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Follow the published construction into its registered claims, then explore reviewed research questions, attempts and the connections that remain open.

Reviewed results

128 matching reviewed results

Scoped exclusion

Register charge obstructs renormalized local half-flux fields under full word contract

In the question: Historical: common source, state and event selection

Only specified grade2/register/word/projection contracts. Changed physical nets, globally supported register Wilson loop, other originally derived sector actions and edge absorbers not excluded. No all-P1 no-go and no assertion that every spinor has this register grade.

Read the exact result, assumptions and evidence

Result

Any arbitrarily long/smeared/renormalized original grade2 sequence obeys exact omega(T*Z*T Z)=-omega(T*T); a bosonic field local away from retained even local Z gives +omega(T*T). Positive nonzero field norm and full joint words exclude locality even without bounded/unitary limit. Shared ZL=ZR excludes faithful left-only flux flip under same full label contract. An old A/A*-projector retaining full even matter and actual QWZ time is register-diagonal; retaining F/D ties r,r+2 or all r. It does not remove register obstruction.

Required assumptions

  • Local register retained in full charged word-limit contract

    Comparison class: original v1033 register grade2 under AdZ, Z retained as bounded even local unitary outside field support, full joint positive word limits with nonzero field norm. No boundedness of renormalized field sequence assumed. Separate two-edge test retains original shared flux ZL=ZR. Projection classification only when retaining the FULL original even matter algebra, time and A/A*-admissibility.

  • 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.

Original evidence

  • REGISTER-GRADE-LIMITS-GAUSS-AND-DIRAC.txt lines 1–111

    Source checked at this snapshot

    Original location and fingerprint

    experiments/theory-contracts/mixed-current-origin-20261014/REGISTER-GRADE-LIMITS-GAUSS-AND-DIRAC.txt

    94dc3fe2f4b612b2a6f081db8339165f6b7beadfb764f4e3ae143b922d9aa8dd

  • REGISTER-GRADE-LIMITS-GAUSS-AND-DIRAC.txt lines 301–344

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    Original location and fingerprint

    experiments/theory-contracts/mixed-current-origin-20261014/REGISTER-GRADE-LIMITS-GAUSS-AND-DIRAC.txt

    94dc3fe2f4b612b2a6f081db8339165f6b7beadfb764f4e3ae143b922d9aa8dd

  • check_register_words_and_fold.py lines 1–141

    Source checked at this snapshot

    Original location and fingerprint

    experiments/theory-contracts/mixed-current-origin-20261014/check_register_words_and_fold.py

    19b57b19a6456e7df7abf9d28559c33525b2a2b272ec9a306cfab51c99bd9bed

  • register-words-and-fold-results.json lines 1–183

    Source checked at this snapshot

    Original location and fingerprint

    experiments/theory-contracts/mixed-current-origin-20261014/register-words-and-fold-results.json

    ecd5bab0a1326aec6b72ba4fdbf6d4a2352100ddb5597d36c46fe8eb250b2160

finding:all-word-register-charged-local-field-limit-obstruction

Scoped exclusion

Direct sharp half flux fails register/quotient locality and local normality

In the question: Historical: common source, state and event selection

Only unchanged sharp actions under their separate actual contracts. Smooth punctured-circle sectors may be locally normal and globally inequivalent and remain open; full-CAR implementability does not imply trivial even sectors. Phi/Sigma witnesses not identified without a map. RightHom(s tensor beta,beta) absorber distinguished from charged field. No all-P1 assertion or microscopic E8 closure. Unavailable user18+38 package not claimed replayed; own original controls and analytic proofs separated.

Read the exact result, assumptions and evidence

Result

22Oct pasted half-flux report independently checked: F_A Z F_A*=-Z while registerZ stays even; finite matterAdP_A inner despite transport/fusion/exchange relations; v746 pair-currentK_j even,clock-invariant and half-flux-flipped in each base window. Direct sharp chiral sign change has non-HS covariance difference near jump with log((eps+delta)^2/(4epsdelta)) divergence; Araki root-HS necessity and even crossed-product extension exclude local normality also on standard even free net. Current v1033 builder Nx8Ny8 confirmsR(d,k)=(2,1),NS(0,0); uniform fixed-filled R has<nLnR>0 versus quasifree1/4,purity1/2. Common flux changes both edges. F_A does not identify complete prescribed NS/R state responses.

Required assumptions

  • Sharp half flux in separate original net/state contracts

    Check separately under their own premises: v1033 with expressly ADDED M4 flux register,F_A=X² tensor(-1)^N_A,even algebra M4 tensor CAR+,common strip flux and uniform fixed zero-space filling; v746 with full CAR of paired window I union(I+N/2),NS-clockS^(N/2),halfcircle sign; direct chiral free limit as sharp-sign Bogoliubov on standard locally normal NS CAR net. No unproved identification of these nets and no exhaustion of smooth/renormalized outer-field limits. Even-to-full normality argument uses the standard free local factor contract.

  • 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.

Original evidence

  • HALBFLUSS-UND-CLAUDE-REVIEW.md lines 1–102

    Source checked at this snapshot

    Original location and fingerprint

    experiments/theory-contracts/mixed-current-origin-20261014/HALBFLUSS-UND-CLAUDE-REVIEW.md

    2132c27bf458130c0c184636256f709a6806c46471ac2c3e6593bce051a7014f

  • check_half_flux_audit.py lines 1–90

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    Original location and fingerprint

    experiments/theory-contracts/mixed-current-origin-20261014/check_half_flux_audit.py

    fe487e44b56d4ca278bf51b299df0c529eafa3a34b2c5dae8403260a5860bb06

  • half-flux-audit-results.json lines 1–47

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    Original location and fingerprint

    experiments/theory-contracts/mixed-current-origin-20261014/half-flux-audit-results.json

    b6b385cbd57357a5e102f5c50072d270c802eded0bff2ea90f819bd950d46041

finding:sharp-half-flux-register-quotient-and-local-normality-exclusion

Scoped exclusion

Automatic full Dirac identification of the chiral current phase fails

In the question: Historical: common source, state and event selection

Original complete two-component Dirac collar and explicit CAR/Lagrangian/implementability class; no novelty claimed for standard current/Dirac theory. No exclusion of all P1 sources or chiral-measure/inflow realizations. Cauchy projection, APS sign subspace and OS Padm stay distinct. No computed fixed-domain spectral response, physical event execution or 4D no-go. Higher-dimensional trace formulas need separate control. All original native4/5/20/carry/E8/eight-preimage structure retained; no new finite-code closure requirement. Prior measure/log-profile boundary and open chiral/determinant-line contracts reused, not closed.

