p.154; C2-006/C2-060 | Rev29 T-bridge scope correction, carried in Appendix B p.154; forcing pending at s502/A1275 | The half-angle π/8 is therefore motivated by the moment structure and chosen by the readout rulePDF p.154 | LIB2-061 |
| LIB2-253 | Retired structural derivation rating of the CKM phase construction The CKM Dirac-phase construction under F-δ is a “Structural claim with a derivation path” or conditional theorem rather than a coincidence-class numeral. | Rev29 F-δ phase wording, explicitly retired in Rev32.5; Appendix B §B.6 p.154; C2-012/C2-065 | Rev29 row-by-row re-tiering and Rev32.5 retirement of the remaining structural/conditional-theorem wording | It drops to coincidence-class and stays there until G7 is derived. The number is not withdrawn; the rating is.PDF p.59 | LIB2-068 |
| LIB2-254 | Withdrawn universal claim that inequality conditions cannot reduce dimension No positivity- or stability-type refinement can select the target because inequality conditions cannot reduce dimension. | Earlier banked universal cone argument, quoted in Appendix E p.171; C2-121 | F-SEL(c) scoped closure, S287.9–.11, D1220/A1533; Appendix E p.171 | Degenerate systems can lower dimension in principle, so any proposed selector must derive its everywhere-active equality locus independently and clear the circularity bar.PDF p.171 | LIB2-035, LIB2-033 |
| LIB2-255 | Retired use of one operator name for Wick chart and shell reversal A single operator label “W” names the compact/split Wick chart and the shell or grading-orientation reversal. | Pre-separation geometry wording, quoted in Appendix T §2 p.301; nearest candidate C2-089 | A1437, S251 two-W separation; Appendix T Theorem 2.1 and Remark 2.2 | The single label “W ” is retired suite-wide in favour of the pair.PDF p.301 | — |
| LIB2-256 | Superseded nontrivial bundle reading of the signature sheets The two signature sheets are glued as a nontrivial real frame-preserving bundle. | Earlier signature-sheet bundle interpretation, superseded in Appendix T §3, Named datum 3.5, p.302 | A1438/s916, Rev28 geometry fold; Appendix T Theorem 3.4 and Named datum 3.5 | a real-form correspondence, not a nontrivial bundle. The two signature presentations are two real structures in one complexified Albert fibre;PDF p.302 | — |
| LIB2-257 | Retired one-bit accounting of distinct gluing and observation structures Local overlap, global holonomy, real-form correspondence and the physical observation map cost one “W bit”. | Earlier W-bit accounting, explicitly corrected by Appendix T Remark 3.8 p.302 | A1438 geometry/accounting correction, Appendix T §3, Remark 3.8 | Charging these as one “W bit” was a conflation; the row is retired and replaced by the four-structure accounting entry.PDF p.302 | — |
| LIB2-258 | Retired finite-sign chamber-lift price computed on the wrong carrier “D5-representation commutant = 3, hence lift ambiguity = 8 orthogonal / 4 orientation-preserving, zero continuous.” | Earlier house-signed chamber-lift row, quoted by the binding S253 erratum in Appendix T p.308 | A1446/s924-W2/W3, S253 binding erratum; replaced by Appendix T Theorem 9.3 | The finite-sign price row is retired and replaced by the minimal-dilation theorem (Theorem 9.3). “Zero continuous” stands; the discrete residue did not.PDF p.308 | — |
