Follow the published construction into its registered claims, then explore reviewed research questions, attempts and the connections that remain open.
Interlocking clocks
The published foundation in this area
23 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.
TFPT uses several distinct algebraic clocks and transfers: Coxeter period 30, phase automorphisms, an order-12 compiler action, and separate relaxation factors. Their mathematical periods do not by themselves define physical duration.
Starting structure in the Atlas orientation
Known structures include finite actions: Coxeter number 30, μ4 on phase data, an order-12 compiler action, and separate relaxation rates.
Which connection is sought
The open work is a common source derivation, event interpretation, and a parent realizing one time rule for matter, boundary, and instruments.
How it connects
Clock actions organize E8/code readouts and event sequences; algebraic orders are neither measured seconds nor proofs of dynamics.
Constructive reuse of existing DHR/extension theorems, no new general mathematics or physical source. Gamma is the dual extension involution, not automatically original CAR fermion parity. Pointwise projection does not preserve all readers; no physical neutral-output counterexample to exact DHR representation was found. Original P1 net/sector map, eight-arc support,Theta/domain, physical time/positivity/clustering/Padm and full consumer remain to identify. Simultaneous fullU plus h inclusion in unchanged V_D8 fails at124>120 in the same-conformal scope; its extension is not excluded. Prior physical exclusions retain exact scope; no F1 or ledger closure.
Read the exact result, assumptions and evidence
Result
On the given even eightfold source the already marked bosonic order2 sector permits a unique-up-to-gauge local index2 extension B=A+AF, Fa=rho(a)F,F²=u. Its D8 union D8+s charges give E8 without prior full U inclusion. E(a+bF)=a=(id+gamma)/2 is canonical positive. For given omega_A, omega_A∘E is its unique gamma-invariant extension and ||F Omega||²=1. Full even words retain exact A expectations with charged intermediate paths. No additional endpoint norm postulate is needed for these reconstructed coordinates. The same source-time lift is continuously unique under sector covariance, square and cocycle relations. In actual M,32/52 targetU roots and8/12 family roots occupy the added sector. All128 odd current states arise from one marked sector with old even coefficients and original cocycle; coefficient weights0,1,2,3,4 have multiplicities1,28,70,28,1.
Required assumptions
Given even eightfold CAR source with marked bosonic DHR sector
Given quotient net A8(I)=CAR(L2(I,C8))^even with level1 form, original source/state/time/adjoint and its localized transportable bosonic dimension1 order2 sector rho_s, s=q/2=(1/2)^8, hs=1. Standard local simple-current extension hypotheses and actual continuous sector covariance for the time lift. One quotient interval corresponds to eight cover arcs. This conditional premise asserts no physical quotient selection or joint P1 dictionary.
The general clock-forced D8 spinor completion is reused from compiler-clock-current-closure-20260919; generator/extension uniqueness is reused from e-series-source-reconstruction-20261024. Delta is actual M/native sigma chart, smallest marked word and HNF without E8 target. Original active source realization, physical locality/state/reflection/time/Padm/P2,3+1D and gravity remain unproved. Rq!=q; no fixed-quarter-state symmetry. Passive transport requires no common physical algebra. Supplied CAR form remains input.
Read the exact result, assumptions and evidence
Result
For the actual later M chart and native order3 sigma, R is orthogonal. p=e0+e2 in D8 maps to Rp=(1,1,-1,1,-1,1,1,1)/2; delta=e2+e4 gives Rp+delta=q/2 and Rp.delta=-1. Original Chevalley code gives ordered [E_(Mdelta),E_(MRp)]=+E_(Mq/2). Exact HNF of [2B|2RB] for a D8 basis B, WITHOUT an E8 target lattice/root population, gives L=D8+RD8=D8+Z(q/2), index2, even integral Gram determinant1 and RL=L. Of old roots48 stayD8 and64 enter one halfspin class. With joint active local admission the minimal same-conformal field closure is marked E8; selfduality and marked sector occurrence then need no separate completion assumptions. Two independent HNF computations and an actual original current-bracket check confirm this scoped theorem.
Required assumptions
Actual fold chart and active native clock in a common source fibre
Given level1 D8 source lattice/form, unchanged original M from v16 operator pullback 20261014 and native sigma(x)=x[[4,5,0,1,2,3,6,7]] from v634. Physical selection additionally requires active admission of old and R=M^T sigma M transformed fields into ONE local connected unitary source algebra with the same conformal vector and actual matching state/reflection/time/carrier data. Passive chart/background transport alone supplies no such joint admission. M and sigma are not derived from P1 here; native sigma is not sigma_d and R moves q.
