Follow the published construction into its registered claims, then explore reviewed research questions, attempts and the connections that remain open.
Quantum and boundary structure
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.
Finite E8, Pauli/Clifford, code, state, covariance, and instrument constructions supply internal quantum models and scoped guarantees. A code or successful channel is not yet a selected, repeatable physical source with the same parent dynamics.
Starting structure in the Atlas orientation
Concrete finite code and operator structures exist, with local results within explicitly specified source and instrument menus.
Which connection is sought
Open items include common physical preparation, source, interaction, repetition, record preservation, and connection to the TFPT parent.
How it connects
Codes and clocks specify internal information and symmetry structures; gravity additionally requires local geometry and dynamics.
Constructive geometric origin of the supplied six-cycle matrix, without selecting a physical character, CP reader, field source, state or time. Keep twist lines and the harmless common orbit phase. The original physical charge assignment of triality and sheet characters still needs its actual operator map. Originals already declare rho/rho^4 as CP readouts. v233 inserts exponents 1/4 rather than evaluating the actual map J from U6^3,U6^4 to color-Casimir sector parity and family center. Geometric q/p names and the old carrier seam tau do not identify quark/lepton sectors. Clarification 30 October: the phase-free orbit basis absorbs partner phases. Raw s pullback is minus transpose, so raw antisymmetry is on the positive U6-cube sheet. Independent full q/p signs plus R have no rank-three projector; see the new complete deck test.
Read the exact result, assumptions and evidence
Result
Actual odd spin lines have nonzero global multiplication isomorphisms into the one-dimensional mixed twisted-canonical sectors. Six off-diagonal sectors form a single orbit under actual R=sc²; spin signs cancel after six steps. On the existing sixteenfold Kummer cover, intrinsic Hodge positivity and deck-character orthogonality make the orbit realization unitarily equal to the oriented v231 U6. Its rho projector has rank one although the full trace vanishes. Existing triality/sheet factors U6^4,U6^3 select rho and rho^4 joint character lines.
Required assumptions
Recovered genus2 cover with retained coefficients
Retain exactly the older three-sheet cover C:w³=(z²-1)/(z²+1), eta=z(1-w³), eta²=1-w⁶, six Weierstrass points p_a=omega^a,q_a=-omega^a, given z base and clock markings. Seek actual flat coefficient lines for existing v117 monodromy, not mere permutation equivalence or an assumed field intertwiner.
Unchanged A0* Fuchsian equation and actual C4 clock
Fix exactly v115 A0*, U=diag(1,i,-i), residues U^k A0* U^-k at i^k and regular base point z=0. Retain base rotation, positive meridian on t=z⁴ and simultaneous fiber basis change. No new Riemann Hilbert solution or D4 reflection lift is assumed.
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.
Retain exactly the older three-sheet cover C:w³=(z²-1)/(z²+1), eta=z(1-w³), eta²=1-w⁶, six Weierstrass points p_a=omega^a,q_a=-omega^a, given z base and clock markings. Seek actual flat coefficient lines for existing v117 monodromy, not mere permutation equivalence or an assumed field intertwiner.
Unchanged A0* Fuchsian equation and actual C4 clock
Fix exactly v115 A0*, U=diag(1,i,-i), residues U^k A0* U^-k at i^k and regular base point z=0. Retain base rotation, positive meridian on t=z⁴ and simultaneous fiber basis change. No new Riemann Hilbert solution or D4 reflection lift is assumed.
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.
Scopedexplicitbarekernel/fixedPstr/positiveconsumer,nouniversalphaseveto. GivenSeedstate/timealreadyexist;typedinsertionsaremissingbeforeevaluation. Originalcoherentopenlegorbroaderconnectionallowed. AlgebraicrhocharacterisnotmeasuredCPphase. Actual G-metric P/Q-to-U6 path is now positively closed; no further free metric choice. Fullspine/Pstr/original insertion remain distinct.
