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.
Conditional complete channel classification at fixed carrier,not proof that P1 supplies full SU5 event covariance. General commutant method is known primary literature;concrete rigidity checked here. No physical time inferred from channel powers.
Read the exact result, assumptions and evidence
Result
Actual dual Choi representation splits multiplicity-free5+45+50 with explicit projectors. All25 gl5 actions,Casimirs24/5,64/5,84/5,and one highest-weight line per sector checked. All covariant CPTP Choi are sum p_d(10/d)P_d. Zero stay forces p50=0,zero intersect p45=0,hence T=Phi including phases. Within exact covariant class,total stay/intersect leaks s,o give p50=5s,p45=3o/2-9s/2 and exact diamond distance3o+s. SM plus actual carrier wedge fivecycle would generate full SU5.
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.
Specified full SU5 covariant channel with Petersen support
H=Lambda²C5 in given oriented unitary duad basis,target dual H. T is CPTP and T(R rho R*)=barR T(rho)barR* for R=Lambda²U,U in SU5. Basis transitions to same or intersecting duads vanish. This is explicitly a mathematical conditional premise,not assumed physical P1 event covariance.
Closes algebraic origin of full Hodge/Petersen channel as mathematical inclusive response of same given E8 source. New50s are not old64s;family5 restricts to oldA3=4+1,not new physical generation count. Joint tensor chart instead of raw coordinate trace. Z5 center not automatically original C5/Galois/Coxeter/physical clock. P1 selection of exactly these50 insertions,their record,state and time iteration is not proved by bracket alone.
Read the exact result, assumptions and evidence
Result
Fixed carrier A4 inside D5 has exactly20 centralizer roots in same E8 with derived A4 Cartan matrix. Four50 sectors give (5,10),(10,5bar),(10bar,5),(5bar,10bar). Actual bracket(5,10) tensor(10,5bar)->(10bar,5) has50 rank12 Kraus B_mab=C_m tensor A_ab. One joint cocycle chart satisfies600 bracket edges plus1500 neutral A4+A4 action edges,including fixed dual Hodge signs. Gain12I50,normalized response Phi_Petersen tensor WH5,WH5=(Tr sigma I-sigma^T)/4. For all correlated inputs,reduced carrier response is Phi,without3/5 conditioning. All600 original P2 X charges satisfy qout+qenv=qin with dual target and qenv=-X_m.
Required assumptions
Given full E8 current source with fixed carrier SU5
Actual weight-one E8 Chevalley source from tfpt_explorer.current_block_geometry._actual_current_source and v498. Given D5/A3 frame uses first5/last3 standard coordinates. Carrier SU5 inside D5 has roots e_i-e_j,i,j<5. Retain full E8 source,cocycle,compact form and group actions. Physical P1 realization of this already given current source is not assumed proved.
Specified inclusive current response with invariant metric
For an explicitly specified irreducible insertion sector and input/output modules,let B_a be actual current brackets in Killing-orthonormal basis. If sum B_a*B_a=kI,E(rho)=sum B_a rho B_a*/k denotes mathematical inclusive response with unread insertion index. Reduced response uses tensor chart transported by group action. This defines tested reader,not asserted selection of physically executed P1 instrument or original time.
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.
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.
No raw bitbasis partial trace:product phase gauge absent there;full group action must transport. No unconditional A/3 onLambda² and no old stay2I/5. Internal Clifford action on bosonic weight-one current states does not supply spacetime fermion fields. Actual P1 event/time selection from this reader remains open.
Read the exact result, assumptions and evidence
Result
In D5+A3 frame:60 g2=(10,6) root brackets g1=(16,4)->g3=(16bar,4bar),gain15I64. All112 D8 root actions/3584 sign equations and all960 nonzero g2 columns match CAR in joint cocycle chart. Normalized response factors Q5 tensor Q3 with Q5=(1/5)sum(a rho a*+a* rho a),Q3 analog1/3. Reduced carrier theorem also holds for correlated input. Lambda² sends3/5 toLambda³ (Petersen A/5 after duality) and2/5 toLambda¹ as genuine carry. Full Fock population isQ5 cube,antipodal quotient already known Clebsch16 of v810.
Required assumptions
Given full E8 current source with fixed carrier SU5
Actual weight-one E8 Chevalley source from tfpt_explorer.current_block_geometry._actual_current_source and v498. Given D5/A3 frame uses first5/last3 standard coordinates. Carrier SU5 inside D5 has roots e_i-e_j,i,j<5. Retain full E8 source,cocycle,compact form and group actions. Physical P1 realization of this already given current source is not assumed proved.
Specified inclusive current response with invariant metric
For an explicitly specified irreducible insertion sector and input/output modules,let B_a be actual current brackets in Killing-orthonormal basis. If sum B_a*B_a=kI,E(rho)=sum B_a rho B_a*/k denotes mathematical inclusive response with unread insertion index. Reduced response uses tensor chart transported by group action. This defines tested reader,not asserted selection of physically executed P1 instrument or original time.