Given local E8 current realization with its actual cocycles, adjoints and meridional coordinate map; known general E8 root-product rules are not claimed as globally new mathematics. Does not derive the P1→Z_adm field map, physical state, measure, time generator or full regional Higgs/metric gluing. No F1 or ledger closure.
Read the exact result, assumptions and evidence
Result
For original v983 spinor and four meridian weights vi=(s,mi), the common metric gives vi²=2, vi·vj=1 for different marks and vi−vj=(0,ei−ej). The actual existing current constructor with v498 Affine.act, ordered cocycle and compact adjoint was then executed: all16 spinor signs times12 ordered distinct marks give192 simple poles exactly on their original family roots,96 with coefficient+1 and96 with−1. No phase fit. All64 diagonal cases have double-pole coefficient+1 and the original Cartan simple pole; mixed double poles vanish. Leading twisted terms transport the remaining family root and the known diagonal Cartan shift. This response was not an input of metric selection.
Required assumptions
Given spinor-meridian extension with integral selfdual charge pairing
Fixed additive L=(D5+A3)+Z((1/2)^5,m0), m0=e0−1/4·1 from four oriented puncture meridians, actual product W(D5)×C4 action, positive real symmetric invariant form and integral unimodular total charge pairing. Root lengths, carrier scale, orthogonality and evenness are not additional premises. These common completion data are not a physical source derived from P1.
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.
Conditional rigidity of charge completion. Fixed additive glue lattice, actual product symmetries, real charge metric and integral unimodular total pairing remain joint inputs. Does not derive their physical origin from P1, select a quarter source/state/time, or close3+1D or F1. Derived in this session with no claim of global mathematical novelty. E8 is not an additional premise of metric selection.
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Result
On the fixed original additive spinor-meridian glue lattice the entire positive real W(D5)×C4 invariant metric has three parameters x,a,b: carrier xI5 and family a(P−vvT)+bvvT, P=I−J/4,v=(1,−1,1,−1)/2. W(D5) removes mixed blocks without assumed orthogonality. Integral root pairings force x,b,a+b and hence x,a,b to be positive integers. The original index four gives detL=x^5 a^2 b. Unimodularity forces exactly x=a=b=1. Carrier scale, orthogonality, root lengths and evenness are no longer extra premises in this class. An explicit A3→D3 map identifies the completed lattice with D8 union D8+(1/2)^8; evenness follows. The theorem covers the entire class analytically rather than by sampling. Thirty exact checks pass normally and with −OO; two independent analytic and full invariant-space reviews.
Required assumptions
Given spinor-meridian extension with integral selfdual charge pairing
Fixed additive L=(D5+A3)+Z((1/2)^5,m0), m0=e0−1/4·1 from four oriented puncture meridians, actual product W(D5)×C4 action, positive real symmetric invariant form and integral unimodular total charge pairing. Root lengths, carrier scale, orthogonality and evenness are not additional premises. These common completion data are not a physical source derived from P1.
Integral marked topology and supplied original charge dictionary; no new selection of four punctures, physical clock or blanket exclusion of a different sector-changing field map. Metric normalization follows only under the separate joint-completion theorem. Original paper and ledger unchanged.
Read the exact result, assumptions and evidence
Result
H1=Z4/Z1 and H^1=ker sum have a canonical index-four quotient Z4 through the marked counting construction. In the normalized realization meridians mi=ei−1/4·1 are A3* weights and their differences are A3 roots. m0 literally equals original v983 OMEGA_F and with the supplied D5 spinor gives its actual LAM. All four mi have the same discriminant class. Corner C4 acts trivially on A3*/A3, so its mark permutation is not glue-class translation. The four-by-four delta residue pairing on puncture loops in Architecture section011:32–45 conflicts with their zero sum; correct readers use zero-sum residues or I−J/4. This dual pairing alone selects no positive metric.
Required assumptions
Given spinor-meridian extension with integral selfdual charge pairing
Fixed additive L=(D5+A3)+Z((1/2)^5,m0), m0=e0−1/4·1 from four oriented puncture meridians, actual product W(D5)×C4 action, positive real symmetric invariant form and integral unimodular total charge pairing. Root lengths, carrier scale, orthogonality and evenness are not additional premises. These common completion data are not a physical source derived from P1.