| LIB2-259 | Withdrawn aggregate bit-and-dimension freedom headline The Rev27 freedom headline combined a bit total, a 17-dimensional decomposition and a surplus into an aggregate count. | Rev27-era freedom headline, explicitly withdrawn in Appendix X §1.3 p.340 | A1436; Rev28 typed-freedom correction, carried in Appendix X §1.3 and Appendix Y casualty register | The Rev27-era headline (a bit total plus a dimension count, with a surplus) is withdrawn pending typed rebuild: its 17-dimensional decomposition is internally inconsistent as typed — confirmed at primary source, lane-caught, and logged as a house casualty bel…PDF p.340 | LIB2-005 |
| LIB2-260 | Retired microscopic selector-deriving status of the earlier parent action D1125 supplies a selector-deriving microscopic parent action with “all ten C fixed exactly”. | D1125/A1429 parent-action return, corrected by Appendix S §8.1 p.292 | D1126/A1430, s909; D1125 falsifier #7 and unconditional KILL-NODE 2 disposition | D1125 is killed as a selector-deriving microscopic parent action. It survives as a mathematically consistent loaded finite effective action once TAM , the copy metric and the discrete marking are declared inputs — a demotion of provenance, not an algebraic in…PDF p.292 | — |
| LIB2-261 | Retired independent-channel source doorway The selector’s channel patterns may be chosen independently in the source doorway. | Earlier house independent-channel doorway, identified as casualty #4 in Appendix S §§4,7 | Paired-source correction, S244–S245 arc; Appendix S §4 p.288 and casualty #4 p.291 | The correct source model (correcting the retired house doorway, casualty #4) is a single common selector contrast, not independent channel patterns.PDF p.288 | — |
| LIB2-262 | Withdrawn unconditional action preference for the root line “The action votes for the root line” without an additional common-lift condition. | Earlier selector-arc action-vote statement, identified as casualty #5 in Appendix S §§5,7 | Common-lift-conditional correction, Appendix S §5 p.289 and casualty #5 p.291 | with the relative lift axis ∆θ unpinned, both character types admit nonzero action-critical equivariant points, so the action’s “vote” for the root line is common-lift-conditional only (casualty #5, corrected in place).PDF p.289 | — |
| LIB2-263 | Retired depth-exclusion inference from commuting charge and mass The commutator [M,Qem] = 0 excludes depth sourcing. | Earlier depth-exclusion cut, casualty #7 in Appendix S p.291 and Appendix X p.339 | S244–S245 depth-exclusion correction; Appendix S casualty #7 p.291 | the depth-exclusion cut retired ([M, Qem ] = 0 forbids identifying the two Z4 labels but not depth sourcing).PDF p.291 | — |
| LIB2-264 | Withdrawn claim that the promotion functional was constructed and run The canonical test functional Spromo “is constructed” and its zero set is “house-verified”, without retaining the scalar-tier qualifier. | Rev28 promotion-gate wording, corrected in Appendix X §3.3 p.347 | Rev29 promotion-gate correction, carried in Appendix X §3.3 p.347; AST audit and restored s954:9 qualifier | the functional is specified, not built, and no run of it exists.PDF p.347 | — |
