TFPT scientific source excerpt Original repository path: experiments/theory-contracts/original-local-source-variable-background-20261102/WEIGHT-FULL.txt Original file SHA-256: e6776276275e6ceb9db60f60c0f7d9a7f85383c00dd2558a18f84faae2ec1438 Inclusive original lines: 1-167 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 | G: COMPLETE ORIGINAL WEIGHT, GAUGE QUOTIENT AND BEREZIN CALL 000002 | 2 November 2026. Independent relational_logic source review. 000003 | Canonical sources unchanged. Entry live plan85, Atlas babeae99b202b43dfe084d2f. 000004 | 000005 | RESULT 000006 | 000007 | Gauge fixing and ghosts are already presented in the Original as the 000008 | representation of an existing gauge quotient. They are not evidence of a 000009 | new independent physical interaction. The explicit geometric ghost 000010 | operator and physical projector occur in the original research contract; 000011 | the later spectral gravity theorem explicitly uses that same quotient. 000012 | Our earlier WEIGHT.txt wording about an unprinted gauge functional must 000013 | not be promoted into a fundamental missing-coupling claim. 000014 | 000015 | The complete original source, including its given gauge/ghost/Berezin 000016 | weight, is transported directly by the fixed full U, as proved in 000017 | FUNCTOR.txt(10) and REFERENCE-SOURCE-COMPLETION.txt. It does NOT first 000018 | require identification with a separate Gibbs reference state. The latter 000019 | is an optional representation, with its own same-basis conditions. 000020 | 000021 | No new physical structure is selected by this G continuation. Nor do 000022 | the inspected S_adm occurrences define a second competing action. They 000023 | call the given action and differentiate it. The first unsupported 000024 | identification would be replacing that whole original call by the compact 000025 | finite-coefficient spectral readout alone, without its actual geometric/IR 000026 | map. Ghost physics is not that obstruction. 000027 | 000028 | 1. WHAT THE 23 LITERAL HITS ACTUALLY COVER 000029 | 000030 | The supplied full-action-literal-hits.json has23 entries in7 unique files: 000031 | tfpt31/012 particle/compiler:1; tfpt32/011 closure:1; 000032 | tfpt42/023 strongCP:1; tfpt42/035 effective average action:9; 000033 | Source45/carrier009 strongCP:1; Source45/QFT003 strongCP:1; 000034 | Source45/QFT007 effective average action:9. 000035 | The18 effective-action hits repeat terms in the same W_k/1PI expansion 000036 | in two historical copies. The strongCP calls use e^-S_adm as the supplied 000037 | weight. Neither type is a new independent enumeration of its full terms. 000038 | This is the exact coverage of that list, not an all-corpus absence claim. 000039 | 000040 | QFT007:3–26 defines e^W_k by integrating e^(-S_adm-phi R_k phi/2+J phi). 000041 | QFT007:119–143 gives Gamma_k=S_adm+(hbar/2)STr log(S_adm''+R_k)+... 000042 | and vertices S_adm^(n). Thus S_adm is the action supplied to the fields 000043 | still integrated; W_k and Gamma_k are the resulting different callers. 000044 | An already effective/coarse-grained input is still an input at that stage. 000045 | This distinction does not permit adding the same determinant a second time. 000046 | 000047 | 2. THE ORIGINAL QUOTIENT IS CONCRETE 000048 | 000049 | ResearchContract2:15–21 supplies a gauge slice on the stated Sobolev 000050 | metric class and the gauge-fixed gravitational complex 000051 | Omega0(TM) --K--> Gamma(Sym2 T*M) --K*--> Omega0(TM), 000052 | Delta_gh=K* K, Pi_phys=Pi_BRST/Hodge Pi_TT. 000053 | It calls the conformal direction BRST exact/nonpropagating in the stated 000054 | Calderon polarization. This is a geometric gauge-complex assertion, not 000055 | an arbitrary ghost coupling introduced in this review. 