Finite joint process on the given epsilon carrier assuming every Kraus operator in the stated tensor amplitude span and global trace preservation. Does not derive the original P1 source, carrier, local embedding, full trace preservation, event register, general multitime process or full TFPT physics.
Read the exact result, assumptions and evidence
Result
For every joint finite-dimensional CPTP operation with Kraus operators L_s=sum_m C_m tensor A_sm on the given H=Lambda²C5 and arbitrary finite family spaces, global trace preservation and the 25 linearly independent C_m* C_n force sum_s A_sm* A_sn=delta_mn I/3. Thus Tr_F' E(rho_HF)=Phi(Tr_F rho_HF) for all joint states, including correlated and entangled ones. No preselected family state or pre-imposed isotropic Gram is needed. For one trace-decreasing event this fails: two exactly constructed joint states with the same H marginal produce probabilities 1 and 0. This is a corollary of the already recorded 25-product selection theorem.
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 five-slot exterior source with retained complement index
V=C5 with given oriented unitary slot basis and volume form,H=Lambda²V. C_m[kl,ij]=epsilon(m,i,j,k,l) are five distinct linear maps to conjugate target;their coherent sum is a different operation. Inner products and CAR grading remain explicit. No physical record,coupling or time iteration assumed from exterior algebra alone.
Only the stated internal phase family and particular comparison with the given old channel. Not P1 sewing, complete SM channel classification, original measurement, or a universal process.
Read the exact result, assumptions and evidence
Result
For the previously defined SM covariant family Phi o Ad(aP_CC+bP_CW+cP_WW) with unit phases, Tr(P5J)=|a+4b+c|²/6+|a+b|² and covers exactly [2/3,10]. This is not the global range of all SM covariant channels. The choice a=-1,b=1,c=(1+2i sqrt2)/3 has the same P5 value 2 as the old Psi channel, but P45 values 16/3 versus 4. Both preserve original populations; one Choi response does not identify the entire process under these conditions.
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 five-slot exterior source with retained complement index
V=C5 with given oriented unitary slot basis and volume form,H=Lambda²V. C_m[kl,ij]=epsilon(m,i,j,k,l) are five distinct linear maps to conjugate target;their coherent sum is a different operation. Inner products and CAR grading remain explicit. No physical record,coupling or time iteration assumed from exterior algebra alone.
Fixed three plus two mark and typed original degree clock
V=C5,P rank3 color projector,G_P=S(U3xU2),X=(-2,-2,-2,3,3),original U5=exp(2pi iX/5). Literal slot cycle c=(01234) is distinct and moves P. Covariant transport over Gr(3,5) concerns different marks,not full SU5 covariance within one fixed marked instrument. Continuous marks are not six old outer event marks or135 D8 frames.
Entire class of fixed finite one-step CPTP channels with the specified full populations, without SM covariance, derived P1 Choi identification, or multitime process. No physical no-go.
Read the exact result, assumptions and evidence
Result
Among all CPTP channels in the fixed given 10 to 10 dictionary with all 100 Petersen transition probabilities, Tr(P5 J) ranges exactly over [0,10]. The original Hodge channel attains 10. Dm obtained from Cm by flipping three signs is HS orthogonal to all five Cn, preserves each Kraus effect and all 100 populations; J0=(1/3)sum |Dm>><<Dm| is CPTP and unital and attains 0. Since 0<=P5<=I and Tr J=10 and mixtures preserve populations, all intermediate values occur. The concrete J0 is not SM covariant by an exactly checked SU3 commutator.
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 five-slot exterior source with retained complement index
V=C5 with given oriented unitary slot basis and volume form,H=Lambda²V. C_m[kl,ij]=epsilon(m,i,j,k,l) are five distinct linear maps to conjugate target;their coherent sum is a different operation. Inner products and CAR grading remain explicit. No physical record,coupling or time iteration assumed from exterior algebra alone.
Conditional actual embedding into supplied graph quantization,not original P1 selection. Reuse earlier theta law; neutral KMS alone remains weaker. Delta is not thermal mean charge. CAR direct decomposition gives graded tensor-product state,not direct sum of densities. Entire NS-cover identity does NOT follow from Spec(-A_alpha)=Z+1-alpha:its map reverses support;original u_cov=[[0,u_base],[I,0]] exchanges quarters whereas u_base I_F preserves grades. Already [B_cov,u_cov]=u_cov versus[2h0,u_baseI]=2u_baseg. Abstractly transported winding is not thereby the actual original local multiplier/deck operation. Iff and averaging theorem assume constant Phi,fixed e,p,beta;not complex eta/Pfaffian measures,variable profiles or quantum bosons. Full interacting TFPT is NOT required to preserve old free source exactly. No complete physics,EM or4D derivation.