| LIB2-265 | Superseded Wyler-baseline route for the muon mass L116: Muon = Wyler Baseline; P32: Muon = Wyler Baseline (0.141%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, L116 and P32 | not located in suite; current-target replacement by the charged-lepton chain in Paper 2 §3.2, pp.33–34 | mµ follows from the algebraic ratio formula [A616, A618], re-typed Structural / Loaded-correspondence / Reproduced above and not citable as zero-parameter (Rev29 );PDF p.34 | LIB2-122, LIB2-125, LIB2-126 |
| LIB2-266 | Superseded electromagnetic-power Wyler formula for the muon Muon Mass Wyler Formula: m_μ = α^{5/4}·(3/16)^{3/4}·v/√2 [G1 CLOSED] | LIBRARY_V1_GROK_ARCHIVE_S304.md, L259 | not located in suite; current-target replacement in Paper 2 §3.2, pp.33–34 | mµ follows from the algebraic ratio formula [A616, A618], re-typed Structural / Loaded-correspondence / Reproduced above and not citable as zero-parameter (Rev29 );PDF p.34 | LIB2-122, LIB2-125, LIB2-126 |
| LIB2-267 | Superseded sub-Wyler route for the electron mass L117: Electron Sub-Wyler Formula; P33: Electron Sub-Wyler from G₂ Minimal Orbit (0.428%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, L117 and P33 | not located in suite; current-target replacement by Paper 2 §3.2, p.34 | The electron mass is determined by the external empirical relation K = 2/3 acting on that mµ chain and the measured mτ anchor [A636, A637].PDF p.34 | LIB2-127 |
| LIB2-268 | Superseded extended-Wyler route for the tau mass L118: Tau Extended Wyler Formula; P34: Tau from Extended Wyler: 19 = dim(G₂)+dim(Shilov) (0.062%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, L118 and P34 | not located in suite; the current chain uses an external tau anchor, Paper 2 §3.2, pp.33–34 | mτ is the external anchor; mµ follows from the algebraic ratio formula [A616, A618],PDF p.34 | LIB2-124, LIB2-221 |
| LIB2-269 | Superseded Peirce-cylinder proposal for the tau mass Tau Mass from Peirce Cylinder: m_τ = m_μ·R₂₃^{19/√2} [PROPOSED] | LIBRARY_V1_GROK_ARCHIVE_S304.md, L262 | not located in suite; current-target replacement by the external tau anchor in Paper 2 §3.2, pp.33–34 | mτ is the external anchor; mµ follows from the algebraic ratio formula [A616, A618],PDF p.34 | LIB2-124, LIB2-221 |
| LIB2-270 | Superseded D-tower formula for the bottom mass [Group B: Gauge and EW Sector] BOTTOM QUARK MASS — D*phi^{-7} TOWER | LIBRARY_V1_GROK_ARCHIVE_S304.md, L26 | not located in suite; current-target replacement in Paper 2 §3.6, pp.36–37 | The mb row must be quoted with its offset: mb = (7/3)mτ = 4146 MeV against PDG 2026 mb (mb ) = 4186 ± 6 MeV is −0.96% and dcmp = −6.67 (cross-scheme, no status).PDF p.37 | LIB2-130 |
| LIB2-271 | Superseded pi-weighted prefactor formula for the bottom mass L138: Numerical prefactor = sqrt(3)r_23/42 ≈3071.5 MeV exact; m_b = prefactor(π/2)^{2/3} ≈4150 MeV; gap -0.78% | LIBRARY_V1_GROK_ARCHIVE_S304.md, L138 | not located in suite; current-target replacement in Paper 2 §3.6, pp.36–37 | The mb row must be quoted with its offset: mb = (7/3)mτ = 4146 MeV against PDG 2026 mb (mb ) = 4186 ± 6 MeV is −0.96% and dcmp = −6.67 (cross-scheme, no status).PDF p.37 | LIB2-130 |
