No complete concrete Finsupp kernel instantiation, physical state selection or automatic K-invariance of the bare shift algebra.
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Result
E0(y*y)=a0*a0+phi^-1(a1*a1) proves positivity of omega0 o E0. General algebra/star/positivity and dual uniqueness theorems are Lean-checked; concrete finite-lattice transfer is analytically proved.
Required assumptions
Fixed CAR source and adjoined half sector
Ordered eight-channel cocycle, s=(1/2)^8, Q, quarter phase and K_alpha=N+|p|²/2+delta_alpha.p are supplied; alpha=1/4,3/4. Parity equivalence is in the global operator envelope without a separately marked physical X. Neither source nor extension is derived from P1/P2.
Positive base functional and explicit observable algebra
For finite crossed words omega0 is positive; dual Z2 invariance is additionally required for unique algebraic extension. Comparing physical densities must retain the actual Cartan observables and the common normal ground space of supplied K.
Global crossed operators; no local field equivalence or physical selection.
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Result
262144 candidates on two H200: four universally Lean-checked presentations. X_plus=Pi X_minus preserves source,Q,K,quarter marker and canonical state; two marked P classes remain. Full T1 and Ward are checked. Graded C lifts realize both P signs; scalar X covariance does not follow from the integer endpoint.
Required assumptions
Fixed CAR source and adjoined half sector
Ordered eight-channel cocycle, s=(1/2)^8, Q, quarter phase and K_alpha=N+|p|²/2+delta_alpha.p are supplied; alpha=1/4,3/4. Parity equivalence is in the global operator envelope without a separately marked physical X. Neither source nor extension is derived from P1/P2.
Balanced W remain within the sector; T insertion/removal responses require Cp. No derived physical measuring instrument.
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Result
η·Qtot is zero on C0. T_p enters Cp; full propagation yields ratio exp(−2tη·p). For v=Bp, conditionally η=Bᵀδ. Only the odd factor is matched.
Required assumptions
Full original charge-field source
Finite Round20 lattice/scalar space with the original bilinear E8 cocycle, complete integer charges, onsite T and balanced W, coercive quadratic Hdiag and supplied hopping. No P1/P2 selection or local chiral field identification is presumed.
Chemical comparison with charged intermediate sectors
Additionally supplied Hη=H+η·Qtot, C-invariant initial density in C0 and full propagation after onsite T moves C0 into Cp. η is comparison input, not a derived seam parameter.
Unchanged finite source and specified invariant start; different states or operator dictionaries are not excluded.
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Result
Original C T_p C=T_−p, T_p*=(-1)^e(p)T_−p and C H C=H. At an invariant start all C-conjugate bounded words agree.
Required assumptions
Full original charge-field source
Finite Round20 lattice/scalar space with the original bilinear E8 cocycle, complete integer charges, onsite T and balanced W, coercive quadratic Hdiag and supplied hopping. No P1/P2 selection or local chiral field identification is presumed.
Charge-conjugation-invariant start
The initial density is invariant under linear C:n→−n, including full and C0 Gibbs starts of unchanged H. Compare actual adjoint-paired, opposite marked T responses at the same time.
Known preparation/time normalization in the given E8 Fock space; identifies δ, not q,τ, physical instruments or P1/P2 source selection. Eight directions require their respective ± responses.
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Result
Cδ(p,t)=exp[−t(|p|²/2+δ·p)]. With yi=−log[Cδ(bi,t)/Cδ(−bi,t)]/(2t), y=Bᵀδ and δ=(Bᵀ)⁻¹y. Eight independent directions suffice and are necessary for unrestricted δ in this linear data class.
Required assumptions
Normalized charged primary responses with known time scale
For the given Kδ, normalized primary charge states ±bi for eight independent original E8 basis charges and their positive e^(−tKδ) return amplitudes at known common t>0 are supplied. Global charge shifts are not thereby derived local physical instruments.
Individually all-Cartan-neutral insertions and fixed vacuum; not charged intermediate fields, charged Gibbs traces or δ-dependent probe operators.
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Result
Each admissible intermediate insertion stays in M(1)⊗|0>. There Kδ=N,Qq=0,tτ=I. All ordered vacuum multitime and Gram responses in this class are therefore identical at arbitrary word length, even with complete36-dimensional quadratic tomography.