Read the exact result, assumptions and evidence

Result

Excluded is the automatic identification of the complete normal-commuting Dirac-CAR vector current with the original nonzero chiral current phase, only under the stated premises. UR.COLLAR.FACE_CURRENT.01, DIRAC-LIFT continuation: For a complete Lagrangian Dirac Cauchy projection C with N C N*=1-C, c_(1-C)=-c_C. For implementable X,Y commuting with N, unitary covariance also gives c_(1-C)=c_C, hence c_C=0. In the existing product collar B=diag(A,-A), occupations n(A) and1-n(A) on ONE boundary face give -2i,+2i and total0 for the original four-mark-fixed profiles. This differs from the earlier two-face cancellation of one scalar block. Fixed Clifford symbols force g I2 on this two-component module; diag(g,I) changes the normal/tangential symbol. The complete lift D_phi=D-i chi_prime phi Jn-chi phi_prime Jn Gamma is a bounded Hermitian perturbation. Transported domain/reference/Padm give frame covariance; a fixed original selfadjoint domain remains analytically valid but specifies a relative boundary attachment not physically selected here. Explicit extra Dref/Drel commutator terms are retained at fixed geometric R; fixing R alone does not break covariance when U commutes with R. Nonconstant four-mark-fixed profiles do not preserve the old APS sign subspace, which is not a selfadjointness no-go. Original Gamma already identifies D_plus, but not its physical measure/line connection. The prior scalar result remains conditionally valid.

Required assumptions

  • Complete data of both product-collar faces

    A selfadjoint B occurs in an exact normal-independent product equation. The full orthogonal L2 Cauchy graph projection of both labeled faces, their actual fiber identification and independently known positive normal length ell are supplied. Selection of these data from P1/P2 is not presumed.

  • Given charged CAR quantization of the full two-face Cauchy graph

    As in section4 of the original collar proof, additionally assume charged CAR(H direct_sum H) and the pure gauge-invariant quasifree state with occupation G_ell. The second labeled face has n=(1+exp(2ell B))^-1. This is a field/statistics premise, not a consequence of P1; reduction does not select or physically execute a one-face operation. The long-collar limit is used only within this declared operator/CAR class.

  • Fixed scalar Hardy model with quarter time

    H=L²(S¹), C projects onto n≥0, B_alpha=−i∂theta+alpha with alpha=1/4 or 3/4. C and B remain fixed for every candidate. Consider scalar unimodular multiplication operators: continuous symbols for isometry classification and H1 symbols for finite excitation energy. This source class is not derived from P1/P2.

  • 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.

  • Complete Dirac Cauchy source with Lagrangian normal action

    Complete orthogonal Dirac Cauchy projection C on the entire boundary module, with actual normal unitary Clifford action N satisfying N C N*=I-C. Explicitly assume charged CAR quantization with pure quasifree covariance C. Bounded current generators X,Y commute with N and have Hilbert-Schmidt commutators with C. The existing compact product collar B=diag(A_alpha,-A_alpha) on both components and both faces is the concrete control; its smooth scalar boundary multipliers are implementable. Statistics and physical measure selection are not derived from P1; no automatic extension of the unrenormalized trace to higher boundary dimensions.

Original evidence

  • DIRAC-LIFT-ADMISSIBILITY.md lines 1–124

    Source checked at this snapshot

    Original location and fingerprint

    experiments/theory-contracts/collar-current-source-bridge-20261021/DIRAC-LIFT-ADMISSIBILITY.md

    dc50b3805ba93a1a4e19890ea0accb04e66cebe192ce526e405cb362a6cdda6a

  • DIRAC-LIFT-ADMISSIBILITY.md lines 125–248

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    Original location and fingerprint

    experiments/theory-contracts/collar-current-source-bridge-20261021/DIRAC-LIFT-ADMISSIBILITY.md

    dc50b3805ba93a1a4e19890ea0accb04e66cebe192ce526e405cb362a6cdda6a

  • check_dirac_lift.py lines 1–117

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    Original location and fingerprint

    experiments/theory-contracts/collar-current-source-bridge-20261021/check_dirac_lift.py

    1e0047ba99ab68b3d1bc71d10a8ef7d894cd86bab6b7e401bdd4cbff1dee7c02

  • dirac_lift_results.json lines 1–54

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    Original location and fingerprint

    experiments/theory-contracts/collar-current-source-bridge-20261021/dirac_lift_results.json

    f6afbd6af36efd7ffdea93bebd1bbcea296c91efc841ff54725fbe69055e1f4a

  • contract_index.json lines 1–61

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    Original location and fingerprint

    experiments/theory-contracts/collar-current-source-bridge-20261021/contract_index.json

    80de96c729cf3e744da3fdc8ae5da56f3588692de12a8f62dd7602036d92e108

  • PROOF.txt lines 21–61

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    experiments/theory-contracts/seam-full-collar-reconstruction-20261015/PROOF.txt

    9f4effed34316798c6a35e1ac0ec2832cd3720180f476cb8747bb32359b56e6a

  • 001-section-primitive-core-and-carrier-interface-handoff.tex lines 65–80

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    Original location and fingerprint

    documents/archive--tfpt-45--source_extracts--01_boundary_kernel_source/sections/001-section-primitive-core-and-carrier-interface-handoff.tex

    7d6e673d99c29d950dc601283cd51c1cc0b113567eeb79c8396fec9c82a02c79

  • 001-section-primitive-core-and-carrier-interface-handoff.tex lines 302–343

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    Original location and fingerprint

    documents/archive--tfpt-45--source_extracts--01_boundary_kernel_source/sections/001-section-primitive-core-and-carrier-interface-handoff.tex

    7d6e673d99c29d950dc601283cd51c1cc0b113567eeb79c8396fec9c82a02c79

  • 002-section-closure-theorems-from-the-admissibility-complex.tex lines 12–123

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    Original location and fingerprint

    documents/archive--tfpt-45--source_extracts--04_qft_source/sections/002-section-closure-theorems-from-the-admissibility-complex.tex