Read the exact result, assumptions and evidence
Result
Actual originalchain usesU6,Dy=yI-deltaU6 andfixedcompressionpositiveKstr. ExactDdaggerDdependsonU6+U6daggerandisorientationeven. UnsquaredresolventhasorientedFourierpowersbutdisplayed36sitematrixelementsarerealpolynomials. UnspecifiedVadmdoesnotderiveorientedresponse. v561suppliesrho;4rho/P2/V5arescalardiagnostics,notE8adjointtrace/sourceoperator. Actualv252/F5callhasnoC6representationororientedinsertion. Existingcommon-rayphaseblindnessanddistinctrelative-sourcequadraturesretained. Clarification30Oct: original A=D_fPstr,H=A†A,Kstr=H^-1/2 is fixed Gram normalization. PolarV=AK is isometric, but originalY uses HolK, not HolV. K as coupling coefficient need not be a CAR field isometry. BareU6=1 norm countertest excludes only that misidentification. K has an exact cubic cosine expression and fixedPstr variation δY=(δHol)K+HolδK with resolvent derivative; actualδD/δHol and endpoint variations must come from source.
Required assumptions
Original hard-holonomy contract with pure closed-triangle trace
Read original45 flavor sources defineY from canonical minimal paths of a Hermitian family connection andPi_triangle=Hol12Hol23Hol31 as ordered closed holonomy,delta=argtrace. DisplayedPi includes neitherKstr nor extraZ6operator. Nonreal asymptotic is a readout contract to test,not completed physical derivation. Active source retains absolute wall selector;no automatic physicalconnection=v117.
Actual full v252 gauge lift and original P2 comparison
Given the full unchanged v252 constructor pi,J_F,gamma_F,D_F and its symbolic Yukawa/Majorana inputs. Compare real gauge lift U=pi(u)J_F pi(u)J_F^-1 on the connected unimodular branch lambda det(m)=1 with original oriented P2 carrier E3+E2,Y=(-1/3)^3+(1/2)^2. No full Spin10 source action is presumed. A cyclically fixed neutral family line is considered only with an expressly supplied sigma=(123) and eigenvalue1; its original physical selection is not assumed.
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 hard-holonomy contract with pure closed-triangle trace
Read original45 flavor sources defineY from canonical minimal paths of a Hermitian family connection andPi_triangle=Hol12Hol23Hol31 as ordered closed holonomy,delta=argtrace. DisplayedPi includes neitherKstr nor extraZ6operator. Nonreal asymptotic is a readout contract to test,not completed physical derivation. Active source retains absolute wall selector;no automatic physicalconnection=v117.
Unchanged A0* Fuchsian equation and actual C4 clock
Fix exactly v115 A0*, U=diag(1,i,-i), residues U^k A0* U^-k at i^k and regular base point z=0. Retain base rotation, positive meridian on t=z⁴ and simultaneous fiber basis change. No new Riemann Hilbert solution or D4 reflection lift is assumed.
Recovered genus2 cover with retained coefficients
Retain exactly the older three-sheet cover C:w³=(z²-1)/(z²+1), eta=z(1-w³), eta²=1-w⁶, six Weierstrass points p_a=omega^a,q_a=-omega^a, given z base and clock markings. Seek actual flat coefficient lines for existing v117 monodromy, not mere permutation equivalence or an assumed field intertwiner.
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.
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.
Actual CAR boundary covariance and oriented amplitude pairing
The full geometric two-face graph G is additionally identified as the actual CAR state covariance. The first labeled fiber is input/dual, the second output; the source realizes the specified fermionic boundary-state/operator pairing. These are physical identification premises, not consequences of matrix sizes or classical Cauchy projection. Normalized data determine only the operator ray and not the absolute partition factor.
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.
Alternative chiral comparison of q columns with actual v252 P2 carrier
For this explicitly alternative comparison identify actual G columns(L0,L2,L1) with supplied generation slots through whole signed P2 dictionary. D_E acts on gamma_F positive,barD_E on negative. Retain unchanged full_D with Y and symmetricMR,F5 structure,faces,graph state and given time. Do not silently replace earlier particlewise hypothesis. No P1 selection,global trivialization,new state/time or physicalE8gauge action assumed.
