Advanced G Model Research | Derivations, Open Problems, and Historical Routes

1. Gravity and Spacetime

Presents the visitor guide to four-null spacetime, matter loading, the K_M to T_c scale route, weak gravity, clocks, tides, re-equalization, relativistic compatibility, strong fields, horizons, and verification priorities.

2. Coefficient Origins

Separates exact four-null geometric results from response, averaging, normalization, and spherical-spreading choices whose physical uniqueness is not yet proved.

3. Formula Derivations

Traces the retained K_M to T_c to G_G chain and keeps measured Newtonian G confined to explicitly labeled comparison calculations.

4. Research Ideas and Hypotheses

Covers causal-fabric ontology, matter loading, dynamic reconnection, causal re-equalization, and finite-scale proposals. These remain proposed structures rather than established microscopic physics.

5. Open Problems and Falsification

Prioritizes independent reproduction of the absolute numerical K_M value, a complete microscopic action and topology law, large-scale Lorentz behavior, and a distinctive independently fixed observable prediction.

6. Rejected and Historical Routes

Retains the dimensional rejection of the original 1/(5π²c) expression as Big G, abandoned coefficient-forcing attempts, the failed one-function static-vacuum route, and other tested no-go paths.

7. Numerical Structure of K_M

Derived relations, the current numerical value, and proposed measurement routes.

1. What is actually derived. Within the retained weak-source branch, the G Model uses K_M ∇²M = ρc² and ∇²M = C_Σ(c³T_c²/ℏ)ρ. Combining them gives K_M = ℏ/(C_ΣcT_c²) = (5π/12)ℏ/(cT_c²).

2. Current numerical K_M. The current working value is K_M = 9.63090777 × 10^42 N. The scale-free reciprocity relation inside the retained branch is G_G K_M = c⁴/(4π), or K_M = c⁴/(4πG_G).

3. K_M → T_c inversion. For K_M in SI units, T_c = sqrt[5πℏ/(12cK_M)]. Using K_M = 9.63090777 × 10^42 N gives T_c = 2.186570237920 × 10^-43 s.

4. Result classification. K_M∇²M = ρc² is the conditional source-modulus formulation. K_M = ℏ/(C_ΣcT_c²) is derived within the retained source branch. G_G K_M = c⁴/(4π) is an exact identity within the retained branch.

5. Proposed measurement routes for K_M. Source-response route: measure ρ and ∇²M, then compute K_M = ρc²/∇²M. Finite-cell dispersion route: measure the relevant wave number and group velocity and infer T_c or K_M.

Author / research direction: Gurbuz Dolu. AI assistance was used for mathematical audit, consistency checking, and document preparation; AI-assisted analysis is not independent scientific verification.

8. Numerical Reconstructions of the Intrinsic Fabric Time T_c

Complete historical audit of routes that produced a numerical T_c value.

AUDIT ANSWER: 4 current numerical reconstruction routes + 2 historical numerical attempts = 6 distinct routes in the retained record. Different published measurements of Newton G are repeat inputs to Route 1, not separate theoretical methods.

Most important scientific conclusion. The records repeatedly produced values near 10^-43 s, but none of the six routes currently constitutes a fully independent, experimentally closed, Big-G-free determination of the absolute T_c scale. The K_M inversion becomes genuinely independent only when K_M itself is independently measured or derived in SI units without recycling the calibrated gravitational scale.

REFERENCE VALUES USED FOR COMPARISON: Current reference: T_c,ref = 2.186570237920 x 10^-43 s. Current reference modulus: K_M,ref = 9.63090777 x 10^42 N. Retained coefficient: C_Σ = 12/(5π).

1. Counted Numerical Routes: 1, Measured Big-G calibration, 2.186570237920000e-43, 0 (reference), CALIBRATED. 2, K_M -> T_c inversion, 2.186570237920000e-43, 0 (reference), ALGEBRAICALLY EXACT GIVEN K_M / NUMERICAL PROVENANCE NOT INDEPENDENT. 3, Mercury perihelion back-inversion, 2.186565119429730e-43, -2.3409 ppm, OBSERVATIONAL INVERSION / CALIBRATED COMPATIBILITY. 4, Two-cloud / moved-source laboratory reconstruction demonstration, 2.186570237529000e-43, -0.0002 ppm, EXPERIMENTAL RECONSTRUCTION FORM / DEMONSTRATION ONLY. 5, Historical K_GD bare-SI numerical closure, 2.200469454000000e-43, +0.6357%, HISTORICAL / PROVISIONAL / SUPERSEDED. 6, Historical Earth source-curvature diagnostic, 2.470000000000000e-43, +12.9623%, HISTORICAL / ILLUSTRATIVE / NOT INDEPENDENT. Count rule: an algebraically equivalent rewrite is not counted as a new method. Repeating the Big-G calibration with another measured value of G is a new empirical input to the same route, not a new route.

