Exclusion only for neutral family currents with unchanged original charge dictionary. No universal TFPT no-go or exclusion of charged insertions, explicit field maps or transported geometry. Prevents equating equal-dimensional spaces.
Read the exact result, assumptions and evidence
Result
Old Bell corner is (10_D5vector,10_A3descendant), weight2 and mu4 class(2,2). P2 Lambda²5 lies in D5 half-spinor paired with A3 fundamental, weight1, classes(1,3)/(3,1). Original Y spectra {±1/3[3],±1/2[2]} and {-2/3[3],1/6[6],1[1]} are disjoint, giving Hom_Y=0. A3 zero modes preserve D5 Y, center and L0, so cannot connect these types. Positive charged A4×A4 bracket remains valid as a different cut of the same E8 algebra.
Required assumptions
Do not identify source types
Observable algebra, OS reflection, state, collar operator, time evolution, carrier connection, family holonomy, and readout are distinct data until an original map relates them.
Given local E8_1 vacuum representation and explicit cocycle
Positive level-one E8 lattice vacuum representation in orthonormal D5+D3 coordinates, declared simple-root cocycle, level-one Heisenberg Ward rules and internal quarter character v=(0^5,1/2^3). Insertions are separated. No raw-P1 pullback or physical time law is assumed or derived from this representation.
Given 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.
Excludes ordinary quartic polarization, existing Hessian family and unchanged purely holomorphic CAR point splitting. Does not exclude mixed-adjoint or asymmetrically differentiated OPE components; new mixed-current representation is unaffected.
Read the exact result, assumptions and evidence
Result
Correct congruences D_m=F_RᵀC_mF_R vanish identically as quartics on S=zzᵀ. Multiplication Sym²(Sym²V4)→Sym4V4 has rank35 and kernel20 with independently checked scalar line and Spin5 five, jointly dimension6. Actual process._code_basis quartics and existing2+2 flattenings have image rank5 and zero intersection with Hodge five. Original holomorphic transport AAᵀ=0 prevents unchanged holomorphic point splitting from lifting the null relation.
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.
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.
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 Pauli and v419 F20 source words
Use frozen v783 two-qubit Clifford generators, existing Pauli16 and central mu8, and actual cyclotomic v419 C5,G matrices. A constructed source-word F20 subgroup is available; its physical seam selection is not assumed.
Counterexample to selection rules in fixed dictionary;not asserted full E8 bracket automorphism,actual OS reflection,or classification of all merely SM covariant instruments. Does not prove fundamental gap is one-dimensional.
Read the exact result, assumptions and evidence
Result
For rank3P,U(P)=-I onCC,+I onCW/WW. T_P=Phi o AdU(P) is full SU5 covariant family overGr(3,5) with dual output,G_P covariant,same population/Choi rank5,but P5 value4/15. S_P=AdbarU(P) o Phi o AdU(P) likewise natural family;in adapted real chart real symmetric Kraus,unital,HS selfadjoint,same5 effects,Petersen population,full spectrum,unique fixedI10/10,but P5 value7/15. Powers similar,not identical. U(P) violates exterior-square phase relation,not carrier torus gauge. Full family covariance plus all listed criteria therefore insufficient.
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.
Only direct bilinear candidate and linear Hodge gauge identification excluded. C_v is not defined as physical operator in v474. No general exclusion of quantum probabilities,quartics,original source or E8. Existing Bell Petersen population process retained,not reinterpreted as source dictionary despite incompatible Sym²C4/Lambda²C5 representations.
Read the exact result, assumptions and evidence
Result
Original bilocal current a_r* a_s changes at most one occupied index and has zero matrix element on all30 directed Petersen edges of disjoint two-words. New natural candidate C_v=*(v wedge .),v=(1,...,1),matches disjointness support exactly,but C_v³=5C_v and chi=lambda^4(lambda²-5)^3. Six of twelve pentagons have negative flux;diagonal phase gauge or orientation does not yield A_Pet. This concerns linear operator equality. Born readout of squared moduli is a distinct specifically tested route and is not excluded merely by this sign result. Existing quartic fields and two-boundary state do not define marked Lambda²C5 compression with weights,compensating charge and time.
Required assumptions
Specified Petersen shells and full finite family recursion
v808: ten two-element subsets of five marked slots, disjointness adjacency and radial P=[[0,1,0],[1/3,0,2/3],[0,1/3,2/3]] on H_pi with pi=(1,3,6)/10 and Y=diag(6,-4,1). v486/v487: M=[[1,0,0],[0,1/2,1/6],[0,1/6,1/2]], deck swap Delta of final two slots. v395: given affine E8 adjacency A,T_net=(A+2I)/4 and given 1:6 scheduler. These finite operators are compared without assuming identification with P1 fields,electromagnetic charge or physical time.
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.
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.
Excludes only full even internal CAR as coordinate algebra with J_H; positive Hodge signs conditional on rank/metric/volume. No physical CAR, J, KO6, spacetime or E=C5 origin derivation. Proper compatible subalgebras and originally derived symmetry breaking remain possible. Whole-space antiunitarity is not automatically the quaternionic W factor of a different triple.
Read the exact result, assumptions and evidence
Result
For the given E=C5, J_H²=1, J_HΓ=-ΓJ_H and (ΓJ_H)²=-1 hold on ΛE. Internal CAR is End(ΛE), its even part End(S+)⊕End(S-). J_H swaps both blocks and maps this full algebra onto itself; order zero would require commutativity. An explicit matrix-unit commutator has rank2. The full internal algebra is thus not a spectral coordinate algebra with this J_H. A selected left/right bimodule subalgebra remains missing. Reuse the existing SU5 no-selector: unmarked exterior algebra and trace balance select no3+2 projector.
Required assumptions
Given unmarked Hermitian rank-five carrier with volume
Given E=C5 with Hermitian metric and unit complex volume, F=ΛE, Γ=(-1)^degree and conjugate-linear Hodge J_H. Neither3+2, named particle/gauge modules nor Yukawas are inserted. Internal Clifford operators are not identified with physical local fermion fields; rank5 and volume are not newly source-derived.
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.