Geometric Clifford boundary with explicit changed complex structure
Assume the existing free product class B=Gamma A or actual smooth tangential odd finite coefficient B_Phi=Z A-S Phi with total grading Z tensor gamma_F. Apply the standard Clifford boundary functor on the underlying real space with NEW complex structure Ical=i_old Gamma_tot and real structure C0=i_old gamma_n; the dual face has -C0. C0 is old-linear and new-antilinear,not identified with original charge J. This differs from full complex CAR quantization of both independent normal copies. State conclusions use the full graph as the actual quantum covariance in this functor. Its physical selection from P1/P2 is not presumed proved; Phi is a fixed classical background. Keep the fixed normal-independent product collar; a(theta) is smooth Hermitian and even,Phi(theta) smooth Hermitian and odd. No quantization of these bosonic backgrounds.
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.
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.
Alternative chiral comparison of q columns with actual v252 P2 carrier
For this explicitly alternative comparison identify actual G columns(L0,L2,L1) with supplied generation slots through whole signed P2 dictionary. D_E acts on gamma_F positive,barD_E on negative. Retain unchanged full_D with Y and symmetricMR,F5 structure,faces,graph state and given time. Do not silently replace earlier particlewise hypothesis. No P1 selection,global trivialization,new state/time or physicalE8gauge action assumed.
Actual full v252 gauge lift and original P2 comparison
Given the full unchanged v252 constructor pi,J_F,gamma_F,D_F and its symbolic Yukawa/Majorana inputs. Compare real gauge lift U=pi(u)J_F pi(u)J_F^-1 on the connected unimodular branch lambda det(m)=1 with original oriented P2 carrier E3+E2,Y=(-1/3)^3+(1/2)^2. No full Spin10 source action is presumed. A cyclically fixed neutral family line is considered only with an expressly supplied sigma=(123) and eigenvalue1; its original physical selection is not assumed.
Geometric Clifford boundary with explicit changed complex structure
Assume the existing free product class B=Gamma A or actual smooth tangential odd finite coefficient B_Phi=Z A-S Phi with total grading Z tensor gamma_F. Apply the standard Clifford boundary functor on the underlying real space with NEW complex structure Ical=i_old Gamma_tot and real structure C0=i_old gamma_n; the dual face has -C0. C0 is old-linear and new-antilinear,not identified with original charge J. This differs from full complex CAR quantization of both independent normal copies. State conclusions use the full graph as the actual quantum covariance in this functor. Its physical selection from P1/P2 is not presumed proved; Phi is a fixed classical background. Keep the fixed normal-independent product collar; a(theta) is smooth Hermitian and even,Phi(theta) smooth Hermitian and odd. No quantization of these bosonic backgrounds.
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.
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.
Actual full v252 gauge lift and original P2 comparison
Given the full unchanged v252 constructor pi,J_F,gamma_F,D_F and its symbolic Yukawa/Majorana inputs. Compare real gauge lift U=pi(u)J_F pi(u)J_F^-1 on the connected unimodular branch lambda det(m)=1 with original oriented P2 carrier E3+E2,Y=(-1/3)^3+(1/2)^2. No full Spin10 source action is presumed. A cyclically fixed neutral family line is considered only with an expressly supplied sigma=(123) and eigenvalue1; its original physical selection is not assumed.
Original oriented exterior carrier
Given E=C5=E3⊕E2, a Hermitian metric, volume orientation, S± and Y=(-1/3)^3⊕(1/2)^2. Internal carrier labels are not physical vacua; geometric seam reflection is not identified with carrier conjugation.
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.
Existing declared jointK/family comparison onC. Positivebundlelift is not automatic microscopic96/E8 orinnerA_Fgaugeidentity. Qisnotkappa orphysicaltime. No universal fixedQSeedcondition/P1veto. Actual localalgebra,seam,collar,reference,state/time stillrequirecommonidentification;givenSeeddataretained.
