TFPT scientific source excerpt Original repository path: experiments/theory-contracts/original-local-source-variable-background-20261102/ORIGINAL-TIME16-EVALUATION.txt Original file SHA-256: fcf192141afdcbef2a94e880f6d1d76491a9a6dd7e386f636d670a64a296c1d8 Inclusive original lines: 1-165 Line numbers below refer to the original source. This bounded excerpt is source evidence; it is not a new proof/checker run. Conversation metadata and personal execution details are omitted where indicated. 000001 | R106. Executed time evolution on the actual sixteen original CAR fields 000002 | 3 November 2026. Native execution and source attribution, not a new parent. 000003 | 000004 | REQUEST AND PRECISE OUTCOME 000005 | 000006 | [OMITTED: non-scientific conversation or execution metadata] 000007 | [OMITTED: non-scientific conversation or execution metadata] 000008 | [OMITTED: non-scientific conversation or execution metadata] 000009 | [OMITTED: non-scientific conversation or execution metadata] 000010 | [OMITTED: non-scientific conversation or execution metadata] 000011 | 000012 | The different primitive H_adm reconstructed from the common S/Z has not 000013 | been evaluated on these16 fields: the cited seed/OS statements provide its 000014 | definition/existence but not that field/transfer intertwiner. This is an 000015 | explicit uncomputed quantity, not a zero or a secretly substituted parent. 000016 | The saved native JSON records primitive_H_adm_evaluation with null matrix 000017 | element and status not_computed_unidentified_original_field_transfer_map. 000018 | 000019 | All G/H/I/J and R104/R105 results remain. J already analytically established 000020 | the whole R104 chart and distinguished additive versus flat time. This 000021 | execution applies those original formulas to the native65536D carrier and 000022 | evaluates their exact number-charge coefficient and all sixteen field laws. 000023 | It is not counted as a new derivation of the physical parent or of P1. 000024 | 000025 | 1. ACTUAL ORIGINAL SOURCE CALLS AND DATA 000026 | 000027 | v1002_spin10_mirror_projector.py supplies all16 native c_i, P_phi and 000028 | theta=pi/7. Its original local parent is Q=I-P_phi, unit gap. 000029 | v1013's literal table supplies the DIFFERENT coefficient2Q. 000030 | v1027_signed_det_car_wall.py:82-153 gives the original canonicalization 000031 | U and a_i=Uc_iU*, N_a=sum a_i*a_i, with Q<=N_a<=nQ. It explicitly says 000032 | Delta N_a is not Delta Q. Its finite dense control is n4 and theta0; 000033 | its proof is the same even-n conjugation rule. We use that rule on the 000034 | actual native n16, with the already specified v1002 phase. We do not call 000035 | this a preexisting n16/pi7 dense code run or claim phase selection. 000036 | 000037 | For F=|full><0|, P0=|0><0|, PF=|full>0, 000058 | 000059 | =-8 Delta exp(i theta), 000060 | <0|H_add|0>==8 Delta, 000061 | =Delta. (3) 000062 | 000063 | For the actual v1013 flat parent H_flat=2Q, 000064 | =-exp(i theta), 000065 | <0|H_flat|0>==1, 000066 | =2. (4) 000067 | 000068 | Both original rules therefore have an actual charge16 transition. They 000069 | do not give the same coefficient or the same diagonal hierarchy. At a 000070 | common one-particle gap Delta2, their charge16 amplitudes differ by16 000071 | and ||2N_a-2Q||=30. At unit coefficient ||N_a-Q||=15. 000072 | 000073 | The whole exclusion does not depend on choosing Delta2: on k dressed 000074 | excitations H_add has energy Delta k, while H_flat has energy2 for every 000075 | k>=1. Matching k1 fixes Delta2; then k2 gives4 versus2. No positive common 000076 | clock rescaling or additive energy constant fixes both once the common 000077 | ground energy and actual relative normalization are retained. This is 000078 | the original explicit parent distinction, now actually executed, not a 000079 | new global exclusion of other original TFPT sources. 000080 | 000081 | 3. REAL-TIME UNITARY EVOLUTION OF ALL SIXTEEN FIELDS 000082 | 000083 | Use the original Heisenberg convention alpha_t(O)=exp(itH)Oexp(-itH). 000084 | For every native bare field c_i, P c_i P=0. Exact spectral multiplication 000085 | gives 000086 | 000087 | alpha_flat,t(c_i)=c_i+(exp(-2it)-1)P c_i 000088 | +(exp(2it)-1)c_i P. (5) 000089 | 000090 | For every original dressed field a_i, a_i P=0, hence 000091 | 000092 | alpha_flat,t(a_i)=a_i+(exp(-2it)-1)P a_i, 000093 | alpha_add,t(a_i)=exp(-i Delta t)a_i. (6) 000094 | 000095 | Equation(5) is on the SAME old c fields, not just on renamed a fields. 