Required assumptions
Every insertion preserves all eight Cartan charges
In the same given E8 Fock space every word starts in the vacuum. Each individual insertion belongs to the fixed Heisenberg/quadratic Jordan OPE algebra and commutes with all eight Cartan zero modes; normal ordering, operator labels and initial state do not change with δ. Overall neutrality or Qq neutrality alone is insufficient.
Given E8 completion; no physical sectors, switching rates or local instruments selected from P1/P2. As a torus operator τ is identifiable only modulo the dual lattice.
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Result
The original cocycle admits a unitary lift UJ with UJ⁴=I. It intertwines Kδ,Qq and the full quarter transition with KJδ,QJq,tJτ on the entire stipulated Fock space. The four frames are a covariant family; q must be transported.
Required assumptions
Stipulated E8 Fock space with marked clock tuple
Given the original ordered CAR/E8 cocycle, E8 Fock representation, Kδ(p,N)=|p|²/2+δ·p+N, original q and full uncompensated quarter transition. J is the actual Gaussian lattice operator, not the cyclotomic Galois operator. A covariant comparison transports δ,q,τ together; a fixed marked source holds them fixed.
Complete matrix reconstruction in the specified neutral quadratic vacuum sector; neither four measurements nor all charged, state or multitime responses of a physical source.
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Result
P5, CPCᵀ, JPJᵀ and C²P(C²)ᵀ generate all36 real-symmetric8x8 matrices through Jordan words up to degree4. The double-pole OPE realizes these products. An explicit rational inverse reconstructs A from36 mixed responses Tr(BℓA)/2; prescribed trace leaves35 directions.
Required assumptions
Native clock fields and mixed OPE access
Fixed free eight-current vacuum, original C/J/P5 in the same E8 index basis and real-symmetric quadratic fields; access to mixed two-point responses of iterated weight-two double-pole OPE coefficients is assumed. Four individual measurements or a physical detector from P1/P2 are not thereby supplied.
Source provenance and exact algebra under each stated normalization, carrier, primitive sector and defect response contract. No general nonderivability theorem, no retraction of the canonical circle defect line, marked D5 response or positive root uniqueness. No new physical selector or ledger promotion. Historical linear, exponential, quadratic and resummed openings are different calculation contracts; similar coefficients do not prove identical physical actions.
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Result
Older originals give explicit factor provenance: V1.06 uses g=n/(8pi²), n=1 and g=8c3². ImprovedCubic of18September2025 gives linear backreaction1-2alpha; v2.7 derives exp(-alpha J) under additive defect coupling with J=d SF=2. In the later carrier gamma=tr_EY²=3/9+2/4=5/6 and B=rankE3/rankE2=3/2, so B gamma=5/4; family trace tr(S+)Y²=10/3 gives b1=41/10 for three families and one Higgs. The rank-one determinant yields (1-q)^(-5/4); its response q+(5/4)q²+(45/32)q³+... embeds the earlier two-defect coefficient in a fixed series. These factors must not be dismissed collectively as unexplained fits. Full identification remains narrower: v2.7 declares the CFE potential coefficients as supplied scheme inputs; v4.2 supplies P_loc'=alpha³-2c3³alpha² as a condition and defines Gamma by integrating the desired response. The master proof identifies its U(1) block with the already-defined EM action; it does not evaluate an original coupled Dirac determinant to obtain that F there.
Required assumptions
P1/P2 remain declared starting axioms
This program checks which additional source, state, event, and observable structures follow from accepted TFPT principles; it does not revoke or replace P1/P2.
Model results remain conditional
Calculations in a fixed E8 net, quotient, family packet, or readout apply only under their stated inputs and do not select those inputs.
Source-reviewed status/type correction, not a new general nonderivability theorem or gate. P1/P2 remain accepted starting principles; being axioms is not an objection. The line is derived on the old circle, not an arbitrary vector to select again. v382 replay26October:6/6; literalTrue status checks do not prove open functional origin. Ledger Numerical and full physical status remain unchanged.
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Result
Coefficient identities and the unique alpha root are retained. The old circle canonically supplies Pi and det_F(1-qPi)=1-q; for trace-class C-P the same relative factor survives exactly in every faithful KMS polarization class on that same circle. Actual full positive projection covariance fixes the whole CAR state without an extra Gaussian premise. The finite Quillen chain is beyond its older open summary: v985 resolves the finite mu4 channel swap; v995 closes finite KMS rigidity and state extension; v1014 checks the finite determinant-line restriction isomorphism and records reference A0. Do not reopen those steps. What remains is the original local EM source/operator map and relative real renormalized determinant norm producing the seam factor with response exponent5/4, coupling q(alpha), local variation terms and normalization in the same channel. Abstract continuum/Bismut-Freed identification and matching to the physical Thomson coupling do not follow from finite calculations. Chiral phase cancellation does not refute real EM susceptibility. EM.WARD.01 and ALPHA.QUILLEN.EXACT.01 retain their existing physical residual.
