Follow the published construction into its registered claims, then explore reviewed research questions, attempts and the connections that remain open.
Carrier, families and E8 closure
The published foundation in this area
32 authored claim references lead into the original ledger and paper sections. This source record remains available even where no separate reviewed research packet is attached.
The finite compiler combines a five-slot carrier, a selected half-spinor action, D5×A3 and Z4 glue into an E8 lattice closure. This establishes a mathematical construction within its stated choices, not the physical gauge group or a first-principles origin.
Starting structure in the Atlas orientation
Under the stated actions, D5×A3 with Z4 glue gives the even unimodular rank-8 E8 lattice; the half-spinor reading depends on the chosen group action.
Which connection is sought
Open items include physical boundary realization, a local interacting chiral 3+1D implementation, mirror decoupling, and derivation of the action from the origin.
How it connects
E8 carries internal clock, code, flavor, and arithmetic structures. Rank, representation, family count, and spacetime dimension remain distinct types.
Counterproof only to the generic positive-weight preservation inference in cited original passages,not the entire geometric/BRST measure theorem under all additional conditions. Finite test is no full P1/P2 countermodel,no TFPT prediction,and no newly chosen physical source. Source Bernstein cone means completely monotone profile,not a general Bernstein function. No actual original field map or completeT1-T8 goal closed. Preserve existing given-source paths,positive transfer constructionv330,Schur/projector/Weyl results. Do not introduce full ambient geometric measure construction as a prerequisite for every neutral local response;direct local OS embedding remains possible. P1 already assumesRP;only a proposed derivation shortcut is excluded.
Read the exact result, assumptions and evidence
Result
The generic RP preservation inference in the old constructive-measure proof is false. A strictly positive RP base with eigenvalues19,1 becomes non-RP under w=exp(-Tr exp(-D²)),despite positive weights,reflection covariance and gap>=1. Exact Delta=e^-1(1-e^-4)²>75/256>1/9>log(10/9);normalized reflected sign response changes from1/19 to-0.12394264612509166625. General nonconstant positive Laplace profiles haveDelta>0;generic failure uses r in(exp(-Delta),1),while fixed9/10 base requires the stated threshold. Finite W>=0 is the universal Schur-multiplier preservation criterion;for a fixed base K0 elementwise-times W>=0 is exact. A suitable reflected factorization is sufficient for repair. Source-independent positive reference denominator cancels in normalized responses and repairs neither false RP nor missing cross coherence.
Required assumptions
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.
Finite test of the generic spectral RP preservation inference
Test only the generic inference used in old measure proofs that a pointwise positive reflection-symmetric spectral weight exp(-Tr f(D²)) preserves existing RP. Test class: classical reflected finite halves,K0=[[10,9],[9,10]],D(s,t)=[[2s,1],[1,2t]],s,t=plus/minus1,f(u)=exp(-u). No full geometric/BRST/branch or P1/P2 realization of these data assumed. General-profile formula uses finite positive Laplace measure;the9/10 threshold is not asserted for arbitrarily small profiles.
Source-reviewed inventory and reuse audit with explicit coverage: automated inventory is not manual full proof/archive review,not a full current suite run,and not a universal absence claim. Existing model arguments are not upgraded to formal or complete physical proofs. Original sources and ledger unchanged. Earlier local-source criticism is recovered knowledge,not a new scientific gap. Full-CAR ground-state reduction requires the same gapped Bogoliubov action,H>=0,H Omega=0 in the same representation; neutral route directly transports full functional. No unnecessary full E8 observable extension for neutral response.
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Result
Inventoried current registry with all707 present modules,788 ledger rows and3108 project Python/Lean/Wolfram sources; closely inspected24 strong Python closure candidates and11 formal interfaces for actual source premises. Reuse the existing QWZ to CAR field/time map,v746/v779 net blocks,v745 analytic sector bound and neutral octic composition. v1015 is a finite QWZ times deck response block; its ZERO wording assumes external source identification. Inspected Lean compositions assume realization implications as axioms,while Calderon/Yukawa interfaces explicitly retain upstream provenance. Two targeted current runs reproduce v622 at10/10 and v1030 at27/27; the latter retains microscopic FEGEN/ALG2 as open. Original master TFPT.TOE.COMPLETE.01 requires AND(T1..T8),all eight remain open in current ledger. Joint two-face source is a current provenance bridge,not sufficient total closure.