000096 | The routine computes both full unitary matrices sparsely and verifies 000097 | (5) for all16 c_i, then(6) for all16 a_i. Maximum entry errors are 000098 | 3.926e-17,5.552e-17,9.551e-16 respectively at diagnostic t0.31,Delta2. 000099 | The proof is spectral for every real t; sampled time only checks code. 000100 | 000101 | The original nonlinear flat term retains multiparticle information. The 000102 | attempted linear law [2Q,a_i]=-2a_i holds on the one-excitation-to-vacuum 000103 | transition but fails on two-to-one: mode0 residual norms are approximately 000104 | 3.109e-17 and exactly2 in those two original sectors. 000105 | 000106 | For i!=j, |ij>=a_j*a_i*|phi> is normalized. Its actual ordered four-field 000107 | amplitude is 000108 | =exp(-2it), 000109 | =exp(-2iDelta t). 000110 | At t0.31,Delta2 the latter is0.3247962844-0.9457839994i and the former 000111 | 0.8138784567-0.5810351605i. They are amplitudes, not probabilities. 000112 | Their different phases are a direct whole-source word mismatch. 000113 | 000114 | 4. EUCLIDEAN WORDS AND Z0, KEPT DISTINCT FROM REAL TIME 000115 | 000116 | The same four-field Euclidean amplitudes at s0.31,Delta2 are 000117 | exp(-4s)=0.2893842179 for H_add, 000118 | exp(-2s)=0.5379444376 for H_flat. (7) 000119 | The actual complete zero-source cluster traces are 000120 | Z_add(beta)=(1+exp(-Delta beta))^16, 000121 | Z_flat(beta)=1+65535 exp(-2beta). (8) 000122 | At diagnostic beta1,Delta2 these are7.6205471889 and8870.1977869114. 000123 | No beta, energy normalization or physical temperature is selected. 000124 | 000125 | The report also records selected old-c inverse-heat conjugation entries. 000126 | They are explicitly named euclidean_conjugation, not unitary Heisenberg 000127 | evolution. Large inverse-heat entries are not a real-time instability. 000128 | The real-time matrices, field laws and complex words are checked separately. 000129 | 000130 | 5. WHY THIS IS NOT YET AN EVALUATION OF PRIMITIVE H_ADM 000131 | 000132 | The relevant original Boundary002:78-83 states the reconstructed admissible 000133 | Lorentzian group alpha_t(O)=exp(itH_adm)Oexp(-itH_adm), under the later 000134 | carrier fluctuation/admissibility hypotheses. Lines103-143 define the 000135 | operational seed as (A_loc,tau_t,Theta,omega,[u_Sigma],D_coll); tau_t is 000136 | part of that supplied structured object, not a numeric sixteen-field 000137 | matrix manufactured from c3 alone. 000138 | 000139 | Original QFT008:215-254 defines H_adm through the complete OS Schwinger 000140 | family and time translations. That reconstruction is a real source 000141 | definition, not an explicit coefficient on the v1002 000142 | mirror fields. The particular native c_i/field-intertwiner is not assigned 000143 | in these cited passages. The internal sixteen-dimensional spinor is not 000144 | itself a complete Fock/field/time correspondence. 000145 | 000146 | The original neutral Q0 current generator is already explicitly evaluated 000147 | and its vacuum/BW source is solved. It is not identified with these sixteen 000148 | mirror insertions. J's whole U_det R104 map likewise starts with H_flat 000149 | and transports it. It does not provide an independent primitive generator. 000150 | Reading either as that missing primitive H_adm would answer a different 000151 | question by relabeling existing results. No such relabeling is made here. 000152 | 000153 | Consequently the strongest actual computed verdict is: 000154 | - native v1002/v1013 supplied DET time: exact equations(4)-(8); 000155 | - original v1027 canonical number rule: generates(2)-(3), NOT2Q; 000156 | - primitive S/Z OS H_adm on the SAME c_i: not computed, its original 000157 | field/transfer assignment is not furnished by the cited source chain. 000158 | 000159 | It is not legitimate to replace that last entry by zero, the number parent, 000160 | a bare Dirac matrix or the already supplied DET parent. Nor is this a 000161 | proof that no such map occurs elsewhere in the corpus. It is the precise 000162 | boundary of the requested evaluation with these actual original inputs. 000163 | No fundamental solution or physical impossibility has been established. 000164 | All prior52 scoped completions,G/H/I/J,E8/clocks,state/time/RP,memory and 000165 | solved Yukawa/flavor/alpha remain. No paper/ledger/Lean promotion.