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.
Outcome-dependent phase averaging before forgetting m,not one phase channel after coarsening. K4 is actual tested projective four-group,not automatically cyclic C4 clock. Proof in fixed event-label chart,without physical Bell10/Lambda²5 or SU5/native group identification. Classically merging20 outcomes does not restore lost coherences.
Read the exact result, assumptions and evidence
Result
For each of6 marks,old20 jump events group into5 blocks of4 with Hodge effectP_m/3 and same basis movement. Exactly R_l=D_l C_m onP_m;relative to baselineD0,H_l=D_lD0* form projective K4 with3 characters each multiplicity2. Psi_m=(1/4)sum Ad(H_lD0) after Phi_m. New/old Choi ranks peroutcome1/3,total5/15;superoperator ranks100/40. All60 ordered intersecting-duad coherences permark distinguish channels. No common10-label diagonal gauge for all5 baselines:complete finite test0 solutions permark.
Required assumptions
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.
Specified old J20 instrument in fixed six-mark duad chart
Actual twenty jump events U_l(I-D_l) per mark from compiler-correlated-event-clock-20260919/source_channel.py;J20 effect3I/5,normalized jump channel Psi=(5/3)J20. Retain common duad labels of ten basis states. Comparison chart does not provide linear SU5/native group identification of Bell10=Sym²C4 with Lambda²C5 or already selected P1 apparatus.
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.
Previously excluded single coherent sum C_v remains excluded as Kraus normalization;five events change premise. Fermionic reduction channel is known mathematics;new result is concrete TFPT source/record/rate connection. Same three values identify neither all100 quantum directions with3D family space nor physical time or initial state.
Read the exact result, assumptions and evidence
Result
C_m²=P_m of rank6,sum P_m=3I10. Phi=(1/3)sum Ad(C_m) is CPTP,unital,HS selfadjoint;population exactly A_Pet/3 without time or filter,Choi rank5 with eigenvalue2^5,superoperator rank100. Correct covariance connects10 and10bar. Actual24 is dGamma(sl5),Phi(dGamma A)=-(2/3)dGamma(A)^T. On End10=1+24+75,Phi²=Pi1+4/9 Pi24+1/9 Pi75,so Phi^6 spectrum1^1,(64/729)^24,(1/729)^75. Actual radial restriction on Petersen shells1,3,6 yields previously transported P. As specified channel,Phi has unique stationary density I10/10.
Required assumptions
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.
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.
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.
New exact Born-magnitude bridge and conditional population matching. No equality of full instruments or P1 derivation of measurement basis,time,acceptance or reset rule. Linear sign obstruction explicitly does not imply general exclusion of quantum-probability derivation.
Read the exact result, assumptions and evidence
Result
Entrywise |C_ef|²=A_Pet[e,f]. For x=cos(sqrt5 t),U(t)=exp(-itC) has exact population values p_diag=(2+3x)²/25,p_edge=(1-x²)/5,p_nonedge=(1-x)²/25. Thus no full U(t) population is pure Petersen transition. At t*=(pi/2+k pi)/sqrt5,added edge filter yields existing subnormalized jump block A_Pet/5 with probability3/5. Reject is4/25 at input plus1/25 at each of six nonneighbors,not old stay block2I/5. Conditioning on change gives A_Pet/3 in short-time limit. C/sqrt3 is not Kraus;C/sqrt5 has rank6 projector effect rather than3I/5 and superoperator rank36 versus actual J20 rank40. Six actual J20 phase matrices gauge to -A_Pet,not C.
Required assumptions
Oriented five-slot Hodge candidate with explicit basis readout
Ordered orthonormal basis e0,...,e4,its volume form and v=sum e_i. On Lambda²C5 consider new mathematical candidate C=*(v wedge .). Conditional Born test explicitly sets two-words as measurement basis,U(t)=exp(-itC) as generator ansatz and input-label-dependent disjointness filter. These readout data and choice of C are not derived physical P1 rule.
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.
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.
Exclusion of precisely specified single-face inclusion;not every source-derived invariant shell inclusion. Same formula2P-I or minus sign identifies neither spaces nor actions. The reviewed responses remain external proposals;no automatic proof acceptance or source-time change.
Read the exact result, assumptions and evidence
Result
For Pi=[[I-C,X],[X,C]],Pi is rank3 orthogonal projector on six-space. Natural single-face compression C has eigenvalues{1/2,4/13,1/10},hence rank3,not a projector and not rank1 Perron projector. I-C also has full rank. Seven rational checks establish counterexample to The reviewed proposed identification in natural finite comparison. Two actual The reviewed Opus4.8 consultations retained with corrections;The reviewed retracted five false time/state/grading claims of first round.