Required assumptions
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.
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.
Original P1, boundary, seed and local restriction definitions
Reviewed originals: P1 declares oriented seam, reflection-positive kernel, unit winding and c3; stronger T_boundary includes A_+ as data; operational seed takes A_loc, time, reflection, state, seam class and collar operator as inputs. A_adm(O) is A/A*-invariant restriction of supplied local insertions. Compare without P2/E8/target spinor assumptions and without presuming an original gauge/microscopic localization intertwiner.
Analytic all-mode theorem in the explicitly existing normal source representation, supplemented by exact finite path controls, not an all-mode inference from finite samples. W(f) must already be bounded in the source von Neumann algebra; no norm CAR membership, bounded imaginary-time conjugates or arbitrary odd OS words asserted. The GNS partner is not identified with a physical P1 second boundary. Older papers32 and45 assume the positive field kernel or its reflection positivity. Actual local physical P1 source map, original measure/coupling, physical time, EM and complete TFPT remain open. The old spatial type exclusion retains its stated scope.
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Result
The old Schottky reflection rho(t,s)=(-t,s) does not reverse spatial profiles; its neutral Weyl profile map is -I and is not excluded by the previous -r_s result. In the existing HS source space, W_R(f)=L_Wf and W_L(f)=R_Wf* have opposite Weyl phases directly from right multiplication. J_HS W_R J_HS=W_L is conjugate-linear multiplicative; centered finite bilinears obey j_L(A)=-R_j(A) and J n_R J=I-n_L. The joint functional Tr(sqrt(rho)Wi*sqrt(rho)Wj) is the positive HS Gram of rho^1/4 Wi rho^1/4 without a Gaussian premise. For the given thermal source, fully ordered heat products K_F handle bounded even insertions: ||K_F||2<=sqrt(Z_beta)product||Aj|| and S(ThetaF,G)=Tr K_F* K_G/Z_beta. Strong approximation extends the existing polynomial free functional to existing bounded neutral Weyls. The old Green midpoint X and all four graph blocks are reused, not chosen anew. Exact NS modes pi,3pi test the same original implementation path, including null relations, particle-hole contribution and reflected noncommuting histories.
Required assumptions
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.
Normal even sea CAR source with canonical graded HS doubling
For the algebraic source test use the already given sea Fock/CAR carrier,with faithful even normalized traceclass density rho and its standard HS space,Omega=sqrt(rho),L_A X=AX,R_A X=XA,Gamma X=Pi X Pi. Gamma is the canonical GNS implementer of source parity fixing Omega. Partner fields are represented in the fixed mode-index chart by b_j=−Gamma R_aj;this assumes no physical second P1 boundary. The finite saturation theorem covers arbitrary faithful even finite densities;the separate all-mode route requires the actual normal HS carrier,a complete covariance eigenbasis and saturation in every mode. For the free elliptic connection,rho is the already derived original thermal density,not a newly chosen geometry or temperature. TomitaJ,OSTheta,classical doubling and physical time remain distinct until actually mapped.
Free chiral Cauchy quantization of the canonical elliptic annulus
Treat the dividing half of the given square curve in its canonical flat conformal representative as a product collar. Compute the Cauchy graph of Dplus=partial_t+B_Sigma,B_Sigma=−i partial_s with NS boundary,then interpret it using the expressly free chiral CAR construction as a quasifree two-boundary state. The labelled second-face compression is the covariance;the other is complementary. This Gaussian interpretation does not derive the original relative spectral-action measure,P1 time or EM/Quillen response.
Existing normal thermal source with bounded neutral insertions
Use the already given thermal sea representation of the free elliptic NS source with H>=0, finite Z_beta=Tr exp(-beta H), W=beta/2, rho=exp(-beta H)/Z and its HS standard space. Neutral even insertions including existing current Weyls are bounded in the source von Neumann algebra. Their imaginary-time conjugates are not assumed everywhere bounded; ordered heat products define the functional. The general HS Gram formula needs only an existing normal density, not Gaussianity. This comparison premise asserts neither physical P1 source, second geometric field family nor physical time identification.
