TFPT scientific source excerpt Original repository path: experiments/theory-contracts/original-paper-source-reconciliation-20261102/shorttime_20261105J/shorttime20261105J_verification/VERIFICATION-WOLFRAM-SOURCE-PRODUCER-REVIEW-20261105.txt Original file SHA-256: 25f3d801ed156d71f2f3a6f5a15e3ebcb4431496ed2f50c2af57243ae7cba8f1 Inclusive original lines: 1-60 Line numbers below refer to the original source. This bounded excerpt is source evidence; it is not a new proof/checker run. Conversation metadata and personal execution details are omitted where indicated. 000001 | Verification and Wolfram: actual source producers and the missing I value 000002 | 2026-11-05. Readonly canonical review; scratch only. 000003 | Requested target: evaluate the original common open OS source, especially I_orig[u], I_orig[UY], K_U and its whole body; recover old genuinely completed source relations before introducing any new model. 000004 | 000005 | Result 000006 | The targeted producer review found genuine complete old closures in their original classes, but no reviewed producer supplies the remaining dynamical H/g integral. This is a source specific result, not a claim of global nonexistence. The existing whole U, state, time, reference and selector maps remain retained. No old P1 gate is reopened. 000007 | The useful recovered closures are (i) full finite CAR KMS rigidity, (ii) exact finite transfer and anchor moment recurrences, and (iii) the infinite affine PBW vacuum engine. They remove redundant work once their actual operator/state hypotheses match. None of these reviewed implementations calls the original dynamical H/g source. 000008 | 000009 | A. Actual code, inputs, outputs and type checks 000010 | 000011 | 1. verification/v995_kms_subnet_rigidity.py:40-69,100-149 000012 | exact_partition_function() returns product_j(1+Q^j), j=1..8, Q=(2/3)^6. run() enumerates all 256 CAR8 Fock basis states with weights Q^(sum_j j n_j)/Z and exact occupations Q^j/(1+Q^j). The original finite KMS equations remove all 33 tested mixing directions; full matrix KMS fixes the state once this Hamiltonian is supplied. This is an actual full finite density, not just a name. 000013 | It does not take dynamical H/g endpoints, a proper time profile nu, the full 96 dimensional Yukawa/MR operator, or a physical OS strip as input. Eight complex modes are not eight folded source arcs or eight ordered letters. The fixed exponent vector 1..8 is an explicit input to this producer. Tensoring with an actual bosonic source would preserve the missing bosonic state, rather than evaluate it. 000014 | No fresh finite KMS run was performed: it would not test the missing common source value. 000015 | 000016 | 2. verification/v1005_relative_pencil_bridges.py:237-331 000017 | claim_2_anchor_moments() starts from the actual anchor (1,1,2), evaluates p_n=2+2^n and reconstructs exactly the measure 2 delta_1+delta_2. It derives the Jacobi matrix [[4/3,sqrt(2)/3],[sqrt(2)/3,5/3]], the symbolic Hankel law p_n p_(n+2)-p_(n+1)^2=2^(n+1), vanishing shifted 3x3 determinants, and p_(n+2)=3p_(n+1)-2p_n. This is a genuine full moment closure for the anchor spectral measure. 000018 | Its variable is the anchor eigenvalue, not Higgs u=|H|^2. Its moments are power moments of a two atom measure, not OS time moments. No equality with the u source is present in the function. 000019 | 000020 | 3. verification/v171_os_moment_cluster.py:46ff and v971_markov_embedding_generator.py:61-70 000021 | The actual boundary transfer T=J+(64/729)P2+(1/729)P3 and all three projectors are explicit. v171 uses C_n=A+B(64/729)^n+C(1/729)^n. Its test sets A=B=C=1 with the explicit comment that any nonnegative A,B,C are allowed. It does not derive the observable dependent weights for U. 000022 | Exact consequence, useful only for an actually matched reducing three spectrum sector: 000023 | K_(n+3)=(794/729)K_(n+2)-(47449/531441)K_(n+1)+(64/531441)K_n. 000024 | For the connected two spectrum part: 000025 | C_(n+2)=(65/729)C_(n+1)-(64/531441)C_n. 000026 | Thus a correctly matched K_U could be determined by three actual initial values. The spectrum alone supplies neither those values nor the statement that U's spectral support is confined to this sector. This is a conditional finite recurrence shortcut, not a new whole source evaluation. 000027 | 000028 | 4. verification/v500_celestial_wp5c_gns_limit_state.py:652-685 000029 | This is the actual infinite source candidate, rather than another finite KMS matrix. gram_entry(eng,th,ukey,vkey) evaluates by applying the theta adjoints through eng.act and selecting the vacuum coefficient. pair_states and block_gram extend it linearly and construct exact rational Gram matrices. The supplied algebra is affine E8 at k=1, with the PBW engine and vacuum relations; the radial family has pairings x^(wr), loop sector the affine vacuum. Level two rank4124 and kernel27000 are actual old computations. The full extension is typed by the named affine positivity facts; local normality and further continuum conclusions are separately scoped in the original header. 000030 | No dynamic Higgs operator or full 96 dimensional MR field source is consumed by this engine. The current parameter x is a Gibbs/formal grading variable, not the original physical proper time profile nu. The common original maps must not be replaced by this affine state merely because an infinite state is available. No whole H/g integral is thereby recovered. 