    61ecee7727bdec47936bbffc028d3dbac5260a025b6dbcce30124a60d635fc9c

  • P1-COVARIANT-INSERTION.txt lines 26–146

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    Original location and fingerprint

    experiments/theory-contracts/seam-collar-multifield-20261016/P1-COVARIANT-INSERTION.txt

    ebb9e0cb15cdc017914d8567131c8d8b75855f20e05551b6f7b350989061e152

  • PROOF.txt lines 271–326

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    Original location and fingerprint

    experiments/theory-contracts/seam-collar-multifield-20261016/PROOF.txt

    3537a2b080df0bb8b5d30c73da7dd83dc8e1ae5a6cfea4bb48a8b99f0080dfce

  • 015-source.tex lines 235–266

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    Original location and fingerprint

    documents/tfpt_research_contracts/sections/015-source.tex

    2ec9c3ab6903e9d29823ee5a52ef588cf8504848df6c51c21f0412f31f9eb886

  • 017-source.tex lines 239–285

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    Original location and fingerprint

    documents/tfpt_research_contracts/sections/017-source.tex

    492599a0d20043a5589ca610ce7e1ebceffb8de043eae8eb406e4469d3e4be83

  • status_ledger.csv lines 746–746

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    Original location and fingerprint

    verification/status_ledger.csv

    8723b921bdc50a6157acc6bee4342b40586eb89bec6d7dcc0abc3309562c78b4

  • status_ledger.csv lines 758–758

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    Original location and fingerprint

    verification/status_ledger.csv

    8723b921bdc50a6157acc6bee4342b40586eb89bec6d7dcc0abc3309562c78b4

finding:full-dirac-cauchy-vector-cocycle-cancels-and-endpoint-domain-distinction

Scoped exclusion

Four polar planes are not a fixed-state equivalence of the quartic space

In the question: Historical: common source, state and event selection

Only markedobservables in statedexistingfield-state/coordinate/adjoint/reference dictionary. Notfourunmarkedtheories orphysicallyadmissibleP1preparations. Larger maps abandoningactualquarticspace/sourcecoordinates/referenceobject notclassified. Nomaximum/minimum/overlap/measurementselector or3+2derivation. Sourcecontainsallfourfields simultaneously; distinguishabilitydoesnotselect.

Read the exact result, assumptions and evidence

Result

Excluded is identifying the four marks as all-response-preserving symmetries of the FIXED original fold state within the specified actual quartic space. Universal central OPE metric forces such action unitary and preservation of tr(Pq D1), whose four exact values are pairwise distinct per quarter. Not a universal classification of physical P1 gauge equivalences or exclusion of passive whole-presentation transports.

Required assumptions

  • 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.

  • Actual native G31 event representation

    Use the actual original Hamming/E8/J matrices and60 reflections, their four-dimensional action, characteristic P64=O2(G31), and existing S6 quotient. These are accepted mathematical core data, not a physical source derived from P1 in this round.

  • Symmetric quartic and actual erasure intertwiner

    Use Sym^4 of the native four-representation, the actual five codeword sums, and the existing one-register erasure intertwiner. The symmetric tensor rule and its physical selection are not silently inferred from the full tensor product.

  • Actual positive Cartan quartic Fock embedding

    Use original Construction-A roots with physical metric dot/2 and u_j=(h_2j-i h_2j+1)/sqrt2 as J=+i basis. Canonically embed the actual five Sym^4 code support sums as neutral grade4 Heisenberg polynomials in the given E8_1 lattice vacuum. No physical preparation follows.

  • Original displayed J-equivariant root isometry

    Use existing S=_SIMPLE and T=_TARGET_SIMPLE from cartan_source._glue_deck_character_certificate: O=T S^-1/sqrt2 maps actual Construction-A roots r/sqrt2 to original Chevalley roots r/2, preserving metric and J. This is the existing concrete map, not a newly fitted embedding; physical P1 selection stays separate.

  • 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.

  • Intrinsic event geometry without marked clock as selector

    User159c5316 17Oct replaces automatic instrument/whitening-origin next step with intrinsic structure test. In accepted full unitaryE8_1 fieldnet use actual quarticproducts,eventrelations,*-operation,centralOPEnormalization. No originalpolar/P2,desired3+2,markedq,selectedclock orphysicalrealstate rule as construction criterion. Compare originalgeometry/clocks only afterwards. Transportmetrics withbasis changes; distinguish centralalgebraicOPE data andstate-dependentGNS responses. Only states with definedcommonfieldmoments; positivefiniteenergycontrols not automaticallyRP/clustering/finiterelativeactionP1seeds. Retain full localproducts,composition,correlations; no assumed independenttensorphysics.

  • Original seam/state data on actual60 flags without fitted selection

    User17Oct: test originalseam/statedata onactual60 flags P(q,S); no fittedclock,coupling,newselectionrule. Additional EXISTING data topreviousunmarkedobject: fullchargedinternalv=(0^5,1/2^3),deck square,originalE8vacuum; optionaloriginalR_neut/retained48familyomission explicitgivenpremise,all4cases. SEPARATEactualoriginalfoldphasesalpha1/4,3/4withfixedexistingM,d=M((j+alpha)/8−1/2);disshift/timediagnostic,notautomaticallyfullCARcovarianceorE8vacuumexpectation. Fullroot/fieldaction,nocompressiononly. NopostulatedphysicalTheta,field/state/normalorderingdictionaryorP1selection.

  • Fixed conformal current reference in original fold-state transport

    Continuation17Oct: same givenchiralCARquarterfold,sea,F Cα F*,existingM/literalO; no newcopies/clock/coupling/selectionrule. NativehidentifiedherewithFIXEDconformalNSpointsplitcurrents;countertermagainstsea-normalorderedHfollowskerneldifference. ThisreferenceidentificationisCONDITIONALdictionarypremise,notphysicalP1originfromM/O. OriginalQWZpositivej≥1andnegativeDfoldorientationwithcharge/current/particleholetransportseparate;bothquartersretained. E8DeltatwistedextensionandoriginalglobalW4fromexistingevenCAR/E8cocyclefactorizationremaingivenextension,nooddCAR/E8localityproof. Noreselectedgroundstate;sourcechargesinitiallyZ8. Fullproducts/oppositepolarization/exteriormodes/charges,noperformedcodeprojection;originali0boundaryvalues,nofittedcontactterms.

  • Four starts at fixed state versus joint datum transport

    Comparison scope: q2,3,4,5 and globalS01. Retain originalFCαF*,M/O,fullE8fields,nativeJ andactualchargedfold,time,adjoint,normalordering,erasure. Separate passive whole-presentation changes, active mathematical field automorphisms and symmetries of FIXED given source state. Marks are actual intrinsic quartic rays/polar planes,not chosen couplings; equivalence retains stated field/coordinate/reference object. Do not postulate physical access orP1selection from comparison.