000056 | 000057 | Metrology004:35–60 defines Q_geo to quotient diffeomorphism and local 000058 | frame gauge directions and Delta_tot={Q_adm+Q_geo,(Q_adm+Q_geo)*}. 000059 | Its proof at151–162 says the same complex removes pure gauge directions 000060 | from the common Einstein/Higgs/R2/gauge-curvature spectral package. 000061 | StandardModel007:29–32 explicitly identifies the physical sector with 000062 | this cohomology, under the stated Fredholm/APS condition. 000063 | 000064 | Contract008:287–293 gives the relevant existing Ward premise 000065 | =0, 000066 | with the eta boundary phase cancelling the APS anomalies. This is attached 000067 | to that contract's projective-limit/moment/regularity hypotheses. It is 000068 | not newly proved by the existence of a formal nilpotent matrix alone. 000069 | StandardModel007:141–155 likewise retains Ward/BRST in its named source 000070 | hypotheses and carefully limits the all-order EG result to its local 000071 | perturbative matter/gauge scope. 000072 | 000073 | 3. THE SMALLEST DECISIVE GAUGE REPRESENTATION IDENTITY 000074 | 000075 | Apply the existing Ward premise on its legitimate original caller and 000076 | domain. In a BRST gauge-fixed representation S_t=S_inv+s Psi_t, with the 000077 | original measure, eta, boundary conditions and common normalization 000078 | retained, let F be a BRST-closed physical source word. Then 000079 | 000080 | d_t I_t(F)=-I_t((s dotPsi_t)F) 000081 | =-I_t(s(dotPsi_t F))=0. (1) 000082 | 000083 | The same holds for finite products of physical insertions and hence their 000084 | source coefficients. Applied to both bound original calls, it preserves 000085 | their relative quotient. This follows from the ORIGINAL Ward premise; 000086 | it is not a new freely chosen model or density. 000087 | 000088 | Equation(1) is not a claim that every gauge-variant W_k[J] or off-shell 000089 | Gamma_k is gauge independent. Generic elementary gauge/ghost source 000090 | insertions are not BRST closed; a regulator must carry its actual Ward 000091 | identity. Direct transport by the same U instead preserves ALL original 000092 | source legs in one given gauge, without changing that gauge at all. 000093 | 000094 | The ghost determinant need not cancel pointwise between two different 000095 | backgrounds. K_g* K_g and its reference value can differ. The full quotient 000096 | integration, with its determinant/Jacobian/domain, is the invariant object. 000097 | Deleting its field-dependent ghost factor would change the given caller. 000098 | 000099 | The primary BRST/BV distinction is standard: gauge fixing is represented 000100 | by a canonical antifield transformation; antighost/auxiliary variables 000101 | form a contractible sector. A nontrivial physical action deformation 000102 | belongs instead to BRST cohomology modulo exact terms. See Barnich, 000103 | Brandt,Henneaux, Local BRST cohomology in gauge theories, section2.6, 000104 | equations2.26–2.47: https://arxiv.org/pdf/hep-th/0002245 . 000105 | That local algebraic result is not a new global gauge-slice existence 000106 | theorem. The actual original quotient/Ward hypotheses remain attached. 000107 | 000108 | 4. WHAT IS FIXED, AND THE FIRST ILLEGAL IDENTIFICATION 000109 | 000110 | Boundary001:302–315 explicitly calls S_prim a relative spectral SEED and 000111 | introduces gauge fixing, ghosts and compatible fluctuations later. 