Exact necessary algebra identity and complete declared finite menu, not a classification of all profile maps or sources. The excluded candidate was expressly conditional, not an established OS bridge. No exclusion of OS Grassmann symbol products or existing positive Green/null relations. The opposite-face pair is an algebraic target candidate; actual P1 field map, state/RP, physical time/locality/EM and complete TFPT remain open.
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Result
For Theta(W(f))=W(Lf), scalar sign c and product-order sign o, the ordinary Weyl relation forces sigma(Lf,Lg)=c o sigma(f,g). A conjugate-linear order-reversing map requires symplectic L. The previously conditional Theta(Wf)=W(-r f) is antisymplectic on the same single chiral current and is excluded under these type premises. A compactly supported local witness g=f-prime has integral f g-prime=-integral(f-prime)^2 nonzero. A common field minus or Weyl characters do not fix the central phase. Conjugate-linear multiplicative and linear order-reversing reconstructed types pass the single-current test. Oppositely oriented faces with swap and r pass the anti/anti algebraic test conditionally.64 declared variants are checked exactly by matrix forms and directly multiplied rationally scaled Weyl words, with independent normal/-OO review.
Required assumptions
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.
Given eightfold even CAR quotient with marked charge and source time
Use existing fold eta_r(x)=psi((x+2pi r)/8)/sqrt8, local even rank8 CAR algebra on punctured quotient circle, fixed D8 Cartan chart and q=(1)^8, original current normal ordering/Weyl rule, and declared K_alpha source time. DHR sector labels/local von Neumann statement use standard locally normal even-CAR reference/Haag-dual vacuum-net representation. Assume neither normal local P1 single-interval identification,primitiveOS time,spin-structure sum nor bounded sharp spinor field.
Ordinary Weyl products and explicitly specified reflection type
Compare the given chiral current Weyl relations under a real linear profile map L, retaining scalar linearity/conjugation and product preservation/reversal as separate explicit types. Transfer of the OS Grassmann word type to ordinary Weyl products is the tested identification hypothesis, not a proved P1 property. An oppositely oriented face pair remains a conditional target type.
Exact comparison within given actual current representation,not new physics or P1-selected weights. ProvesPhi alone cannot identify source andspinor Kraus operators are not necessary for everyPhi realization. NS14 does not embed allH40 states inrawNS vacuum.4+6 is internal grading of ten pair labels,not new physical3+2 or spacetime dimension. No exclusion of neutral DHR route or allP1 sources.
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Result
Same FoldM splits Ward input40/output40 asNS20+spinor20 andcreation30 asNS14+spinor16. All360 signed columns are168 sector-preserving and192 sector-changing. UniformNS14 has effects3,4,5 and no scalar TP normalization. Positive weights1/6 on8 actualNS roots and1/3 on6 give exactTP onH40 and family gainI4/3 for everyC_m,hence identical fullPhi marginal even for entanglement. This different process preserves source sector. Physical color e3-e2 takesNS e2+e6 tospinor e3+e6;NS14 support lacks full color covariance. Source gradingw=Me1=(e1+e2+e6+e7)/2 factorsPC tensorPF withcarrier dimensions4+6;pureNS20 inputs have only52 of100 carrier matrix directions.
Required assumptions
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.
Given eightfold even CAR quotient with marked charge and source time
Use existing fold eta_r(x)=psi((x+2pi r)/8)/sqrt8, local even rank8 CAR algebra on punctured quotient circle, fixed D8 Cartan chart and q=(1)^8, original current normal ordering/Weyl rule, and declared K_alpha source time. DHR sector labels/local von Neumann statement use standard locally normal even-CAR reference/Haag-dual vacuum-net representation. Assume neither normal local P1 single-interval identification,primitiveOS time,spin-structure sum nor bounded sharp spinor field.
Given E8 fold with retained source charge and P2 grading
Use the same explicit Weyl matrix M from v16-operator-pullback-20261014/fold-results.json, mu_alpha=(j+alpha q)/8 with q=(1)^8 and alpha=1/4 or3/4, Qsource=(Mq).H, and original P2 Cartan charge X=(-2,-2,-2,3,3,0,0,0). Given D5+A3 target frame and compact E8 current representation. Do not assume raw local P1 spinor-field map, executed spectral filter, new physical time or changed source phase.
Conditional normalized-source criterion,not proof P1 suppliesL_gamma or executes a chosen intervention. Priority is original local iota_I preserving support,state,reflection,true time and marked Ward response. For claimed correlation kernel do not require added measurement instrument. Full field/spacetime claims retain stronger conditions.