| LIB2-272 | Superseded cylinder-prefactor proof prompt for the bottom mass P51: m_b Prefactor from J₂₃ Cylinder | LIBRARY_V1_GROK_ARCHIVE_S304.md, P51 | not located in suite; current-target replacement in Paper 2 §3.6, pp.36–37 | The mb row must be quoted with its offset: mb = (7/3)mτ = 4146 MeV against PDG 2026 mb (mb ) = 4186 ± 6 MeV is −0.96% and dcmp = −6.67 (cross-scheme, no status).PDF p.37 | LIB2-130 |
| LIB2-273 | Superseded D-tower formula for the charm mass [Group B: Gauge and EW Sector] CHARM QUARK MASS — D*phi^{-9} TOWER | LIBRARY_V1_GROK_ARCHIVE_S304.md, L27 | not located in suite; current-target replacement in Paper 2 §3.6, pp.36–37 | The charm bridge value mc = 1291.9 MeV lies +1.49% above the PDG 2026 MS comparator mc (mc ) = 1272.9 ± 4.5 MeV.PDF p.37 | LIB2-131 |
| LIB2-274 | Superseded triality log-geometric-mean charm formula Charm Mass from SO(8) Triality P46: m_c = m_μ·(m_t/m_μ)^{1/3}; P46: m_c (Charm) from Triality Log-Geometric Mean — NEW (gap 1.64%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, L132 and its explicitly named P46 | not located in suite; current-target replacement in Paper 2 §3.6, pp.36–37 | The charm bridge value mc = 1291.9 MeV lies +1.49% above the PDG 2026 MS comparator mc (mc ) = 1272.9 ± 4.5 MeV.PDF p.37 | LIB2-131 |
| LIB2-275 | Superseded cubic-to-tower triality bridge for the charm mass P29: Charm Triality Bridge — J₃ Cubic to D-Tower | LIBRARY_V1_GROK_ARCHIVE_S304.md, P29 | not located in suite; current-target replacement in Paper 2 §3.6, pp.36–37 | The charm bridge value mc = 1291.9 MeV lies +1.49% above the PDG 2026 MS comparator mc (mc ) = 1272.9 ± 4.5 MeV.PDF p.37 | LIB2-131 |
| LIB2-276 | Superseded resummed-electromagnetic charm formula P67: m_c = m_t × α/(1−α) — Charm from Resummed EM Coupling (gap 0.044%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, P67 | not located in suite; current-target replacement in Paper 2 §3.6, pp.36–37 | The charm bridge value mc = 1291.9 MeV lies +1.49% above the PDG 2026 MS comparator mc (mc ) = 1272.9 ± 4.5 MeV.PDF p.37 | LIB2-131 |
| LIB2-277 | Superseded early cubic-phase ansatz for the leptonic Dirac phase δ_CP(PMNS) Best Candidate P44: −133.4° [OPEN, 6% gap]; P44: δ_CP(PMNS) from J₃ Cubic Invariant Phase (gap 7.4%); L256 bare-target clause: δ_CP(PMNS) Bare vs Torsion: −133.4° vs PDG −142° [HP9, OPEN] | LIBRARY_V1_GROK_ARCHIVE_S304.md, L130, its named P44, and the bare-target clause of L256 | Paper 7 §7 p.116 explicitly supersedes the old ansatz at Rev29; the exact assessment chain for the archived prompts is not supplied | The old ansatz value −133.36◦ is superseded.PDF p.116 | LIB2-062 |
| LIB2-278 | Superseded imaginary-correction prompt for the leptonic phase L135: Numerical imag corr to δ_CP = β_δ * sin(φ * π/4) ≈ {degrees value}; adjusted δ_CP = tree + corr ≈ -142°; gap {calculated %} | LIBRARY_V1_GROK_ARCHIVE_S304.md, L135 | not located in suite; current-target replacement by the conditional phase readout in Paper 5 §3 p.84 | δCP = −2π/ 5 = −160.997◦PDF p.84 | LIB2-062 |