000112 | Its spectral/reference ratio is fixed by its displayed same constructor, 000113 | as WEIGHT.txt proves. The old geometric residue constructor already 000114 | jointly fixes the Einstein, Higgs, gauge and curvature terms in its stated 000115 | branch. No independent copy of those terms is to be added here. 000116 | 000117 | The actual original finite Higgs one-form/Yukawa/Majorana consumer and 000118 | same-collar kinetic pairing are already established. Given its actual 000119 | fermion bilinear and orientation, Berezin integration produces that same 000120 | determinant/Pfaffian and all external-source minors once. The fixed full 000121 | U carries the original bilinear, sources, Jacobian and reference exactly; 000122 | FUNCTOR.txt:section3 and equation10 provide the full source statement. 000123 | This transport neither adds a fermion law nor changes the original state. 000124 | 000125 | Neither QFT007's higher-derivative notation nor an optional symbol S_extra 000126 | licenses independently selected new interactions. In each actual original 000127 | call those derivatives/terms are whatever its GIVEN action has. If a new 000128 | gauge-invariant, BRST-nonexact deformation were added, its selection would 000129 | be new physical input. None was added or forced by the inspected passages. 000130 | A missing displayed Psi cannot stand in for evidence of such a deformation. 000131 | 000132 | The actual whole U transports D to mathfrakD_h, including derivatives and 000133 | boundary domains, NOT to Phi alone. Even on an original constant product 000134 | coefficient, mathfrakD_h^2 contains -partial_r^2+p^2+Phi^2. The compact 000135 | coefficient Phi has neither original derivative. Accordingly the current 000136 | v259 profile-moment and v255 finite heat-coefficient readings must retain 000137 | their actual geometric/IR expansion map. Equating their finite coefficient 000138 | trace to the entire unnormalized S_adm/Z_rel is the first unsupported step 000139 | in this proposed compact rewrite. It is not repaired by choosing ghosts. 000140 | 000141 | The direct whole-source transport remains exact regardless of that optional 000142 | rewrite. The full given P1 state/RP/reference, all original null-source 000143 | factors and eta, and the common S/Z/OS/Gamma architecture remain present. 000144 | This review closes the spurious gauge-choice objection and does not claim 000145 | a complete fundamental solution or an all-corpus failure of full S_adm. 000146 | 000147 | SOURCE RECORDS CHECKED THROUGH READ_SOURCE 000148 | 000149 | Boundary001:296–343, paper-source:8027564739689dd02e02f11c, 000150 | sha7d6e673d99c29d950dc601283cd51c1cc0b113567eeb79c8396fec9c82a02c79. 000151 | ResearchContract2/007:1–21, paper-source:4493812a05dfb280095129c7, 000152 | sha3bc402debcf11dbf7d5560b37e64c6afe6126bc121c9af39901bb39f90cb89fd. 000153 | Contract008:260–309, paper-source:2ef6f12ed69539ba7ea94be8, 000154 | sha8fba02c4b93076592cd51ec0c3c69f8469cc9eabc0048bf085d74508e7f98a2b. 000155 | Metrology004:1–169, paper-source:3a81043815727ab8a8dbca23, 000156 | sha669d088bea83eef25cfd9960905893cc57d2827c7b4d7558c5aa7b408b85581a. 000157 | StandardModel007:1–49,92–178, 000158 | paper-source:c59f5347aabe949c45484c99 /5c596f27c86a48c72a794495, 000159 | shad110376a2d97decdaa06d3f6c90375ec242e63a26ea7af299d45945f9658f91b. 000160 | QFT007:1–28,119–143, paper-source:f588a78cad85dd5237213db3, 000161 | sha9c1c587cbd61fc4034649d778d16f1ee0e8c1e1189885babb3d8148a6fe72d7c. 000162 | Contract015:144–183, paper-source:167e6cda6ca60a72b6789845, 000163 | sha2ec9c3ab6903e9d29823ee5a52ef588cf8504848df6c51c21f0412f31f9eb886. 000164 | Companion full action and source-map evidence: FUNCTOR.txt, 000165 | REFERENCE-SOURCE-COMPLETION.txt, PAIR-TYPING.txt and WEIGHT.txt in 000166 | this same work/reference_transport_G directory. Their exact scope and 000167 | original source manifests are retained rather than reclassified here.