Original evidence

finding:four-native-polar-marks-not-fixed-source-state-gauge-equivalent

Scoped exclusion

Unit flow, gap and four marks do not force original Ward

In the question: Historical: common source, state and event selection

ONLY implication from named weakercircleconditions to fixedoperatorWard excluded; premise list deliberately does NOT include fixedWard. No completeP1/E8countermodel or physical3+2/eventno-go. Do not identify rawP1 seamindex symbol with givensourcecircle without actuallocalization/operator dictionary.

Read the exact result, assumptions and evidence

Result

For arbitrarya>0,Z*BZ=B+a,pathB_s=B+s a has eigenvaluesomega(n+beta+s):0<beta<1 gives exactlyone upwardcrossing independentofa. UnitSF is not constantunitWard. Exact controls a=(1+epsilon cos(ktheta))^-1,c=alpha,abs(epsilon)<1,k1/4 have samegap1/4,holonomy,SF1;k4 additionally preservesall4marks,equalarctimes/geometricquartercovariance. Yet[B,Z]=aZ differsfromZ forepsilon!=0. Controls not claimed completeP1models; under fullcovariantdatatransport they represent sameunmarkedsource.

Required assumptions

  • Fixed scalar Hardy model with quarter time

    H=L²(S¹), C projects onto n≥0, B_alpha=−i∂theta+alpha with alpha=1/4 or 3/4. C and B remain fixed for every candidate. Consider scalar unimodular multiplication operators: continuous symbols for isometry classification and H1 symbols for finite excitation energy. This source class is not derived from P1/P2.

  • 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.

  • Whole scalar positive first-order comparison class

    Compare all smooth scalar first-order differential operators on already given oriented source circle, fixedL2(dtheta),H1per,positive nowhere-zero principal symbol. Periodic chart contains quarterphase in c/holonomy; do not add domain twist again. Original Balpha is reference point; comparison operators are not all claimed physically admissibleP1 data. Point defects,matrix fibers,nonlocal and general higher-dimensional sources are outside.

Original evidence

finding:unit-spectral-flow-gap-and-four-marks-do-not-imply-fixed-source-ward

Scoped exclusion

Source-fixed gap occupation is not a sharp native3+2 mark

In the question: Historical: common source, state and event selection

ONLY literal identification of this canonical gap-CAR component with sharp native3+2 mark excluded. Qgap itself NOT claimed P1-selected physical event; no measurement, executed projection, closedC5 requirement, no exclusion of all unsharp/nonlinear events or allP1. Boundary eigenmode/internal direction/physical species distinct; original sixrays/60flags/globalpair/E8 retained.

Read the exact result, assumptions and evidence

Result

Actual original gap definition selects mode0 foralpha1/4 and mode-1 foralpha3/4, gap1/4 each. Within same stipulated CAR, Qgap=sgn(E0):a_r*a_r: is full particle/hole projector without rank fitting. On complete actual R_b4 inputs, B=I*I,H=I*QgapI obey EXACTLY H>0 and B-H>0, both rank5. Correct metric response strictly between0 andI, nonscalar/nonidempotent; exterior H-HB^-1H strictly positive rank5, bothquarters. This direct spectral bridge from original scale function is not a sharp3+2 input mark. Qgap is global spectral mode, not insertion localized in proper interval.

Required assumptions

  • 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.

  • Actual native G31 event representation

    Use the actual original Hamming/E8/J matrices and60 reflections, their four-dimensional action, characteristic P64=O2(G31), and existing S6 quotient. These are accepted mathematical core data, not a physical source derived from P1 in this round.

  • Symmetric quartic and actual erasure intertwiner

    Use Sym^4 of the native four-representation, the actual five codeword sums, and the existing one-register erasure intertwiner. The symmetric tensor rule and its physical selection are not silently inferred from the full tensor product.

  • Actual positive Cartan quartic Fock embedding

    Use original Construction-A roots with physical metric dot/2 and u_j=(h_2j-i h_2j+1)/sqrt2 as J=+i basis. Canonically embed the actual five Sym^4 code support sums as neutral grade4 Heisenberg polynomials in the given E8_1 lattice vacuum. No physical preparation follows.

  • Original displayed J-equivariant root isometry

    Use existing S=_SIMPLE and T=_TARGET_SIMPLE from cartan_source._glue_deck_character_certificate: O=T S^-1/sqrt2 maps actual Construction-A roots r/sqrt2 to original Chevalley roots r/2, preserving metric and J. This is the existing concrete map, not a newly fitted embedding; physical P1 selection stays separate.

  • 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.

  • Fixed conformal current reference in original fold-state transport

    Continuation17Oct: same givenchiralCARquarterfold,sea,F Cα F*,existingM/literalO; no newcopies/clock/coupling/selectionrule. NativehidentifiedherewithFIXEDconformalNSpointsplitcurrents;countertermagainstsea-normalorderedHfollowskerneldifference. ThisreferenceidentificationisCONDITIONALdictionarypremise,notphysicalP1originfromM/O. OriginalQWZpositivej≥1andnegativeDfoldorientationwithcharge/current/particleholetransportseparate;bothquartersretained. E8DeltatwistedextensionandoriginalglobalW4fromexistingevenCAR/E8cocyclefactorizationremaingivenextension,nooddCAR/E8localityproof. Noreselectedgroundstate;sourcechargesinitiallyZ8. Fullproducts/oppositepolarization/exteriormodes/charges,noperformedcodeprojection;originali0boundaryvalues,nofittedcontactterms.

  • Original single-circle density and geometric stress

    Same stipulated chiral CAR source, negative-D sea, actual quarter domains, eightfold F and existing M/O. Local density J_m=sum:a_r* a_(r+m): and its half-density geometric stress with alpha ground energy follow from this source. Original scalar phases fold to correlated generally offdiagonal channel profiles, not independently selected E8 root weights. NS/quartic reference remains conditional. Global Fourier modes control existing fields; no P1-selected local profile/detector/coupling. No isolated b->-b invariance for these new responses; transport positive QWZ occupation with charges/currents/V/b together.

  • 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.

  • 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.

  • Fixed scalar Hardy model with quarter time

    H=L²(S¹), C projects onto n≥0, B_alpha=−i∂theta+alpha with alpha=1/4 or 3/4. C and B remain fixed for every candidate. Consider scalar unimodular multiplication operators: continuous symbols for isometry classification and H1 symbols for finite excitation energy. This source class is not derived from P1/P2.