| LIB2-279 | Superseded determinant-imaginary-part route for the full leptonic phase P48: Full δ_CP(PMNS) from Im(Det(J₃)) — Extended P44 | LIBRARY_V1_GROK_ARCHIVE_S304.md, P48 | not located in suite; current-target replacement by the conditional phase readout in Paper 5 §3 p.84 | δCP = −2π/ 5 = −160.997◦PDF p.84 | LIB2-062 |
| LIB2-280 | Superseded sum-rule and torsion-corrected reactor route to the leptonic phase P66: δ_CP via P50 Sum Rule + Torsion-Corrected θ₁₃ (gap 0.051%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, P66 | not located in suite; current-target replacement by the conditional phase readout in Paper 5 §3 p.84 | δCP = −2π/ 5 = −160.997◦PDF p.84 | LIB2-062 |
| LIB2-281 | Superseded cylinder formula for the reactor angle θ₁₃(PMNS) from J₁₂ Cylinder P45: arctan(α^{1/3}/√φ); P45: θ₁₃(PMNS) from J₁₂ Cylinder Mixing — NEW (gap 1.17%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, L133 and its explicitly named P45 | not located in suite; current-target replacement in Paper 5, p.79 | sin2 θ13 = sin4 (π/8)PDF p.79 | LIB2-061 |
| LIB2-282 | Superseded torsion-corrected cylinder formula for the reactor angle P65: θ₁₃(PMNS) = arctan(α^{1/3}/√φ) − δ_torsion — EXACT (gap 0.000%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, P65 | not located in suite; current-target replacement in Paper 5, p.79 | sin2 θ13 = sin4 (π/8)PDF p.79 | LIB2-061 |
| LIB2-283 | Superseded torsion-corrected PMNS angle scheme PMNS Torsion-Corrected Angles: QLC + Shilov + G₂(2) [HP9, PROPOSED] | LIBRARY_V1_GROK_ARCHIVE_S304.md, L254 | not located in suite; current-target replacement in Paper 5, p.79 | current: θ12 , δCP Derived-conditional, the physical θ23 octant Loaded-correspondence — A1566PDF p.79 | LIB2-060, LIB2-002, LIB2-061 |
| LIB2-284 | Superseded Shilov-circle correction prompt for the atmospheric angle P40: θ₂₃(PMNS) Shilov Circle Correction (0.032%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, P40 | not located in suite; current-target replacement in Paper 7, p.116 | The current framework value is the mismatch-geometry branch sin2 θ23 = 7/16, rather than the older higher-octant phenomenological placeholderPDF p.116 | LIB2-002 |
| LIB2-285 | Superseded Peirce golden-power assignment for two CKM magnitudes CKM Elements from Peirce J₂₃: V_cb = λ²/φ, V_ub = λ³/φ [OPEN] | LIBRARY_V1_GROK_ARCHIVE_S304.md, L129 | not located in suite; current-target replacement in Appendix B, p.156 | first row Loaded, |Vcb | Loaded-correspondence attach- ment (physical) / Structural formulaPDF p.156 | LIB2-066, LIB2-067 |
| LIB2-286 | Superseded additive correction prompt for Vcb L137: Numerical corr = (1/(2π)) * β_δ ≈0.009; adjusted V_cb ≈0.0405; gap -1.2% | LIBRARY_V1_GROK_ARCHIVE_S304.md, L137 | not located in suite; current-target replacement in Appendix B, p.156 | |Vcb | 1/(9 7) = 0.041996PDF p.156 | LIB2-066 |
| LIB2-287 | Superseded golden-power ratio of CKM hierarchy magnitudes L282 ratio clause: |V_ub/V_cb| = φ⁻⁵; |V_ub/V_cb| = φ⁻⁵ from R_b · sin θ_C Peirce Suppression | LIBRARY_V1_GROK_ARCHIVE_S304.md, L282 ratio clause and L294 | not located in suite; current-target replacement in Appendix B, p.156 | |Vub | |Vus ||Vcb |/ 6 = 0.003862PDF p.156 | LIB2-067 |