Read the exact result, assumptions and evidence
Result
Actual G order(L0,L2,L1) givesW=omega diag(1,-1,1),extendedbyFq=diag(omega,omega,-omega,-1)inSU4. This sameglobalparallelKautomorphism onC preserves allE8branches,Lieproducts andadaptednativekappa,sigma,c. ItconjugatesKQtoinverse whilefullbase remainsQ;nonzero[S,Pc] preventsparallelzdescent. Candidateiota_mq(-I5)hasdifferentGsign. FullE0 obeysinverseQrelation;leftcompensationleavesverticalDQ. Seedopdoesnotseparatelyfixv117Q. Simultaneouswholetransportdiffersfromleftcomposition;localQimagecanforgetDQonlyifAdDQtrivial,andwholeevenfamilyCARdetectit.
Required assumptions
Supplied split carrier with actual q sign lines on genus-two cover
Given existing split carrier E3⊕E2 with unitary split connection onX and actual unitary flat q linesL0,L1,L2 on old coverC:w³=(z²−1)/(z²+1),η²=1−w⁶,product1 andπ*Fv117=L0⊕L1⊕L2. Pull these data toX×C and combine with declared alignment to mA slots. This does not selectX,E,mA or alignment as original P1 quantum source.
Unchanged A0* Fuchsian equation and actual C4 clock
Fix exactly v115 A0*, U=diag(1,i,-i), residues U^k A0* U^-k at i^k and regular base point z=0. Retain base rotation, positive meridian on t=z⁴ and simultaneous fiber basis change. No new Riemann Hilbert solution or D4 reflection lift is assumed.
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 whole operator/state/time FAMILY covariance of givenF5/96 source under explicitq/generation alignment. D_E alone is not generic sameΦ symmetry;complexY/MR are reflected. Numerical countercontrol is diagnostic;block identity is proof. W_E is algebra-preserving commutant unitary basis equivalence,not innerSMgauge;nativeK/clock/reference admissibility not proved. A sharedG frame change transformsΦ andJ jointly,different from additionalW_E source action. No universalMajorana/OS obstruction fromω. Circle parameter is not derived physicalOS time. No physicalE0cut or antiξ-to-linear seam deduction. Source001/002 already supply boundary operator,Seedstate/time;old local-source embedding on cyclic image suffices,no unnecessary global presentation equivalence. No universal rank6q+p requirement for all doubles. FullP1generation andT1–T8 remain unclosed. Update: abstractparallelK/E8coverextensionisnowproved. Itsactualchiral96restrictiondiffersfromthisearlierparticlewisehypothesis. Adaptednativeclocksfixed,flavorQtransportedandnotuniversalSeedrequirement.
Read the exact result, assumptions and evidence
Result
Original realA equation gives fullE0 field map J_E^rowψ=U_Fbarψ(ibarz). In actual constructedG frame,D_E=Gbase^-1U_FbarGbase=ω²S,S=diag(1,−1,1),unitary,D_EbarD_E=I;independent exact matrix substitution verified. Canonical spinξ cancels against half-form boundary factor in NS coefficients. Under declared v252 generation alignment KE=DcalκP_E has D_E on particles,barD_E on antiparticles,commutesγ_F,J_F andsquares1. Exact coupling images:Y_f^E=SbarY_fS,MR^E=ωSbarMR S,with requiredMajorana transpose. ExistingIcal makes𝒥=IcalKE NEW-complex-antilinear involution transportingC0,C_faces andallfourT_faces slots. Exact𝒥GΦ𝒥^-1=GΦE includesbothcrossblocks;givenprojectorCARstate andallwordstransportwithnonewstate. Givenunitarytime has parameterreversal j_Ee^(ithΦ)j_E^-1=e^(-ithΦE). Realconstructorcontrols return tosameΦviaW_E=VωL_S=Dcal^-1;actualtridiagonalMRrequiresbothfactors.
Required assumptions
Declared comparison of actual q columns with supplied v252 generation slots
For operator comparison identify actual ordered horizontal q columnsG with three supplied generation slots of v252 full_D basis. D_E=Gbase^-1U_FbarGbase acts on particle families,barD_E on antiparticles; Φ remains given full_D constructor with its Y_f and symmetricMR. Retain F5 Ical,C0,T_faces,NS domain and full graph covariance. This alignment is declared comparison input,not derived from kernel count,H0,equal dimensions orP1. Selects no mass,state,physical time or native action permission.