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Result
Pure observable response can be written T(a)=sum L_beta†aL_beta+sum L_gamma†rho_s(a)L_gamma for given localized star automorphism and bounded local observable coefficients. Unitality fixes normalization; each term is CP. Individual charged spinor need not belong toA. Full local E8/Q-system extension is stronger realization for charged individual fields and0<->s field coherences. Spinor endomorphism and smooth transport now constructed on given quotient net are not another missing choice there.
Required assumptions
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.
Given eightfold even CAR quotient with marked charge and source time
Use existing fold eta_r(x)=psi((x+2pi r)/8)/sqrt8, local even rank8 CAR algebra on punctured quotient circle, fixed D8 Cartan chart and q=(1)^8, original current normal ordering/Weyl rule, and declared K_alpha source time. DHR sector labels/local von Neumann statement use standard locally normal even-CAR reference/Haag-dual vacuum-net representation. Assume neither normal local P1 single-interval identification,primitiveOS time,spin-structure sum nor bounded sharp spinor field.
Given E8 fold with retained source charge and P2 grading
Use the same explicit Weyl matrix M from v16-operator-pullback-20261014/fold-results.json, mu_alpha=(j+alpha q)/8 with q=(1)^8 and alpha=1/4 or3/4, Qsource=(Mq).H, and original P2 Cartan charge X=(-2,-2,-2,3,3,0,0,0). Given D5+A3 target frame and compact E8 current representation. Do not assume raw local P1 spinor-field map, executed spectral filter, new physical time or changed source phase.
Closes algebraic DHR existence/smooth neutral line on given quotient net. Proven bounded implementers,localized Ad action,and local vN transporters in Haag-dual vacuum-net representation; do not infer norm-C* membership from kernel. Sharp step violatesH1/2; exponent2 and renormalized matrix elements are determined,general closability/UV operator normalization require energy bounds/domains. Quotient interval has eight cover arcs. No raw P1 single-interval,OS-time,field-channel or executed-CP proof.
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Result
On given even quotient CAR net g_I=exp(i a_I/2),with exterior values a_I=0,2pi,defines localized automorphism. Branch signs are trivial parity on even words. Fixed q chart labels s=q/2,Q=4,h=1; odd pseudolocality alone does not distinguish s/c. For two localizations b_IJ=(a_I-a_J)/2 is smooth periodic and existing W(-b_IJ oF) implements transport. Exact fold gives J_tot,n=J_cover,8n,level8 and8(1/2)^2=2=s². Original CCR,adjoint and Hall/Wick functionals determine smooth transport histories. K_alpha time gives exp(-itn); unscaled cover time exp(-i8tn). Retain Q zero modes and charged-field action.
Required assumptions
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.
Given eightfold even CAR quotient with marked charge and source time
Use existing fold eta_r(x)=psi((x+2pi r)/8)/sqrt8, local even rank8 CAR algebra on punctured quotient circle, fixed D8 Cartan chart and q=(1)^8, original current normal ordering/Weyl rule, and declared K_alpha source time. DHR sector labels/local von Neumann statement use standard locally normal even-CAR reference/Haag-dual vacuum-net representation. Assume neither normal local P1 single-interval identification,primitiveOS time,spin-structure sum nor bounded sharp spinor field.
Given E8 fold with retained source charge and P2 grading
Use the same explicit Weyl matrix M from v16-operator-pullback-20261014/fold-results.json, mu_alpha=(j+alpha q)/8 with q=(1)^8 and alpha=1/4 or3/4, Qsource=(Mq).H, and original P2 Cartan charge X=(-2,-2,-2,3,3,0,0,0). Given D5+A3 target frame and compact E8 current representation. Do not assume raw local P1 spinor-field map, executed spectral filter, new physical time or changed source phase.
Sector-resolved response needs actual designated branch with scalar effect. Exclusive C5 support of unread entire process is required only for unconditional purePhi total response. Orthogonal output grades already define mathematical instrument components; added hardware record is unnecessary. Full process retains actual2/5 Lambda1 carry. No physical event-time law,reset or raw P1 use follows. Process and state remain distinct.