Read the exact result, assumptions and evidence
Result
For fixed local V_e f=f tensor e in the given Clifford graph,Phi e0 gives full H1/Borel/CAR/graph/product-reflection/time intertwining with the SAME QUARTER time. Actual original maps obey B_Sigma W_alpha=4pi W_alpha A_alpha and B_cov W_alpha=2 W_alpha A_alpha; W1/2 gives the entire graph at ell2pi,beta4pi without fit. Unchanged eightfold gives8 directsum A_mu,mu_a=(a+alpha)/8,beta_fold32pi and already existing full theta charge law. Delta_a=mu_a-1/2 is transported old reference correction. New exact result for all constant oddPhi: for p=k+alpha nonzero,n_e(p)=1/2[1-p<e,tanh(beta sqrt(p²+Phi²)/2)/sqrt(p²+Phi²)e>]. Strict monotonicity of tanh(cx)/x proves n_e(p)>=n_beta(p) for p>0,reversed for p<0,equality IFF Phi e0. A single occupation is thus equivalent to the entire fixed scalar source/time map. Positive classical averaging reproduces it only for Phi e0 almost surely.
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.
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.
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.
Original quarter CAR source with fixed fold and current dictionary
The already supplied single-channel CAR source with actual quarter domains alpha=1/4,3/4, negative-D sea, positive original excitation time, unitary eightfold F and actual channel diagonalization is fixed. M,O,U+ and the conformal NS point-splitting reference are the same original dictionary data; the single delta counterterm follows from the kernel difference. Even CAR current composites retain full arc correlations, charges, domains, all modes, original time and the existing subtraction prescription including finite derivative counterterms. No E8 root/spinor extension is assumed for this neutral current subalgebra. Identity with the original P1 net, Theta, collar and reference sector is not supplied. Real profiles and pulse strengths are intervention data.
Fixed local quarter channel in a constant odd source coefficient
Given the existing Clifford graph source h=A_alpha g-i g Phi with A_alpha=-i partial_theta+alpha,alpha1/4 or3/4,Hermitian involution g and constant selfadjoint odd Phi. Compare fixed local map V_e f=f tensor e,g e=e,unit e,at fixed beta>0 and identical momenta/references. Original elliptic comparison uses actual W1/2 normalization,beta4pi and unchanged fold/normal-ordering reference. If classically averaged,a positive probability law on such constant Phi with fixed e,p,beta is explicitly supplied. This describes neither complex Pfaffian weights,moving field dictionaries nor general quantum-boson families.
New content is the concrete global v252/P2 dictionary and actual Phi test. Basic spinor-CAR level4 was already finding:joint-spinor-not-source-coefficient and is not rediscovered. Full Spin10 can be transported to v252,but is neither implemented there nor derived as physical source symmetry. A charged invariant ray is not a neutral fixed vector;sigma eigenvalue1 is stronger than ray invariance. Sterile neutral line carries source-clock charge but Y0,not automatically physical EM readout. No derivation of Ynu,MR,physical family clock,E8_1 source identity,4D or full solution.
Read the exact result, assumptions and evidence
Result
On the full real gauge lift,det(pi(u))=(lambda det(m))^4 per generation. On the connected unimodular branch,gamma_F=+ is exactly Q_L,L_L,u_R^c,d_R^c,e_R^c,nu_R^c with original SM charges. An explicit unitary map to 1,c_c wedge w_a,epsilon_cjk c_j wedge c_k,w1 wedge w2,epsilon_cjk c_j wedge c_k wedge w1 wedge w2,vol_c wedge w_a intertwines the ENTIRE S(U3xU2) action with Lambda_even(E3+E2),including global Z6 form and opposite action. Three generations use W tensor I3. With an additionally supplied sigma=(123),eigenvalue1,the unique SM-neutral fixed line is e=nu_R^c tensor s,s=(1,1,1)/sqrt3. Actual coefficient gives Phi e=nu_R(MR s)+nu_L^c(barYnu s); preservation iff MR s=barYnu s=0. Reuse existing level4 result concretely for actual Y: tr16Y²=10/3 versus D5_1 basic norm5/6,three-family ratio12. Rescaling to match levels changes Ward charges.