2. Current Retained Numerical Reconstructions. 2.1 Route 1 - Measured Big-G Calibration. The mature continuum bridge can be inverted using measured Newton G as an empirical dimensional anchor. This is the official calibrated/reference route; it is not a native prediction of G. G_G = (C_Σ/4π) c^5 T_c^2 / ħ = [3/(5π^2)] c^5 T_c^2 / ħ. T_c = [4π ħ G / (C_Σ c^5)]^(1/2) = [(5π^2/3) G ħ / c^5]^(1/2). T_c = 2.186570237920 x 10^-43 s. STATUS - CALIBRATED: Measured Big G fixes the absolute scale. Every downstream number inherits that input. A T_c obtained this way cannot be fed back to claim an independent prediction of the same Big G. Source record: G_Model_COMPLETE_RECONSTRUCTION_AUDIT_09SEP2026_203P.pdf; current manuscript calibration record.

2.2 Route 2 - K_M to T_c Inversion. Matching the weak source law to the source-modulus form yields an internal K_M-T_c relation. If K_M is independently known in newtons, the positive-root inversion fixes T_c without inserting Big G into the inversion itself. K_M = ħ/(C_Σ c T_c^2) = (5π/12) ħ/(c T_c^2). T_c = [5π ħ/(12 c K_M)]^(1/2). K_M = 9.63090777 x 10^42 N -> T_c = 2.186570237920 x 10^-43 s. STATUS - EXACT INVERSION GIVEN THE RETAINED K_M LAW; NUMERICAL INDEPENDENCE OPEN: The 12 September provenance audit found that the present numerical K_M is equivalent to the earlier Big-G-calibrated scale. Therefore the current number is not yet an independent native absolute-scale determination. A direct Big-G-free source-response measurement of K_M would make this route genuinely independent. Source record: G_Model_KM_to_Tc_Derivation_Study_11SEP2026.pdf; G_Model_Response_on_KM_Numerical_Provenance_12SEP2026.pdf.

2.3 Route 3 - Mercury Perihelion Back-Inversion. The observed Mercury perihelion advance was inserted into the retained conditional continuum perihelion expression and inverted for T_c. K_GD appears only as the historical c-reparameterization; it is not Newton G. K_GD = 1/(5π^2 c). T_c = [625π^7 ħ K_GD^3 a(1-e^2) Δϖ /(18 M_sun)]^(1/2). T_c,Mercury = 2.18656511942973 x 10^-43 s. K_M,Mercury = 9.630952860 x 10^42 N. STATUS - OBSERVATIONAL INVERSION / CALIBRATED COMPATIBILITY: The result is -2.3409 ppm from the retained reference. It is a real observational benchmark, but the continuum formula is conditional and a high-precision solar mass in kilograms can inherit gravitational information. It is not yet a parameter-free native T_c prediction. Source record: G_Model_KGD_Substitution_Tc_Reconstruction_Audit_12SEP2026.pdf; G_Model_CURRENT_MANUSCRIPT_55P_MMM_AAA_XYZ_LAW_UPDATE_12SEP2026.pdf.

2.4 Route 4 - Two-Cloud / Moved-Source Laboratory Reconstruction. A direct differential-acceleration experiment can reconstruct an effective coupling, K_M, and T_c from independently characterized source geometry and a measured source-induced acceleration difference. D = r_n^(-2) - r_f^(-2). G_eff = Δa_mod /(2 M_s D). T_c = [15625π^12 ħ K_GD^5 Δa_mod /(6 M_s D)]^(1/2). 100 kg demonstration: T_c = 2.186570237529 x 10^-43 s. K_M = 9.63090777344 x 10^42 N. STATUS - EXPERIMENTAL RECONSTRUCTION FORM; NUMERICAL DEMONSTRATION ONLY: The formula is suitable for a real source-swap laboratory test. However, the recorded 100 kg numerical demonstration used an acceleration generated from the familiar gravitational strength, so that numerical agreement is an algebraic consistency check, not an independent experiment. Source record: G_Model_CURRENT_MANUSCRIPT_55P_MMM_AAA_XYZ_LAW_UPDATE_12SEP2026.pdf, Sec. 19.1 / CF199-CF201.