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Result
Previously verified full60 current process has canonical CP outputs E+ from carrier degree2 to3 and E- to1. Creationgain3 times familygain3 and annihilationgain2 times3 with totalgain15 give E+*(I)=3I40/5 and E-*(I)=2I40/5. Thus Q+=(5/3)E+ is CPTP and equals direct30 normalization1/9. Tr_F Q+=Phi Tr_F holds for entangled inputs. More generally L_r=sum_m C_m tensorF_rm with effect pI and independence of25 C_m†C_n forces operator-valued sum_r F_rm†F_rn=(p/3)delta_mn I, hence Tr_F E=pPhi Tr_F without uniform weights.
Required assumptions
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.
Given local E8_1 vacuum representation and explicit cocycle
Positive level-one E8 lattice vacuum representation in orthonormal D5+D3 coordinates, declared simple-root cocycle, level-one Heisenberg Ward rules and internal quarter character v=(0^5,1/2^3). Insertions are separated. No raw-P1 pullback or physical time law is assumed or derived from this representation.
Given E8 fold with retained source charge and P2 grading
Use the same explicit Weyl matrix M from v16-operator-pullback-20261014/fold-results.json, mu_alpha=(j+alpha q)/8 with q=(1)^8 and alpha=1/4 or3/4, Qsource=(Mq).H, and original P2 Cartan charge X=(-2,-2,-2,3,3,0,0,0). Given D5+A3 target frame and compact E8 current representation. Do not assume raw local P1 spinor-field map, executed spectral filter, new physical time or changed source phase.
Exact joint character identity on same marked source, no fitted extra clock or discarded charged phase. Lattice proof extends beyond complete240-root check. Closes this internal clock comparison; identifies neither affine winding, NS/R transition nor OS time. Actual local P1 use of filter remains part of Xi.
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Result
For actual given fold holonomy g_alpha=exp(2pi i Mmu_alpha.H), entire E8 lattice module satisfies g_alpha²=exp(2pi i alpha Qsource/4) Cint^-1. With c0=M(j/4)=(-1,0,2,-1,0,3/2,-1/2,-1/2) and v=(0^5,1/2^3), c0+v=(-1,0,2,-1,0,2,0,0) belongs toD8 subsetE8=E8*. Inverse is essential: C0 differs from Cint on all128 halfroots. For either quarter, U5 residue3 plus eigenvalue-1 of g_alpha² exp(-2pi i alpha Qsource/4) selects exactly creation30. Omitting charge factor leaves raw Ward-phase spaces of1 or11 directions, each with only one creation root.
Required assumptions
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.
Given local E8_1 vacuum representation and explicit cocycle
Positive level-one E8 lattice vacuum representation in orthonormal D5+D3 coordinates, declared simple-root cocycle, level-one Heisenberg Ward rules and internal quarter character v=(0^5,1/2^3). Insertions are separated. No raw-P1 pullback or physical time law is assumed or derived from this representation.
Given E8 fold with retained source charge and P2 grading
Use the same explicit Weyl matrix M from v16-operator-pullback-20261014/fold-results.json, mu_alpha=(j+alpha q)/8 with q=(1)^8 and alpha=1/4 or3/4, Qsource=(Mq).H, and original P2 Cartan charge X=(-2,-2,-2,3,3,0,0,0). Given D5+A3 target frame and compact E8 current representation. Do not assume raw local P1 spinor-field map, executed spectral filter, new physical time or changed source phase.
Closes smaller algebraic bridge under given local E8 representation and oriented Ward comparison. No added physical SU5 gauge, mandatory family A4 closure or hardware measurement. Original U5 is scalar on fixed carrier degree; theorem uses uniquely extended adjoint current action. E_lambda is old-source bosonic current of Qsource4, not raw P1 single fermion. Algebraic selection alone derives neither local Xi nor actual response policy.
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Result
Original D5+A3 target g2=(10,6) splits into Creation30=(5,6) of U5 residue3 and Annihilation30 of residue2. Neutral SU5_C times D3_F orbit of stipulated lambda_A=e3+e6 is exactly Creation30. Full E8 residue3 instead has50=30g2+20g3; joint internal quarter grade2 and U5 residue3 selects30. Actual Chevalley amplitudes Lambda2 C5 tensor4 to Lambda3 C5 tensorbar4 have360 signed columns and gain9I40 on both sides. With pinned joint CAR phases, normalization1/9,Hodge and family trace, full carrier Hodge channel follows for arbitrary inputs. Color18 and weak12 separately have nonscalar effects; marked union has scalar gain.