Unchanged A0* Fuchsian equation and actual C4 clock
Fix exactly v115 A0*, U=diag(1,i,-i), residues U^k A0* U^-k at i^k and regular base point z=0. Retain base rotation, positive meridian on t=z⁴ and simultaneous fiber basis change. No new Riemann Hilbert solution or D4 reflection lift is assumed.
Recovered genus2 cover with retained coefficients
Retain exactly the older three-sheet cover C:w³=(z²-1)/(z²+1), eta=z(1-w³), eta²=1-w⁶, six Weierstrass points p_a=omega^a,q_a=-omega^a, given z base and clock markings. Seek actual flat coefficient lines for existing v117 monodromy, not mere permutation equivalence or an assumed field intertwiner.
Geometric Clifford boundary with explicit changed complex structure
Assume the existing free product class B=Gamma A or actual smooth tangential odd finite coefficient B_Phi=Z A-S Phi with total grading Z tensor gamma_F. Apply the standard Clifford boundary functor on the underlying real space with NEW complex structure Ical=i_old Gamma_tot and real structure C0=i_old gamma_n; the dual face has -C0. C0 is old-linear and new-antilinear,not identified with original charge J. This differs from full complex CAR quantization of both independent normal copies. State conclusions use the full graph as the actual quantum covariance in this functor. Its physical selection from P1/P2 is not presumed proved; Phi is a fixed classical background. Keep the fixed normal-independent product collar; a(theta) is smooth Hermitian and even,Phi(theta) smooth Hermitian and odd. No quantization of these bosonic backgrounds.
Constant odd circle-source coefficient with existing sea and full boundary graph
In the existing Clifford chart on L2(S1,K) with finite K let h0=(-i∂theta+alpha)gamma,alpha=1/4 or3/4,gamma*=gamma,gamma²=I. Supply constant selfadjoint odd Phi,{gamma,Phi}=0,and V=-i gamma Phi,h=h0+V on common periodic H1. Compare given CAR sea projectors P_-(h0),P_-(h) and complete pure two-face projector G_ell(h),ell>0,including crossings. This is the existing source class with classical background, not physical selection from P1 or quantization of dynamic bosons.
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.
Actual full v252 gauge lift and original P2 comparison
Given the full unchanged v252 constructor pi,J_F,gamma_F,D_F and its symbolic Yukawa/Majorana inputs. Compare real gauge lift U=pi(u)J_F pi(u)J_F^-1 on the connected unimodular branch lambda det(m)=1 with original oriented P2 carrier E3+E2,Y=(-1/3)^3+(1/2)^2. No full Spin10 source action is presumed. A cyclically fixed neutral family line is considered only with an expressly supplied sigma=(123) and eigenvalue1; its original physical selection is not assumed.
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.
Only literal pointwise fixed-locus identification on actual C and specified circle map excluded. Sheet-permuting reflection,different original cut or reflected-source transport remain possible. Retain valid q/p point map,spin formula and previous open-source reflection. No global P1 impossibility or ban of geometric doubles. Choosingπ*|dz|² is not forced by canonical spin-line identity. the reviewed source global G calibration question now solved by explicit G,not another gap. Orbit fact doesnot introduce artificialnew physicalchoice:iforiginalQuarterisSeedmorphism,thetwo representativescanbeequivalent. Must checkactualsidemarks. For explicitpointmapσk fiberisU^k;oppositeU^-kframeidentity remainsvalidunderpropercontravariantconvention.