| LIB2-288 | Superseded Cabibbo-squared formula for Vcb P68: V_cb = sin²(θ_C)/√φ with Corrected θ_C (gap 0.28%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, P68 | not located in suite; current-target replacement in Appendix B, p.156 | |Vcb | 1/(9 7) = 0.041996PDF p.156 | LIB2-066 |
| LIB2-289 | Superseded reciprocal weak-angle proposal Weinberg Angle: sin²θ_W = 1/(2+φ) [OPEN, +19.5% gap] | LIBRARY_V1_GROK_ARCHIVE_S304.md, L127 | not located in suite; current-target replacement in Paper 4, p.73 | We therefore carry ϕ−3 as a ∼ 2% structural tree-level target on the electroweak curve, not as a completed Z-pole precision prediction.PDF p.73 | LIB2-199, LIB2-200 |
| LIB2-290 | Superseded logarithmic loop-correction prompt for the weak angle L134: Numerical 1-loop Δsin²θ_W = - (α / (4π)) * log(r₁₃ / v) ≈ {calculated value}; adjusted sin²θ_W = tree + Δ ≈ 0.231; gap to PDG {calculated %} | LIBRARY_V1_GROK_ARCHIVE_S304.md, L134 | not located in suite; current-target replacement in Paper 4, p.73 | We therefore carry ϕ−3 as a ∼ 2% structural tree-level target on the electroweak curve, not as a completed Z-pole precision prediction.PDF p.73 | LIB2-199 |
| LIB2-291 | Superseded cylinder-running proof prompt for the weak angle P47: 1-loop sin²θ_W from J₁₃ Peirce Cylinder Running | LIBRARY_V1_GROK_ARCHIVE_S304.md, P47 | not located in suite; current-target replacement in Paper 4, p.73 | We therefore carry ϕ−3 as a ∼ 2% structural tree-level target on the electroweak curve, not as a completed Z-pole precision prediction.PDF p.73 | LIB2-199 |
| LIB2-292 | Superseded electromagnetic-subtraction formula for the weak angle P70: sin²θ_W = 1/φ³ − 2α/π — One-Loop EM Correction (gap 0.088%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, P70 | not located in suite; current-target replacement in Paper 4, p.73 | We therefore carry ϕ−3 as a ∼ 2% structural tree-level target on the electroweak curve, not as a completed Z-pole precision prediction.PDF p.73 | LIB2-199, LIB2-200 |
| LIB2-293 | Superseded QLC-plus-cylinder correction for the Cabibbo angle L136: Numerical Δθ_C = arctan(α^{1/3} / (r₁₂ / v)) ≈ {degrees}; adjusted θ_C = QLC + Δ ≈ 13.04°; gap {calculated %} | LIBRARY_V1_GROK_ARCHIVE_S304.md, L136 | not located in suite; current-target replacement in Paper 3, p.47 | current value is |Vus | = 0.225256 (the exact framework angle arctan( 3/ϕ2 ) = 33.4880◦ , printed from the kernel line s1162;PDF p.47 | LIB2-063 |
| LIB2-294 | Superseded torsion-corrected Cabibbo–Weinberg formula P64: θ_C = arctan(1/φ³) − δ_torsion — Cabibbo = arctan(Weinberg) (gap 1.09%) | LIBRARY_V1_GROK_ARCHIVE_S304.md, P64 | not located in suite; current-target replacement in Paper 3, p.47 | current value is |Vus | = 0.225256 (the exact framework angle arctan( 3/ϕ2 ) = 33.4880◦ , printed from the kernel line s1162;PDF p.47 | LIB2-063, LIB2-199 |
| LIB2-295 | Superseded Cabibbo–Weinberg residual identity as a physical target P73: Cabibbo-Weinberg Residual Identity: tan(θ_C)−sin²θ_W = α/(2π²) | LIBRARY_V1_GROK_ARCHIVE_S304.md, P73 | not located in suite; current-target replacement in Paper 3, p.47 | current value is |Vus | = 0.225256 (the exact framework angle arctan( 3/ϕ2 ) = 33.4880◦ , printed from the kernel line s1162;PDF p.47 | LIB2-063, LIB2-199 |