Required assumptions
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.
Given local E8_1 vacuum representation and explicit cocycle
Positive level-one E8 lattice vacuum representation in orthonormal D5+D3 coordinates, declared simple-root cocycle, level-one Heisenberg Ward rules and internal quarter character v=(0^5,1/2^3). Insertions are separated. No raw-P1 pullback or physical time law is assumed or derived from this representation.
Given E8 fold with retained source charge and P2 grading
Use the same explicit Weyl matrix M from v16-operator-pullback-20261014/fold-results.json, mu_alpha=(j+alpha q)/8 with q=(1)^8 and alpha=1/4 or3/4, Qsource=(Mq).H, and original P2 Cartan charge X=(-2,-2,-2,3,3,0,0,0). Given D5+A3 target frame and compact E8 current representation. Do not assume raw local P1 spinor-field map, executed spectral filter, new physical time or changed source phase.
Removes another unnecessary origin condition: full Killing orbit average is sufficient but unnecessary for carrier marginal. P1 must deliver actual normalized closed CP bracket process on the correct charged carrier. A single Ward current, non-TP postselected branch, extra Kraus directions or mere field availability do not automatically meet these conditions. No complete physical TFPT solution. Whole-CPTP theorem remains correct. Actual sector-resolved source branch only needs same carrier Kraus support and effect pI; its normalized carrier marginal is alreadyPhi. Do not demand an exclusively Hodge unread total process as general necessary physical premise.
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Result
Every CPTP joint map End(H10⊗F5bar)→End(H10bar⊗F5) with all Kraus operators in actual span{C_m⊗A_ab} obeys Tr_Fout E=Phi∘Tr_Fin. For any family density, reduced carrier map is CPTP with Kraus space inC5; existing injective25-coefficient TP theorem forces Phi without SU5 covariance. Product operators span the full input algebra, extending equality to entangled inputs. Arbitrary coherent insertion metric and unknown family state cannot change this marginal if TP and support hold.
Required assumptions
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.
Given local E8_1 vacuum representation and explicit cocycle
Positive level-one E8 lattice vacuum representation in orthonormal D5+D3 coordinates, declared simple-root cocycle, level-one Heisenberg Ward rules and internal quarter character v=(0^5,1/2^3). Insertions are separated. No raw-P1 pullback or physical time law is assumed or derived from this representation.
Concrete new cut bridge under still-conditional original E8 Ward dictionary and full charged current closure. Lie-orbit closure alone derives neither source measure nor actual positive normalized process. Old grade2 alone is not the full50-module. The50-module theorem remains correct as larger A4×A4 closure. New Ward/P2 route needs only original D5+A3 creation30 for carrier response.
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Result
Existing conditional Ward root lambda_A=e3+e6 belongs to actual A4×A4 insertion(5,10), with carrier weight(-2,-2,8,-2,-2) and family Dynkin(0,1,0,0). Closure under40 neutral roots reaches all50 insertion roots through500 directed edges. Old quarter grades split30 grade2 and20 grade3; P2 X values are-2[30],+3[20]. A single bracket has rank12 and is not TP. Thus given Ward dictionary determines the algebraic module more sharply than previously stated.
Required assumptions
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.
Given local E8_1 vacuum representation and explicit cocycle
Positive level-one E8 lattice vacuum representation in orthonormal D5+D3 coordinates, declared simple-root cocycle, level-one Heisenberg Ward rules and internal quarter character v=(0^5,1/2^3). Insertions are separated. No raw-P1 pullback or physical time law is assumed or derived from this representation.
Full existing local E8 field algebra with observer five-code
Accepted field-algebra scope: In accepted original E8_1 lattice vacuum use all existing Cartan/root currents, normal products, derivatives and local smooth smearings; native five-code is input/observer slice, not assumed dynamically closed. Retain all exterior charges/modes and both actual twenties. P,Q only decompose analytic endpoint/memory formulas, never execute intermediate projection. Global mode products of local fields are not localized instruments. PhysicalP1 pullback, intervention history, state/time stay separate. Intrinsic tensor/real-form/simplex reconstruction is not a postulated physical potential/state rule.