3. Historical Numerical Attempts Preserved in the Record. 3.1 Route 5 - Provisional K_GD Bare-SI Closure (3 September 2026). Before the later scale-symmetry/provenance audits, the bare SI numerical magnitude of K_GD was used as a deliberately heuristic target in the single-T_c gravitational bridge. This produced a numerical T_c without inserting measured Big G, but the operation compared unit-stripped numerical magnitudes of quantities with different dimensions. Heuristic test only: Num_SI[G_eff(T_c)] = Num_SI[K_GD]. Equivalent unit-stripped numerical solution: T_c = [Num_SI(ħ)/(3 Num_SI(c)^6)]^(1/2). T_c = D_0,eq = 2.200469454 x 10^-43 s. STATUS - PROVISIONAL SI NUMERICAL CLOSURE - SUPERSEDED AS AN ABSOLUTE-SCALE CLAIM: This value is +0.6357% above the current reference. The method was explicitly recorded as unit-system dependent and not a dimensionally valid physical identity. It remains historically important but is not an active independent closure. Source record: G_Model_Produced_Numerical_D0_03SEP2026.pdf; G_Model_Integrated_Research_Manuscript_04SEP2026.pdf. 3.2 Route 6 - Earth Source-Curvature Diagnostic (4 September 2026). A uniform-Earth curvature estimate and mean density were inserted into the then-current source relation, producing another numerical T_c estimate. Archived inputs: Q_u ≈ 5.14 x 10^-23 m^-2, ρ ≈ 5.5 x 10^3 kg m^-3. Archived result: T_c^(Earth,diag) ≈ 2.47 x 10^-43 s. STATUS - ILLUSTRATIVE DIAGNOSTIC - NOT INDEPENDENT: This value is about +12.96% above the current reference. The curvature estimate was inferred from weak-field Earth quantities rather than measured as an independent microscopic clock-curvature observable. It therefore did not close the scale. Source record: G_Model_Turkce_M_D0_Aciklayici_Manuscript_04SEP2026.pdf.

4. Why Several Other T_c Values Do Not Increase the Method Count. Several records use different experimental or tabulated values of Newton G and then map each value through the Big-G calibration formula. These can produce slightly different numerical T_c values - including reconstructions from precision laboratory G determinations such as atom-interferometric measurements - but mathematically they are all Route 1. They are useful cross-checks of sensitivity to the measured G input, not independent G Model scale-setting mechanisms. For any measured G_i: T_c(G_i) = [(5π^2/3) G_i ħ / c^5]^(1/2). Therefore T_c ∝ sqrt(G). Audit decision: do not count each published G experiment as a separate T_c method. Count the calibration equation once, then list experimental G values as subcases when needed.

5. Operational Routes Derived but Not Yet Numerically Closed by Independent Data. The record contains additional ways that could determine T_c if their upstream observables were independently measured. They are not included in the six numerical-route count because no independent numerical T_c has yet been produced from them. Direct source-response / modulus: K_M = ρ c^2 / ∇^2M; T_c = [(5π ħ/(12 c^3))(∇^2M/ρ)]^(1/2); CONDITIONAL PASS if ρ and M-curvature are measured without Big-G inference. Finite-cell dispersion: T_c = [sqrt(3)/(c k)] arccos(v_g/c); OPERATIONAL PASS within the retained dispersion branch; physical realization remains conditional. Neutral tension / energy: T_c = (24/c)(σ_0/u_f0) = 120π^2 K_GD (σ_0/u_f0); PROMISING CONDITIONAL route; requires independently measured/derived tension-energy ratio. Recovery-time extraction: T_c = (3/2) τ_rec; CANDIDATE; requires a physically identified microscopic recovery time. Neutral area-stiffness closure: κ_C L_c^2 = ħ -> T_c = [ħ/(κ_C c^2)]^(1/2); CANDIDATE; κ_C has not been independently fixed, so this only relocates the missing scale. Independent D_0 / Aggregation anchor: Current audit gives a T_c relation if D_0 is independently observed rather than defined from T_c; OPEN experimental anchor; no independent microscopic D_0 measurement yet.

6. Independence Audit - What Has Actually Been Achieved? Numerically, T_c has been reconstructed six distinct ways across the historical record. Scientifically, however, the absolute scale remains independently open. The routes separate into calibration, algebraic inversion, observational back-inversion, demonstration reconstruction, and historical diagnostics. This distinction matters more than the raw count. How many current numerical reconstruction routes? 4. Big G, K_M, Mercury, laboratory reconstruction demonstration. How many total historical numerical T_c routes in the retained records? 6. The four current routes plus the provisional K_GD SI closure and Earth diagnostic. How many are fully independent, Big-G-free experimental determinations today? 0. No upstream dimensional anchor has yet been independently measured/closed without inherited gravitational calibration. Can K_M become an independent route? YES. Yes, if K_M is directly measured/derived in SI units from source response without hidden Big-G or T_c reuse. Do different published G measurements count separately? NO. They are different inputs to the same Big-G calibration equation.