Read the exact result, assumptions and evidence
Result
Actual lift τ_C(w,η)=(−barw,barη) of z→1/barz is antiinvolution,sendingq_a→p_-a,but does not fix wholeπ^-1(|z|=1). Exact regular fiber:z=e^(iπ/4),η=√2,w=(√3+i)/2,(−√3+i)/2,−i. First two are exchanged,only third fixed. Each other global cubic deck liftc^kτ_C likewise fixes only one of three. Literal identification Fixτ_C=entire cable seam fails away from every vertex. Valid half-form relationJτ√dz=±iz^-1√dz determines spin transition in specified reflected inner/outer frame,not original physical Γ± normal-frame identification. Complete marked-circle class:16Mobius/antiMobius sphere mapsi^kz,i^k/z,i^kbarz,i^k/barz give8D4circle actions. Amongq-compatibleanti-cuts,σ1=ibarz ANDσ3=−ibarz avoidmarks and areQ-conjugate. Data giveone mark-freeorbit,not absolute representative. Spinξanti-frame phase is not a newlinearΓ±clutch proof.
Required assumptions
Recovered genus2 cover with retained coefficients
Retain exactly the older three-sheet cover C:w³=(z²-1)/(z²+1), eta=z(1-w³), eta²=1-w⁶, six Weierstrass points p_a=omega^a,q_a=-omega^a, given z base and clock markings. Seek actual flat coefficient lines for existing v117 monodromy, not mere permutation equivalence or an assumed field intertwiner.
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.
Full algebraic frame for given v117 connection on original Yq;actual spin-line origin separately derived. RR justifies finite two-coefficient search,no numerical fit. Initial negative was corrected solver restriction:constants belong toQ(ω),d=ωc;not old-source counterevidence. Meromorphic functions are not flat fiber values. Makes old group-averaged positive coefficient metric explicit,not a CAR state. Three columns are coefficient directions,not physical generation derivation. Does not derive A0 itself from P1 or full96 field/Phi/Γ± domains/state/reflection/physical time. No exhaustive historical novelty claim. Original ledger/proof statuses unchanged. Trace/domain result explicitly uses analytic original inner z disk and its existing NS continuation. This is an input condition,not new physical BΣ selection. Image is C3-equivariant pullback subspace,not arbitrary rank9 space.
Read the exact result, assumptions and evidence
Result
For unchanged plus-sign equation Ψ'=A(z)Ψ with original A0 and U=diag(1,i,−i),an algebraic3×3 G is constructed on actual negative q Kummer cover. A column is g=(h0 p1/(ab),h0 z p2/b,h0 z p3),a=2√2/3,b=√5/3,with explicit rational p1,p2,p3 overw inQ(ω). Its two c images give detG=−27√2(2ω+1)(z4−1)/10. Ψ=G Gbase^-1 has Ψ(0)=I,detΨ=1−z4. All three original equations independently checked by exact direct substitution. V4 acts on right bydiag(ε0,ε2,ε1),c by3cycle. Actual calibrated Kummer Qh=(ω/h2,−ω/h1,−ω/h0) gives entrywise checked G(Qy)=UG(y)KQ,KQ=[[0,1,0],[-1,0,0],[0,0,1]],hence Ψ(Qy)=UΨ(y)U^-1. This is an explicit differential gauge,not only monodromy or point counting. Positive flat coefficient metric is G^-daggerG^-1. Independent metric calculation gives Gbase Gbase†=diag(27/10,9√3/5,3√3). Canonical spin yields explicit weighted trace Wψ=3^-1/2√π' G^-1ψ∘π. With given inner NS continuation,B_H=−i(∂θ−izA)=G(−i∂θ)G^-1 onD_H=G H1_NS inL2_H is closed selfadjoint;no new extension between four marks.
Required assumptions
Unchanged A0* Fuchsian equation and actual C4 clock
Fix exactly v115 A0*, U=diag(1,i,-i), residues U^k A0* U^-k at i^k and regular base point z=0. Retain base rotation, positive meridian on t=z⁴ and simultaneous fiber basis change. No new Riemann Hilbert solution or D4 reflection lift is assumed.
Recovered genus2 cover with retained coefficients
Retain exactly the older three-sheet cover C:w³=(z²-1)/(z²+1), eta=z(1-w³), eta²=1-w⁶, six Weierstrass points p_a=omega^a,q_a=-omega^a, given z base and clock markings. Seek actual flat coefficient lines for existing v117 monodromy, not mere permutation equivalence or an assumed field intertwiner.
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.