| LIB2-296 | Superseded singular-vacuum premise of the protection-and-bounce chain Det(J_vac) = 0 ↔ λ₃ = 0 ↔ M_Z Protection ↔ Bounce | LIBRARY_V1_GROK_ARCHIVE_S304.md, L278; legacy vacuum normalization discussed in Appendix I §6 | Explicit normalization supersession in Appendix I §6, Remark 6.4, p.209; current unit-determinant premise at Appendix E §1 p.163; exact legacy assessment chain not supplied | the legacy vacuum normalization diag(ϕ2 , 1, 0) is superseded by the current {ϕ, 1, ϕ−1 } frame, the structural statements unaffected.PDF p.209 | LIB2-047 |
| LIB2-297 | Retired compact-colour subgroup claim in the split-G2 real form P28: SU(3)_color as Maximal Subgroup of G₂(2) — Branching Rules | LIBRARY_V1_GROK_ARCHIVE_S304.md, P28 | Appendix N Part N.B, Proposition 2.1, s253, states the opposite inclusion obstruction; exact P28 retirement chronology not located in suite | The compact colour algebra su(3) (dimension 8) cannot embed in the compact part available to the loaded subimage, whose maximal compact dimension is 6 < 8.PDF p.253 | LIB2-096 |
| LIB2-298 | Withdrawn physical-generation implication of the triality carrier cycle SO(8) Triality τ: 8_v → 8_s → 8_c Generation Mechanism | LIBRARY_V1_GROK_ARCHIVE_S304.md, L280 | A691/A693 generation-replication exclusions, Paper 0 p.17; current discrete-branch scope at Rev32.3; exact L280 retirement chain not supplied | algebraic replication of three generations inside a single J3 (Os ) is excluded: three families need 3 × 16 = 48 fermionic dimensions, which do not fit in the 27 (8+8+8 = 24 off-diagonal, and triality maps 8+ → 8− → 8v , so the blocks are not three gauge-iden…PDF p.17 | — |
| LIB2-345 | Superseded use of the first JUNO oscillation comparison L-JUNOv1 — JUNO First Oscillation Result; STATUS: EXPERIMENTAL (first precision measurement); Comparison with Our Predictions; Tension with JUNO: (0.3185 − 0.3092)/0.0087 ≈ 1.07σ | C2-161, L-JUNOv1_first_oscillation_result.md; supplied S173 supersession flag | S173 SUPERSEDED flag in C2-161; the precise retiring passage is not located in suite; current benchmark stated in Paper 5 p.79 | The paper therefore keeps the structure simple: the angle set, the phase formula, the current comparison to NuFIT 6.1, and the DUNE-era test scenario.PDF p.79 | LIB2-003, LIB2-204, LIB2-205, LIB2-206, LIB2-226, LIB2-227, LIB2-228 |
Machine surface: library_v2.jsonl (filter class == "RETIRED"); the hub H09 · Retired statements lists the same records.
| release | suite | engine workbooks (sha256 prefix) | status |
|---|---|---|---|
| Rev33.1 / S369 | 433 pp | Machine 32875b1696a2 · Outputs 4e6e7c32b307 | current — the suite of record |
| Rev33.0 / S364 | 429 pp | Machine b47f7bc9db75 · Outputs a67bb0ebddb4 | superseded by Rev33.1 |
| Rev32.11 / S348 | 412 pp | Machine 9ab03a2efac2 · Outputs 337d899aad01 | superseded by Rev33.0 · zip re-issued S364 (R180: ledger lines withheld on export; tex, PDF and engine unchanged) — erratum: its engine workbook (Machine 9ab03a2efac2) recalculates to 25 of 27 checks PASS — RCI rows 22 and 24 fail behind stale cached PASS values (measured S363, re-derived at application S364) |