  • Charged CAR algebra and original negative sea

    Assume the actual field algebra is charged CAR(H) and its reference state is the pure quasifree sea with occupation 1−C. Relative charge and positive excitation time are normal ordered against this sea. This physical identification is an additional premise.

  • Original gap-normalized relative P1 action

    Original source defines chi_seed=1/lambda_1^+(|B_Sigma|), S_prim=Tr f(D_rel/chi)-Tr f(D_ref/chi)+i pi Deltaeta/2 for declared spectral test profile. D_rel/ref are geometric odd/even parts; varying reflection, boundary domains, reference, state and eta must be retained. This is the given source function, not a new coupling or physical event rule. Scalar quarter CAR realization and NS/native field dictionary remain explicitly conditional.

Original evidence

finding:original-p1-gap-car-component-not-native-sharp-32-event

Scoped exclusion

Complete original seam response does not yield sharp3+2 input sectors

In the question: Historical: common source, state and event selection

ONLY sharp input-sector/common-spectrum identification excluded. No axiom that physical mark must commute with every response; no exclusion of all nonlinear event relations, histories, output rules or P1. Existing intrinsic six rays/60flags and global seam pair retained. Mathematical response effects are not postulated/performed POVM.

Read the exact result, assumptions and evidence

Result

All four complete Grho are EXACTLY positive definite rank5 in BOTH quarters, sum32B4. Hence Erho=(32B4)^-1/2 Grho(32B4)^-1/2 lies strictly between0 andI, as does every proper nonempty coarsening. Deck-even/odd responses both rank5. Exact common commutant of(32B4)^-1Grho has dimension1 overQ(i). No sharp deterministic character/deck classification of five input directions or common reducing3+2 spectrum of these forms.

Required assumptions

  • 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.

  • Actual native G31 event representation

    Use the actual original Hamming/E8/J matrices and60 reflections, their four-dimensional action, characteristic P64=O2(G31), and existing S6 quotient. These are accepted mathematical core data, not a physical source derived from P1 in this round.

  • Symmetric quartic and actual erasure intertwiner

    Use Sym^4 of the native four-representation, the actual five codeword sums, and the existing one-register erasure intertwiner. The symmetric tensor rule and its physical selection are not silently inferred from the full tensor product.

  • Actual positive Cartan quartic Fock embedding

    Use original Construction-A roots with physical metric dot/2 and u_j=(h_2j-i h_2j+1)/sqrt2 as J=+i basis. Canonically embed the actual five Sym^4 code support sums as neutral grade4 Heisenberg polynomials in the given E8_1 lattice vacuum. No physical preparation follows.

  • Original displayed J-equivariant root isometry

    Use existing S=_SIMPLE and T=_TARGET_SIMPLE from cartan_source._glue_deck_character_certificate: O=T S^-1/sqrt2 maps actual Construction-A roots r/sqrt2 to original Chevalley roots r/2, preserving metric and J. This is the existing concrete map, not a newly fitted embedding; physical P1 selection stays separate.

  • 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.

  • Fixed conformal current reference in original fold-state transport

    Continuation17Oct: same givenchiralCARquarterfold,sea,F Cα F*,existingM/literalO; no newcopies/clock/coupling/selectionrule. NativehidentifiedherewithFIXEDconformalNSpointsplitcurrents;countertermagainstsea-normalorderedHfollowskerneldifference. ThisreferenceidentificationisCONDITIONALdictionarypremise,notphysicalP1originfromM/O. OriginalQWZpositivej≥1andnegativeDfoldorientationwithcharge/current/particleholetransportseparate;bothquartersretained. E8DeltatwistedextensionandoriginalglobalW4fromexistingevenCAR/E8cocyclefactorizationremaingivenextension,nooddCAR/E8localityproof. Noreselectedgroundstate;sourcechargesinitiallyZ8. Fullproducts/oppositepolarization/exteriormodes/charges,noperformedcodeprojection;originali0boundaryvalues,nofittedcontactterms.

  • Original single-circle density and geometric stress

    Same stipulated chiral CAR source, negative-D sea, actual quarter domains, eightfold F and existing M/O. Local density J_m=sum:a_r* a_(r+m): and its half-density geometric stress with alpha ground energy follow from this source. Original scalar phases fold to correlated generally offdiagonal channel profiles, not independently selected E8 root weights. NS/quartic reference remains conditional. Global Fourier modes control existing fields; no P1-selected local profile/detector/coupling. No isolated b->-b invariance for these new responses; transport positive QWZ occupation with charges/currents/V/b together.

Original evidence

finding:original-seam-complete-density-grading-not-sharp-32-input-sectors

Scoped exclusion

Density and geometric responses have no common 3+2 spectral sector

In the question: Historical: common source, state and event selection

ONLY common spectral-sector identification for these forms and literal mode30 polar shortcut. Not a physically executable compressed M5 algebra, no axiom requiring physical marks commute with every response. No exclusion of nonlinear intrinsic event relations/other full field histories/all P1/3+2. Mode30 not adopted as selected intervention.

Read the exact result, assumptions and evidence

Result

Both quarters: B4^-1G_J and B4^-1G_L are B4 selfadjoint with common commutant dimension1 overQ(i), hence generated complex response *-algebra M5 on input labels. No common reducing rank2/3 decomposition of these actual response forms. Density response has five distinct generalized eigenvalues. In COMPLETE mode family J30 response rank2, but rank3 kernel matches none of60 original polar flags; Adjacent rank3 J29 response is not ORTHOGONALLY complementary in B4 metric, but joint rank5 gives an oblique algebraic direct sum. Positive relative normalization for this supplied mode pair remains possible; neither its original selection nor a literal normalized polar comparison is claimed. Mode30 lowers source energy by30, not a derived unitary Coxeter30 action.

Required assumptions

  • 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.

  • Actual native G31 event representation

    Use the actual original Hamming/E8/J matrices and60 reflections, their four-dimensional action, characteristic P64=O2(G31), and existing S6 quotient. These are accepted mathematical core data, not a physical source derived from P1 in this round.

  • Symmetric quartic and actual erasure intertwiner

    Use Sym^4 of the native four-representation, the actual five codeword sums, and the existing one-register erasure intertwiner. The symmetric tensor rule and its physical selection are not silently inferred from the full tensor product.