000031 | 000032 | 5. verification/v520_celestial_wp5e_measure_decision.py:1002-1016 000033 | run_integral(beta,ws,V4,V2,CNT,weight) really evaluates Harvey-Moore modular integrals using prescribed Weil/Theta and dressing data and compares two grid cuts. The measure decision is conditional on TP1..4, and the header retains the normalization of w_m itself as open. This is a modular one loop factor, not the original common Higgs and geometry configuration distribution. The Wolfram mirror verifies the invariant algebra, characters, pairing and levelwise moment identities; numerical modular integration remains Python only. 000034 | 000035 | B. Tempting shortcuts already excluded by their actual owning source 000036 | 000037 | v160_seam_gaussianity_from_pf.py: the proposed promotion from the three dimensional Perron gap to Wick factorization on the full OS Schwinger cone is explicitly marked conditional. Its exact Pfaffian identities consume quasi-free data. They do not generate whole interacting H/g cumulants. 000038 | v147_clock_gaussian.py:53ff: exact Gaussian zero mode partition ratio (1-alpha)^(p2/2) and clock ring sum, but the original header and final check keep the gravitational measure identification as [P]. This is not a forgotten primitive integral. 000039 | v1009_rho0_minimizer.py:49-64: expectation(rho,operator) consumes the density; density_from_hamiltonian(H,beta) normalizes exp(-beta H). The declared finite 96 dimensional 1+1D model uses sites2, linkdim6, fermion modes4 and specific couplings. Its own projector constraints kill the tested SK response. It is not the full 96 component internal MR Higgs operator merely because both use 96. 000040 | v1003_nu_structural_nulls.py:407-410: effective_kernel(candidate,eta) computes a finite seesaw Schur complement for declared matrices. Here nu means neutrino, not the proper time measure. Both structural and scale nulls are retained by its original source. 000041 | v584_ext_source_response.py: the actual rational rank one Gibbs pencil and flip thresholds belong to the declared Ext trace pairing platform. It does not become an OS measure; the original code explicitly keeps that distinction. 000042 | v166_higgs_free_seam.py:85-96: _run(lam0,yt0,Lambda,n) integrates the two loop SM RG equations using measured boundary couplings and V_EW. It predicts/test couplings under free seam boundary conditions, not omega(u). 000043 | v269/v271: the real Epstein-Glaser calculations are formal perturbative S_pert and one loop renormalization data. v271 explicitly says no path integral. They do not compute a nonperturbative vacuum distribution. 000044 | v398 and v311: finite transfer/character commutation, clustering and gap margins are actual scoped calculations; those functions do not integrate a new Higgs configuration variable. Parent separately owns the newer ambient no dependency argument, which this report does not reopen. 000045 | 000046 | C. Smallest decisive comparison for a false finite whole source closure 000047 | 000048 | For the already scoped whole local residue branch with matched Higgs coordinate field and fixed/block diagonal geometry, the original kinetic coefficient gives 000049 | [u,[H_joint,u]]=32 pi^2 (N/V) u, 000050 | where u>=0 and N/V>0. On an entire closed finite Hilbert space, Tr[u,[H,u]]=0 by cyclicity, while the stated right hand side has strictly positive trace when u is nonzero. Therefore no nontrivial finite anchor/KMS whole algebra can exactly represent that whole local Higgs dynamics. 000051 | This test does not exclude finite matrix elements cut out of an infinite source: retained returns make P[u,[H,u]]P different from [PuP,[PHP,PuP]]. It does not exclude a finite spectral measure for one particular U Omega, nor nonlocal profile branches. It uses no newly selected model or measure. 000052 | Hence the productive use of the recovered exact finite closures is as target sector identities and evaluations after the actual operator map, not as a replacement for the original dynamical bosonic factor. The infinite PBW candidate avoids the finite trace obstruction but still does not evaluate the actual common H/g caller. 000053 | 000054 | D. Coverage and continuation 000055 | 000056 | This was targeted original source review, not a fresh whole suite run. The prior 2026-10-29 verification recovery inventory already screened 3108 source files and directly reviewed 24 strong Python closure candidates. Its historical open map statements are superseded where the current original U/state/time/reference maps have since been closed. Its ground state source reduction and full projector state rigidity remain actual reusable closure theorems; no extra Gaussian choice is required when their same representation hypotheses hold. 000057 | The present review reads concrete producer bodies and preserves source types. No candidate passing the actual common source type check was found to execute. Reexecuting its finite substitute would not answer the requested I value. 000058 | The best current continuation is the parent/route3 construction of an exact untruncated cubic+quartic R048 regulated reweighting producer with a controlled integration remainder. That route evaluates the actual supplied interaction rather than selecting a new finite state. The original source weight, reference, eta, contour and whole operator inputs remain inside it; no full closure is claimed here. 000059 | 000060 | Evidence: original-producer-source-evidence.json records exact current files, hashes and function arguments/line positions for the 16 targeted Python sources. No canonical/Atlas/paper/website edit. No new physical profile, measure, fixed H model, or numerical common source value was introduced.