Required assumptions
Specified EM function with positive seam response
F(x)=x³−2c³x²+(4/5)c⁶M log(p+q(1−q)^(−5/4)), c=1/(8π), p=1/(6π), q=48c⁴exp(−2x), M>0; original budget M=41. The function and inputs are premises here.
Model results remain conditional
Calculations in a fixed E8 net, quotient, family packet, or readout apply only under their stated inputs and do not select those inputs.
P1/P2 remain declared starting axioms
This program checks which additional source, state, event, and observable structures follow from accepted TFPT principles; it does not revoke or replace P1/P2.
Same original circle with trace-class changed polarization
For the mathematical continuation retain H,B_a psi_n=(n+a)psi_n,0<a<1,u psi_n=psi_(n+1),P=1_(B_a<0),uPu*=P+Pi. C is a positive contraction with trace-class C-P; actual functional-calculus C_beta=(I+exp(beta B_a))^-1,beta>0 belongs to this class. Physical KMS/OS/EM source identification is not presumed.
Test a positive joint CAR source against the full geometric projection
Consider an arbitrary normalized positive state on the specified joint charged two-face CAR algebra,without assuming quasifreeness or U1 invariance. The geometric target is the existing closed chiral annulus graph P_A with both marked faces,W=1/2 and original NS B_Sigma. Actual identity C_source=P_A is an explicit condition of the uniqueness theorem and an unresolved P1 source equation,not a fact inferred from geometry or RP. A finite error test applies only on a genuinely P_A reducing CAR block. Complete Dirac vector source,OS Padm and physical time are not identified with this chiral scalar target. No freely chosen purification supplies missing physical cross correlations.
Do not identify source types
Observable algebra, OS reflection, state, collar operator, time evolution, carrier connection, family holonomy, and readout are distinct data until an original map relates them.
Exact response in the specified existing source, not a new field or fitted exponent. Does not derive physical preparation, u=48c3^4, q=exp(-2alpha), outer uq, baseline1/(6pi), or original EM instrument. Common time is not sector-resolved D5 readout. Replay26October2026:21/21; finite coefficient checks through degree12 do not replace the general series proof.
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Result
Exactly G_u(q5,q3)=[(1-u)/(1-uq5)]^(5/4)[(1-u)/(1-uq3)]^(3/4). Hence G_u(q,1)/G_u(0,1)=(1-uq)^(-5/4); the common-time diagonal G_u(q,q) instead has exponent2. Powers follow from actual charge norms and the convergent oscillator series. Normalized local T5 insertion has Ward coefficient5/8. Fixed C/J do not generally preserve P5 but jointly transport charge and marking covariantly.
Required assumptions
Marked regularized E8 charged state and sector-grade response
Existing positive E8_1 lattice vacuum source with original D5/A3 marking and 48 retained charges beta: beta^t P5 beta=5/4, beta^t P3 beta=3/4, beta²=2. The regularized charged vertex state has free preparation parameter u=r² in (0,1). N5,N3 are strongly commuting nonnegative oscillator grades; q5,q3 in [0,1] parametrize spectral readout. Keep original C/J matrices. u=48c3^4, q=exp(-2alpha), physical preparation, instrument and common time do not follow.
Model results remain conditional
Calculations in a fixed E8 net, quotient, family packet, or readout apply only under their stated inputs and do not select those inputs.
Mathematical theorem for the fixed function; not a cubic polynomial because the seam response depends on x. No parameter or physical Thomson-transfer derivation; ledger Numerical unchanged.
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Result
Log-convexity of the stated seam response and the sign before x=2c³ prove exactly one positive simple root globally. For M=41 its reciprocal is approximately 137.0359992168407. The analytic proof is distinct from the 10 rerun symbolic/interval checks. It holds for every M>0 and therefore does not select M=41.
Required assumptions
Specified EM function with positive seam response
F(x)=x³−2c³x²+(4/5)c⁶M log(p+q(1−q)^(−5/4)), c=1/(8π), p=1/(6π), q=48c⁴exp(−2x), M>0; original budget M=41. The function and inputs are premises here.