  • Actual positive Cartan quartic Fock embedding

    Use original Construction-A roots with physical metric dot/2 and u_j=(h_2j-i h_2j+1)/sqrt2 as J=+i basis. Canonically embed the actual five Sym^4 code support sums as neutral grade4 Heisenberg polynomials in the given E8_1 lattice vacuum. No physical preparation follows.

  • Original displayed J-equivariant root isometry

    Use existing S=_SIMPLE and T=_TARGET_SIMPLE from cartan_source._glue_deck_character_certificate: O=T S^-1/sqrt2 maps actual Construction-A roots r/sqrt2 to original Chevalley roots r/2, preserving metric and J. This is the existing concrete map, not a newly fitted embedding; physical P1 selection stays separate.

  • 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.

  • Fixed conformal current reference in original fold-state transport

    Continuation17Oct: same givenchiralCARquarterfold,sea,F Cα F*,existingM/literalO; no newcopies/clock/coupling/selectionrule. NativehidentifiedherewithFIXEDconformalNSpointsplitcurrents;countertermagainstsea-normalorderedHfollowskerneldifference. ThisreferenceidentificationisCONDITIONALdictionarypremise,notphysicalP1originfromM/O. OriginalQWZpositivej≥1andnegativeDfoldorientationwithcharge/current/particleholetransportseparate;bothquartersretained. E8DeltatwistedextensionandoriginalglobalW4fromexistingevenCAR/E8cocyclefactorizationremaingivenextension,nooddCAR/E8localityproof. Noreselectedgroundstate;sourcechargesinitiallyZ8. Fullproducts/oppositepolarization/exteriormodes/charges,noperformedcodeprojection;originali0boundaryvalues,nofittedcontactterms.

  • Original single-circle density and geometric stress

    Same stipulated chiral CAR source, negative-D sea, actual quarter domains, eightfold F and existing M/O. Local density J_m=sum:a_r* a_(r+m): and its half-density geometric stress with alpha ground energy follow from this source. Original scalar phases fold to correlated generally offdiagonal channel profiles, not independently selected E8 root weights. NS/quartic reference remains conditional. Global Fourier modes control existing fields; no P1-selected local profile/detector/coupling. No isolated b->-b invariance for these new responses; transport positive QWZ occupation with charges/currents/V/b together.

Original evidence

finding:original-current-geometric-response-pair-has-no-common-polar-sector

Scoped exclusion

Originalquarticmeansandspectralresponsesmatchnoneof60flags

In the question: Historical: common source, state and event selection

ONLYstateddirectmean/kernel/spectralidentificationsinfixedreference. Physicalprojectorneednotcommutewitheverysourceresponse;NOsuchnewaxiom. NoallP1/state/3+2no-go,norejectionofotheroriginalobservables/chargedhistories/specifiedprofiles. Noeigenvalue/overlap/profilefit.

Read the exact result, assumptions and evidence

Result

Bothoriginalquartercases:onepointRieszraymatchesnoneof6native rays;D1rank4hasuniquekernelalsononeof6. NONEof60P(q,S)commuteswithD1orcompleteB4;thereforenoneisaspectralprojectorofthesematricesandnocommonreducingpolarflagforfull2pointfamily. Exactsymbolic,nothreshold/fit. FullfixedoriginalinputmodeexternaloscillatortermsretainedinB4.

Required assumptions

  • 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.

  • Actual native G31 event representation

    Use the actual original Hamming/E8/J matrices and60 reflections, their four-dimensional action, characteristic P64=O2(G31), and existing S6 quotient. These are accepted mathematical core data, not a physical source derived from P1 in this round.

  • Symmetric quartic and actual erasure intertwiner

    Use Sym^4 of the native four-representation, the actual five codeword sums, and the existing one-register erasure intertwiner. The symmetric tensor rule and its physical selection are not silently inferred from the full tensor product.

  • Actual positive Cartan quartic Fock embedding

    Use original Construction-A roots with physical metric dot/2 and u_j=(h_2j-i h_2j+1)/sqrt2 as J=+i basis. Canonically embed the actual five Sym^4 code support sums as neutral grade4 Heisenberg polynomials in the given E8_1 lattice vacuum. No physical preparation follows.

  • Original displayed J-equivariant root isometry

    Use existing S=_SIMPLE and T=_TARGET_SIMPLE from cartan_source._glue_deck_character_certificate: O=T S^-1/sqrt2 maps actual Construction-A roots r/sqrt2 to original Chevalley roots r/2, preserving metric and J. This is the existing concrete map, not a newly fitted embedding; physical P1 selection stays separate.

  • 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.

  • Intrinsic event geometry without marked clock as selector

    User159c5316 17Oct replaces automatic instrument/whitening-origin next step with intrinsic structure test. In accepted full unitaryE8_1 fieldnet use actual quarticproducts,eventrelations,*-operation,centralOPEnormalization. No originalpolar/P2,desired3+2,markedq,selectedclock orphysicalrealstate rule as construction criterion. Compare originalgeometry/clocks only afterwards. Transportmetrics withbasis changes; distinguish centralalgebraicOPE data andstate-dependentGNS responses. Only states with definedcommonfieldmoments; positivefiniteenergycontrols not automaticallyRP/clustering/finiterelativeactionP1seeds. Retain full localproducts,composition,correlations; no assumed independenttensorphysics.

  • Original seam/state data on actual60 flags without fitted selection

    User17Oct: test originalseam/statedata onactual60 flags P(q,S); no fittedclock,coupling,newselectionrule. Additional EXISTING data topreviousunmarkedobject: fullchargedinternalv=(0^5,1/2^3),deck square,originalE8vacuum; optionaloriginalR_neut/retained48familyomission explicitgivenpremise,all4cases. SEPARATEactualoriginalfoldphasesalpha1/4,3/4withfixedexistingM,d=M((j+alpha)/8−1/2);disshift/timediagnostic,notautomaticallyfullCARcovarianceorE8vacuumexpectation. Fullroot/fieldaction,nocompressiononly. NopostulatedphysicalTheta,field/state/normalorderingdictionaryorP1selection.