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.
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.
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.
The common mathematical field/covariance/reflection/time diagram is closed within the already assumed canonical Clifford graph type. R acts antilinearly and MULTIPLICATIVELY on CAR; an antihomomorphism is a different type and already fails an even occupation word. Odd words require fixed parity twist; untwisted odd RP is not claimed. Normal HS representation needs the stated free thermal class; separate Wick proof needs no trace-class presentation. rho(h_Phi) is not identified with old scalar NS/QWZ density;already h0=A gamma_F is not A tensor I. The inverse-time gap from annihilator labelling is repaired in the preferred creation chart and is not an open problem of this graph type. Original P1 selection,physical insertions/references/domains,quantized bosons and old-source identification remain separate. No RP for arbitrary normal-dependent bosonic families from the constant proof,no 4D/species-count/physical total closure.
Read the exact result, assumptions and evidence
Result
For the existing normal-independent B=Z A-S Phi,F=S tensor gamma_F is the already present product-reflection factor. With Cfaces=(C0,-C0) and R=faceswap tensor F,Ical F=-C0,R G R=G,and the exact real crossing kernel is -i M with positive M. Actual face-Wick ordering is an invertible basis; its Gram blocks are (-1)^{n(n-1)/2}(-i)^n Lambda^n M. Every even n has factor+1,so RP holds on the ENTIRE bounded even CAR algebra. The natural full creation map iota c=a_R*(v0)-a_L*(v1)+a_R(w0)-a_L(w1),with annihilators antilinear in w,has exactly G(h)=[[1-C,X],[X,C]] at beta=2ell. In the corresponding normal thermal HS representation,J_R=(P_even+iP_odd)J_HS implements both geometric field phases. The same entire chart obeys iota(c(exp(t Ical B)u))=U_t iota(c(u))U_t* with THE SAME t,including cyclic GNS closure. No spectral conjugation or inverse time is needed. The even reflection form is ||rho^(1/4) A rho^(1/4)||_HS². Source H=sum |lambda_j| n_exc is positive with finite thermal heat traces; full HS time is the two-sided Liouvillian L_H-R_H. The normalized sech midpoint kernel does not obstruct positive heat evolution at finite ell.
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.
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 finite SM representation with symbolic Yukawa inputs
Use only the existing v252/v254 representation with C⊕H⊕M3, already supplied color/weak modules and four symbolic complex3×3 Yukawa blocks. No physical values are chosen or fitted. Classify the particle LR one-form block; no proof of the full real96-dimensional fluctuation with antiparticles, JAJ and Majorana sector is claimed.
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.
This replaces the prior normal-independence restriction by a broader explicitly fixed product type without redefining the old premise. No arbitrary unbounded Cauchy problem: continuum claims concern actual elliptic Cauchy data,Green form and compatible domains. No moving grading/normal without connection terms. Positive conditional-state integration generally gives a mixed,nonquasifree state; no Wick rule for averaged covariance or projector purity is required. A complex eta/Pfaffian density gives only the integrable algebraic identity. No derivation of measure,physical quantization,original reflection positivity or physical time.
Read the exact result, assumptions and evidence
Result
For B(r)=Z tensor A(r)-S tensor Phi(r),with fixed even connection,odd selfadjoint coefficient and fixed normals/grades,E remains background-independent and B(r)E=E h(r). In a compatible finite regulator,K'= -B(r)K gives exactly C0 K C0=(K*)^-1,without commutation at different r. Thus Cfaces sends the entire graph to its orthogonal complement and the oriented two-face chart gives P_K -> P_Kplus directsum(I-bar P_Kplus),including all crossing blocks. The same fixed algebra map transports all existing integrable joint bosonic insertions and conditional CAR words under an already given common measure. An exact smooth ordering countercase disproves the wrong unadjointed K^-1 formula.
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.
Fixed graded normal-dependent classical source family
Assume fixed normals N,fixed gamma_F and fixed product trivialization,smooth selfadjoint even A(r),odd Phi(r),Ical=i_old Z gamma_F and C0=i_old N. A compatible finite regulator preserves these identities and adjoints; alternatively supply actual closed elliptic Cauchy data with Lagrangian Green form and grading invariance in the continuum. Normal dependence is an explicit extension of the old constant-product premise. State conclusions assume actual Clifford graph quantization per background. Only the additional integrated-moment identity takes an already given common bosonic weight and integrability as inputs; they are not presumed derived from P1.