| Rev32.10 / S344 | 411 pp | Machine 650634658022 · Outputs acd9a7f14da4 | superseded by Rev32.11 · zip re-issued S364 (R180: ledger lines withheld on export; tex, PDF and engine unchanged) |
| Rev32.9 / S341 | 410 pp | Machine 6d489626b664 · Outputs 26377c02e619 | superseded by Rev32.10 · zip re-issued S364 (R180: ledger lines withheld on export; tex, PDF and engine unchanged) |
| Rev32.8 / S339 | 385 pp | Machine 7b09e1a2780b · Outputs 81d3ba688401 | superseded by Rev32.9 · zip re-issued S364 (R180: ledger lines withheld on export; tex, PDF and engine unchanged) |
| Rev32.7 / S303 | 385 pp | Machine 7b09e1a2780b · Outputs 81d3ba688401 | superseded by Rev32.8 · zip re-issued S364 (R180: ledger lines withheld on export; tex, PDF and engine unchanged) |
| Rev32.6 / S303 | 385 pp | Machine 7b09e1a2780b · Outputs 81d3ba688401 | superseded by Rev32.7 (same day) · zip re-issued S364 (R180: ledger lines withheld on export; tex, PDF and engine unchanged) |
| Rev32.5 / S300 | 380 pp | Machine 698a74c0880f · Outputs 3ffa68692c3a | superseded by Rev32.6 · zip re-issued S364 (R180: ledger lines withheld on export; tex, PDF and engine unchanged) |
| Rev32.4 / S300 | 374 pp | Machine 698a74c0880f · Outputs 3ffa68692c3a | superseded by Rev32.5 (same day) |
| Rev32.3 / S300 | 374 pp | Machine f58b326dfdfa · Outputs 351cfeaf496e | superseded by Rev32.4 (same day) |
| Rev32.2 / S300 | 374 pp | Machine f58b326dfdfa · Outputs 351cfeaf496e | superseded by Rev32.3 (same day) |
| Rev32.1 / S290 | 367 pp | Machine f58b326dfdfa · Outputs 351cfeaf496e | superseded by Rev32.2 |
| Rev32 / S288 | 363 pp | Machine f58b326dfdfa · Outputs 351cfeaf496e | superseded by Rev32.1 |
| Rev31.2 / S280 | 354 pp | Machine f58b326dfdfa · Outputs 351cfeaf496e | superseded by Rev32 |
| Rev31.1 / S280 | 354 pp | Machine f58b326dfdfa · Outputs 351cfeaf496e | superseded by Rev31.2 |
| Rev31 / S279 | 353 pp | Machine f58b326dfdfa · Outputs 351cfeaf496e | superseded by Rev31.1 |
| Rev30 / S273 | 344 pp | Machine 66c7a549bbaa · Outputs 8fcd0a2f7dae | superseded by Rev31 |
| Rev29 / S263 | 319 pp | Machine 66c7a549bbaa · Outputs 8fcd0a2f7dae | superseded by Rev30 |
| Rev28 / S254 | 280 pp | Machine 66c7a549bbaa · Outputs 8fcd0a2f7dae | superseded by Rev29 |
| Rev25 / S227 | 222 pp | Machine 66c7a549bbaa · Outputs 8fcd0a2f7dae | superseded by Rev28 |
| Rev23 / S193 | 202 pp | Machine 727b0bf0 · Outputs 7f3bc6f92b74 | superseded by Rev25 |
| Rev22 / S176 | 192 pp | Machine 727b0bf0 · Outputs ba333241316a | superseded by Rev23 |
| Rev21 / S174 | 189 pp | Machine 727b0bf0 · Outputs ba333241316a | superseded by Rev22 |
| Rev20.3 / S159b | 178 pp | Machine 727b0bf0 · Outputs ede9aecc86b9 | superseded by Rev21 |
| Rev20 / S159 | 177 pp | Machine 727b0bf0 · Outputs 68b0256a | superseded by Rev20.3 |
| Rev19.1 / S136b | 160 pp | 727b0bf0 | superseded |
| Rev18 / S127 | 160 pp | 437ce51b | superseded |
| Rev18 / S126 | 160 pp | 1fc4757e | superseded |
| Rev17 / S119 | — | 1fc4757e | superseded |
| Rev16 / S117 | — | 56737bad→1fc4757e | superseded |
| Rev16 / S116 | — | 56737bad | superseded |
Source: the release index kept beside the frozen bundles; rows are printed as recorded there, oldest at the foot.