  • Fixed conformal current reference in original fold-state transport

    Continuation17Oct: same givenchiralCARquarterfold,sea,F Cα F*,existingM/literalO; no newcopies/clock/coupling/selectionrule. NativehidentifiedherewithFIXEDconformalNSpointsplitcurrents;countertermagainstsea-normalorderedHfollowskerneldifference. ThisreferenceidentificationisCONDITIONALdictionarypremise,notphysicalP1originfromM/O. OriginalQWZpositivej≥1andnegativeDfoldorientationwithcharge/current/particleholetransportseparate;bothquartersretained. E8DeltatwistedextensionandoriginalglobalW4fromexistingevenCAR/E8cocyclefactorizationremaingivenextension,nooddCAR/E8localityproof. Noreselectedgroundstate;sourcechargesinitiallyZ8. Fullproducts/oppositepolarization/exteriormodes/charges,noperformedcodeprojection;originali0boundaryvalues,nofittedcontactterms.

Original evidence

  • FOLD-COVARIANCE-TO-NATIVE-FIELD-RESPONSE.txt lines 198–229

    Source checked at this snapshot

    Original location and fingerprint

    experiments/theory-contracts/joint-native-algebra-selection-20261016/FOLD-COVARIANCE-TO-NATIVE-FIELD-RESPONSE.txt

    cd35ac0e65ebf780cc99d3dd8a318255d11251125298d88e88cb676c72b27507

finding:original-fold-quartic-mean-and-spectral-responses-do-not-match-sixty-flags

Scoped exclusion

Internal seam,vacuum and original neutral tensor do not select flag root

In the question: Historical: common source, state and event selection

OnlyspecifiedinternalE8vacuum/character/Robject. R/48includesgivenfamilyomission;preserving48spanisnotpreservingnewcoherentsourcecoefficients. NOexclusionfororiginalfulltwistedCARcovariance,additionalphysicalTheta,allP1sources. Individuallatticeliftsuffice,noglobalsplitsectionassumed.

Read the exact result, assumptions and evidence

Result

Fullinternalcharacter+E8vacuumhasnofixedq/flag;oldcomparisonflag(5,{0,1})isin4orbit. OriginalR_neut/retained48givesstabilizer16/logical8=C2³,q-pairs01|23|45,allsame4familyomissions. ExplicitfullE8isometryG=(x3,x4,x1,x2,x5,x6,x7,x8)preservesJ,v,Rfield,48span,vacuum,OPEandactsasquartic(45). Itswapsflags(4,01),(5,01)withactualpolarHS²distance(816−176sqrt6)/625>0. Nouniquecovariantselectorfromthesetesteddatapossible. Supplyingonlyq5stillleavesinvariantpairs01and23.

Required assumptions

  • 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.

  • Actual native G31 event representation

    Use the actual original Hamming/E8/J matrices and60 reflections, their four-dimensional action, characteristic P64=O2(G31), and existing S6 quotient. These are accepted mathematical core data, not a physical source derived from P1 in this round.

  • Symmetric quartic and actual erasure intertwiner

    Use Sym^4 of the native four-representation, the actual five codeword sums, and the existing one-register erasure intertwiner. The symmetric tensor rule and its physical selection are not silently inferred from the full tensor product.

  • Actual positive Cartan quartic Fock embedding

    Use original Construction-A roots with physical metric dot/2 and u_j=(h_2j-i h_2j+1)/sqrt2 as J=+i basis. Canonically embed the actual five Sym^4 code support sums as neutral grade4 Heisenberg polynomials in the given E8_1 lattice vacuum. No physical preparation follows.

  • Original displayed J-equivariant root isometry

    Use existing S=_SIMPLE and T=_TARGET_SIMPLE from cartan_source._glue_deck_character_certificate: O=T S^-1/sqrt2 maps actual Construction-A roots r/sqrt2 to original Chevalley roots r/2, preserving metric and J. This is the existing concrete map, not a newly fitted embedding; physical P1 selection stays separate.

  • 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.

  • Intrinsic event geometry without marked clock as selector

    User159c5316 17Oct replaces automatic instrument/whitening-origin next step with intrinsic structure test. In accepted full unitaryE8_1 fieldnet use actual quarticproducts,eventrelations,*-operation,centralOPEnormalization. No originalpolar/P2,desired3+2,markedq,selectedclock orphysicalrealstate rule as construction criterion. Compare originalgeometry/clocks only afterwards. Transportmetrics withbasis changes; distinguish centralalgebraicOPE data andstate-dependentGNS responses. Only states with definedcommonfieldmoments; positivefiniteenergycontrols not automaticallyRP/clustering/finiterelativeactionP1seeds. Retain full localproducts,composition,correlations; no assumed independenttensorphysics.

  • Original seam/state data on actual60 flags without fitted selection

    User17Oct: test originalseam/statedata onactual60 flags P(q,S); no fittedclock,coupling,newselectionrule. Additional EXISTING data topreviousunmarkedobject: fullchargedinternalv=(0^5,1/2^3),deck square,originalE8vacuum; optionaloriginalR_neut/retained48familyomission explicitgivenpremise,all4cases. SEPARATEactualoriginalfoldphasesalpha1/4,3/4withfixedexistingM,d=M((j+alpha)/8−1/2);disshift/timediagnostic,notautomaticallyfullCARcovarianceorE8vacuumexpectation. Fullroot/fieldaction,nocompressiononly. NopostulatedphysicalTheta,field/state/normalorderingdictionaryorP1selection.

Original evidence

  • ORIGINAL-SEAM-STATE-FLAG-SELECTION.txt lines 117–154

    Source checked at this snapshot

    Original location and fingerprint

    experiments/theory-contracts/joint-native-algebra-selection-20261016/ORIGINAL-SEAM-STATE-FLAG-SELECTION.txt

    bdbba2dae8386cd94e68663ca3c2291ba652df2de563b1a4e114ffa2af4ec1ee

finding:internal-seam-vacuum-and-original-neutral-tensor-do-not-select-flag-root

Scoped exclusion

Determinant cover is not same complete Cartan-lattice event

In the question: Historical: common source, state and event selection

Literal Cartan/lattice automorphism dictionary, not allE8operations,moduleintertwiners orphysicalsources. Prior innerE8lift on DIFFERENT chargedC4/F20currentblocks and finite representation comparison remain valid, not identicalCartanregistermap. Do not treat coherent relativephase as irrelevant rayphase.

Read the exact result, assumptions and evidence

Result

Existing coupled determinant lifth=e^−iπ/4 r acts onquartics as−rho5(r). Coherent incidentresponses−nj−nq haveGramI+J/3 rather thanI+J; positivepolarmark distance²48/25 fromoriginalP2. Unchanged linearCartan actionofh also fails actualE8 charge-lattice preservation:45degree rotation sendsrawroot(2,0,...,0) to(√2,−√2,0,...), outside lattice. All60native r preserve all240roots; all60phase-shifted lifts failsame root test. Hence noVOA-automorphism with EXACTLYthis Cartandictionary.

