TFPT scientific source excerpt Original repository path: experiments/theory-contracts/historical-dynamics-source-recovery-20261103/HISTORICAL-ORIGINAL-FIELD-MAP-AND-CURRENT.txt Original file SHA-256: 00518f3e9908e21ea425bd8caa79f926d63d7b6e7924b601d4d17da2edb096e9 Inclusive original lines: 1-55 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 | HIST20261103J. Original field map, Hodge transport and actual common current. 000002 | Anonymized source derivation, 3 November2026. 000003 | 000004 | 1. FIRST ORIGINAL FIELD IDENTIFICATION ACTUALLY READ 000005 | J25-TRACE is the earliest recovered source, original raw-content SHA256 000006 | 289b6dc582e800a59391fed6c41604a47915378d28258ec8e9cec9b8d8dd1ab2. 000007 | It explicitly proposes T^{mnr}=d^{[m}(phi*g^{n]r}) and calls this 000008 | "totally antisymmetric torsion". This is the original proposed field 000009 | identification, not a newly invented comparison model. 000010 | Its complete antisymmetrization is identically ZERO, because g is 000011 | symmetric in the last two slots before the first antisymmetrization. 000012 | Thus epsilon*T=0: the stated map has no axial torsion component. 000013 | 000014 | On a constant orthonormal frame, or for the metric-compatible covariant 000015 | version of that expression, set v=dphi and unit-weight antisymmetrization: 000016 | T_vec_mnr=(v_m*g_nr-v_n*g_mr)/2. 000017 | Then T_vec_mn^n=3v_m/2 and T_vec^2=3v^2/2 in4dimensions. 000018 | This is the trace sector, not the axial sector of P25-L:136,155. 000019 | The original partial derivative also needs an actual covariant-field map 000020 | before being treated as a tensor away from its chosen frame. 000021 | 000022 | 2. ACTUAL CANDIDATE DUAL MAP, INCLUDING ITS NORMALIZATION 000023 | Using the SAME supplied Lorentz metric and orientation, define the Hodge 000024 | star on the first two indices: (*T)_mnr=epsilon_mn^ab*T_abr/2. 000025 | Direct contraction gives 000026 | *T_vec_mnr=-epsilon_mnrs*v^s/2. 000027 | Therefore the exact mathematical bridge to the written P25-L contorsion 000028 | K_ax=epsilon*S/2 is K_ax=-*T_vec with S=v. 000029 | If the coordinate convention is T_ax=2K_ax, then T_ax=-2*T_vec, not just 000030 | T_ax=T_vec. The relation to P25-L's auxiliary equation would additionally 000031 | transport dphi=(lambda*kappa^2/3)da and all actual normalizations/periods. 000032 | The numerical old phi0 cannot be imported without that actual field chart. 000033 | 000034 | This is a nontrivial field dualization: (*T)^2=-T^2 on these Lorentzian 000035 | two-form slots. Kinetic terms, source couplings, parity/reflection, measure, 000036 | contour and reference must be transported. It is not a symmetry of the 000037 | old/new actions by declaration. In particular a beta*(dT)^2 term remains 000038 | fourth-order in a scalar after the gradient substitution, also after star. 000039 | The factor2 here is a torsion/contorsion normalization, not a resolution 000040 | of the distinct anomaly-matching factor2 without a whole-source map. 000041 | 000042 | 3. THE EARLIEST NOETHER CLAIM AND ITS SMALLEST TEST 000043 | J25-CURRENT, original raw-content SHA256 000044 | 95ad6cbabf6a72cc716b905629fe451196fb5bce16cadf769ef4d808e87cd44d, 000045 | writes J^m=[-Z*d^m phi+(2beta_bar/M_Pl^2)*(Box phi)*d^m phi]*epsilon, 000046 | Z=1+alpha/(2pi^2), and claims conservation only at phi0=1/(6pi). 000047 | For EVERY constant phi=c this written J and its divergence vanish. 000048 | Thus this local current does not select that constant background. 000049 | The source itself says the full higher-derivative Noether term remains 000050 | to be included. For an L(phi,dphi,ddphi), the actual shift current is 000051 | J^m/epsilon=partial L/partial(d_m phi) 000052 | -d_n[partial L/partial(d_m d_n phi)], 000053 | up to improvements and a boundary variation. No missing L is fabricated. 000054 | Global flux/boundary data could impose further conditions, but those 000055 | must be read/evaluated and do not follow from this written local current.