Required assumptions
Natural single-face inclusion in the given family Calderon graph
Given positive invertible M of v486/v487 family recursion;C=M²(I+M²)^-1,X=M(I+M²)^-1 and Pi=[[I-C,X],[X,C]] on doubled six-space. Tested inclusions are the two coordinate faces. No geometric P1 shell space or its embedding is thereby derived.
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.
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.
Marked spin transport and existing two-object vertex functor. Full open P1 amplitude functor,its determinant line and identification of U_Gamma with normal spin transport remain to derive. No identification of group orders or two-object set with physical spacetime.
Read the exact result, assumptions and evidence
Result
alpha01=T,genuine reversal T^-1,continued positive quarter alpha10=beta0 T^-1. Hence alpha10 alpha01=beta0 and alpha01 alpha10=beta1,whereas forward/reverse yields1. Normalized central cocycle omega(1,1)=beta describes nonsplit1->C4->C8->C2 over mu4,with correct adjoint and defect-line dualization. Positive local spin quarter lift squares to+i independently of lift sign,matching marked q norm factor. Literal unextended D4 reflection s²=1 cannot map to alpha²=beta.
Required assumptions
Marked oriented quarter spin and two-object vertex transport
Positively oriented marked quarter turn z->iz of normal two-plane with Spin(2) lift a=+/-exp(i pi/4),a²=i; existing genus2 source (C,S0,Dq,Q) and selected beta; existing lattice vertex objects F0,F1,unitary T:F0->F1 and beta1=T beta0 T^-1. Continued oriented quarter step and geometric reversal remain distinct arrows. An open P1 amplitude functor 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.
New joint interpretation of existing clock shift and already known charge census. No rediscovery of old ground doublet or D8/E8 Coxeter grading claim. Q is source U1,not automatically electromagnetic charge. p* is an E7 root,not E7 singlet. No time generator changed.
Read the exact result, assumptions and evidence
Result
With rho_A7=(7,5,3,1,-1,-3,-5,-7)/2 and q=(1,...,1),exactly delta=-rho_A7/8+(2a-1)q/16 and H8=8L0-rho_A7.a0+(2a-1)Q/2. p*=(++++----)/2=omega4(A7) has norm²2,Q0,rho.p*=8 and is unique neutral E8 root of H8 grade0. The126 neutral roots form E7(q/2),exactly56 A7 roots plus70 Lambda^4C8 weights. All240 roots and reflection closure checked exactly.
Required assumptions
Four D8 source modules with fixed affine time
Mathematical parent of the four D8*/D8 modules 0,v,s,c with eight identical Heisenberg oscillators, source charge chart p and N≥0. H=8(N+|p|²/2+delta.p),delta_j=(j+a)/8−1/2,0<a<1,Q=sum p_j. Original quarter cases are a1/4,3/4. Conformal L0, individual Cartan charges and totalQ remain distinct. This mathematical completion does not assume a physical P1 realization of the Ramond space or a local field map.
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 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.
Complete finite operator comparison,stronger than sixth-power or spectral agreement. Z already occurs in v409;identification on the same source with v487 and geometric deck remains open. No fixed electromagnetic charge conservation,physical Hamiltonian or identification of K²=1 with full spin lift alpha²=beta.
Read the exact result, assumptions and evidence
Result
P is selfadjoint on H_pi with eigenvalues1,-2/3,1/3. Marked isometry W identifies |P| with M and sign(P) with K=Z Delta,Z=diag(1,-1,-1). Thus WPW^-1=KM and WP^(2n)W^-1=M^(2n);W_n=K^nW identifies each step in a moving frame. Bipartite double admits fixed six-dimensional intertwiner with transported deck tau tensor K. Simultaneous positive M and literal Delta identification is impossible on simple2/3 eigenspace. Y transports but [Y,P] has rank2:raw Frobenius square125,isometric moving-frame700/9. A physical charged total process needs actual compensating transfer.
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.
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.
Implementation repair and exact finite recursion identities. v395 matrix comparisons themselves numerical; rational identity derived separately. E8 Cartan,P2 and scheduler remain given inputs;no quantum-field or physical-time origin. Paper sources and local website copy corrected;full publication audit failed on previously retired registry files,no published overall completion.
Read the exact result, assumptions and evidence
Result
Old _micro_step overwrote T_net@m during family update; old passing test never called it. Integrated fix computes T_net@m@M.T and checks all27 basis inputs through actual function. Existing v486/v487 M replaces incomplete v327 rule:spec M={1,2/3,1/3};O^T M^6 O=diag(1,64/729,1/729). One hand is N C^6=T_net tensor M^6,not (NC)^6. Normal and -OO6/6 with identical output;independently reviewed. McKay Doob transform with existing marks d gives P_ij=(A_ij+2delta_ij)d_j/(4d_i),reversible pi_i=d_i²/120.
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.
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.