Required assumptions

  • 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.

  • Actual native G31 event representation

    Use the actual original Hamming/E8/J matrices and60 reflections, their four-dimensional action, characteristic P64=O2(G31), and existing S6 quotient. These are accepted mathematical core data, not a physical source derived from P1 in this round.

  • Symmetric quartic and actual erasure intertwiner

    Use Sym^4 of the native four-representation, the actual five codeword sums, and the existing one-register erasure intertwiner. The symmetric tensor rule and its physical selection are not silently inferred from the full tensor product.

  • Actual positive Cartan quartic Fock embedding

    Use original Construction-A roots with physical metric dot/2 and u_j=(h_2j-i h_2j+1)/sqrt2 as J=+i basis. Canonically embed the actual five Sym^4 code support sums as neutral grade4 Heisenberg polynomials in the given E8_1 lattice vacuum. No physical preparation follows.

  • Original displayed J-equivariant root isometry

    Use existing S=_SIMPLE and T=_TARGET_SIMPLE from cartan_source._glue_deck_character_certificate: O=T S^-1/sqrt2 maps actual Construction-A roots r/sqrt2 to original Chevalley roots r/2, preserving metric and J. This is the existing concrete map, not a newly fitted embedding; physical P1 selection stays separate.

  • 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.

  • Original clock/simplex without an imposed polar mark

    Retain actual normalized W6 simplex, sigma=(234), tau=(01), q=5. Consider ALL Hermitian rank2 projectors P with RanP inside Fixsigma, [P,tau]=0 and one positive/one negative tau eigenvalue on RanP. The original polar rule is a comparison point, not an imposed condition of this compatibility class.

  • Actual native event fields and distinct state controls

    In accepted full E8 field net test actual native reflection automorphisms on reconstructed quartic fields and coherent difference against identity. Original sigma=(234),tau=(01),markedq=5 remain given comparison data; preparation ofq not derived. Vacuum and normalized marked source state are distinct mathematical controls. Difference of automorphism and identity is NOT assumed physically allowed intervention/instrument. Retain all local Wick/Taylor products and complete source states. Positive Gram/relative normalization is examined as computable tensor, never imposed as physical selection rule.

Original evidence

  • SEAM-STATE-EVENT-POLAR-SELECTION.txt lines 217–249

    Source checked at this snapshot

    Original location and fingerprint

    experiments/theory-contracts/joint-native-algebra-selection-20261016/SEAM-STATE-EVENT-POLAR-SELECTION.txt

    c55c96c733a3ad7c314fe251bc8ff8da8940129fd6e99dfc08e449bf4475c1cf

  • CURRENT-RESPONSE-AND-DICTIONARY.md lines 79–109

    Source checked at this snapshot

    Original location and fingerprint

    experiments/theory-contracts/joint-native-algebra-selection-20261016/CURRENT-RESPONSE-AND-DICTIONARY.md

    db9163de1017810818e104f651e531247378a4c8295580c8936cb19e594b4b73

finding:determinant-cover-not-literal-full-cartan-lattice-event

Scoped exclusion

Raw event response and state positivity do not execute polar prescription

In the question: Historical: common source, state and event selection

No all-E8/P1 no-go or claim physical instruments need orthogonal outcome states. Weight8 control disproves corresponding full formal normalization identity, not replacement of all local profiles. Given instrument or other originally grounded nonvacuum history not excluded. Full source,both20s,exterior/memory paths retained.

Read the exact result, assumptions and evidence

Result

Actual raw orbit kernels have spectraKC=(4,1,1,0,0),KW=(3,1,0,0,0), coefficient-matrix commutatorHS²72 and do not preserve originalP2. GNS supplies metricG; originalslotcutQW is notG-selfadjoint ([G,QW]HS²12). Oblique transport has antihermiticitydefect²2, rawWeakSupport distance²(28−8sqrt6)/25 fromP2. Full weight8 regular quartic insertion on given marked source state hasGq=(43/5)I+(73/5)J; same vacuum-normalized fields retain eigenvalues68/5,43/5^4 instead ofI. NativeJ fixes quartics. Positive source metric alone therefore does not select physical positive normalization/readout law.

Required assumptions

  • 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.

  • Actual native G31 event representation

    Use the actual original Hamming/E8/J matrices and60 reflections, their four-dimensional action, characteristic P64=O2(G31), and existing S6 quotient. These are accepted mathematical core data, not a physical source derived from P1 in this round.

  • Symmetric quartic and actual erasure intertwiner

    Use Sym^4 of the native four-representation, the actual five codeword sums, and the existing one-register erasure intertwiner. The symmetric tensor rule and its physical selection are not silently inferred from the full tensor product.

  • Actual positive Cartan quartic Fock embedding

    Use original Construction-A roots with physical metric dot/2 and u_j=(h_2j-i h_2j+1)/sqrt2 as J=+i basis. Canonically embed the actual five Sym^4 code support sums as neutral grade4 Heisenberg polynomials in the given E8_1 lattice vacuum. No physical preparation follows.

  • Original displayed J-equivariant root isometry

    Use existing S=_SIMPLE and T=_TARGET_SIMPLE from cartan_source._glue_deck_character_certificate: O=T S^-1/sqrt2 maps actual Construction-A roots r/sqrt2 to original Chevalley roots r/2, preserving metric and J. This is the existing concrete map, not a newly fitted embedding; physical P1 selection stays separate.

  • 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.

  • Original clock/simplex without an imposed polar mark

    Retain actual normalized W6 simplex, sigma=(234), tau=(01), q=5. Consider ALL Hermitian rank2 projectors P with RanP inside Fixsigma, [P,tau]=0 and one positive/one negative tau eigenvalue on RanP. The original polar rule is a comparison point, not an imposed condition of this compatibility class.

  • Actual native event fields and distinct state controls

    In accepted full E8 field net test actual native reflection automorphisms on reconstructed quartic fields and coherent difference against identity. Original sigma=(234),tau=(01),markedq=5 remain given comparison data; preparation ofq not derived. Vacuum and normalized marked source state are distinct mathematical controls. Difference of automorphism and identity is NOT assumed physically allowed intervention/instrument. Retain all local Wick/Taylor products and complete source states. Positive Gram/relative normalization is examined as computable tensor, never imposed as physical selection rule.

Original evidence

finding:raw-event-state-positivity-does-not-execute-polar-normalization