7. Controlled Conclusion. Final audit result: the G Model research record contains six distinct routes that actually produced a numerical T_c value. Four are part of the current reconstruction discussion and two are preserved historical diagnostics. The strongest numerical convergence is among Big-G calibration, K_M inversion, Mercury back-inversion, and the moved-source laboratory demonstration, all near 2.18657 x 10^-43 s. This convergence is a useful internal/empirical consistency pattern, but it is not six independent confirmations because several routes inherit the same gravitational normalization directly or indirectly. ANTI-CIRCULARITY TEST. Current scientific target: independent observable -> K_M or T_c -> predict G_G -> compare with measured gravity. not: measured gravity -> T_c -> reproduce measured gravity.

Source Records Used in This Audit: [S1] G_Model_COMPLETE_RECONSTRUCTION_AUDIT_09SEP2026_203P.pdf; [S2] G_Model_KM_to_Tc_Derivation_Study_11SEP2026.pdf; [S3] G_Model_Response_on_KM_Numerical_Provenance_12SEP2026.pdf; [S4] G_Model_KGD_Substitution_Tc_Reconstruction_Audit_12SEP2026.pdf; [S5] G_Model_CURRENT_MANUSCRIPT_55P_MMM_AAA_XYZ_LAW_UPDATE_12SEP2026.pdf; [S6] G_Model_Produced_Numerical_D0_03SEP2026.pdf; [S7] G_Model_Integrated_Research_Manuscript_04SEP2026.pdf; [S8] G_Model_Turkce_M_D0_Aciklayici_Manuscript_04SEP2026.pdf; [S9] G_Model_How_Tc_Was_Obtained_From_KM_Educational_11SEP2026.pdf; [S10] G_Model_Absolute_Scale_Closure_No_Go_Theorem_Educational_11SEP2026.pdf. Author / research direction: Gurbuz Dolu. AI assistance was used for record retrieval, algebraic cross-checking, numerical comparison, organization, and document preparation.

9. Causal Reconnection and Re-Cellulation

G Model | Reconnection of Cells | Website Research Note G MODEL Reconnection of Cells Continuous relational transport, Celal matching, Xyz causal integrity, and the exceptional re-cellulation problem CURRENT STATUS: The G Model does not presently contain a fully action-derived physical link- birth/link-death law. The strongest current architecture separates ordinary continuous relational evolution on existing causal relations from exceptional Xyz rank-loss events. Celal provides exact minimum-discontinuity branch correspondence on an existing centered link. The post-Xyz re- cellulation/topology/phase move set remains OPEN. Website research note - based on the current manuscript and formula register CF001-CF222 Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 1

G Model | Reconnection of Cells | Website Research Note 1. What "reconnection" means in the current G Model In the current G Model, the word reconnect has two different meanings that must be kept separate. Ordinary neighboring cells may need to change how their four causal branches are matched as the local geometry evolves. That is a relational matching problem. A genuine change of graph topology or cell decomposition is a stronger event and is not assumed to occur every time matter moves through a region. The present framework therefore uses a layered architecture: moving matter changes the source; the fabric state responds continuously; neighboring cells are compared and rematched relationally; and the Xyz Law monitors whether the local four-null causal basis remains valid. Only an attempted outward crossing of the Xyz boundary raises the exceptional re-cellulation/topology/phase problem. Why this distinction matters: matter can leave a region while the deformation M remains nonzero. Therefore "matter absent" does not mean "fabric neutral," and an ordinary material surface cannot automatically be a graph-breaking surface. The three layers What it does NOT Layer Main variable What it tells us imply Where direct matter It does not by itself say Matter support χm occupancy/source whether M=0 or whether support is present. topology changes. How the local causal M≠0 does not require fabric and full stress- Fabric/source state M, Hab, γx matter to be locally energy source are present. represented. How neighboring branch Π, Ωyx, graph/cell frames correspond and It need not change at Causal organization decomposition how the causal complex every matter boundary. is organized. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 2

G Model | Reconnection of Cells | Website Research Note 2. Ordinary dynamics: continuous source-driven relational transport The most natural current G Model picture for ordinary moving matter is continuity first, topology second. A planet, particle, star, or laboratory body changes which local regions contain matter. Its motion, rotation, stress, and internal momentum currents change the local source continuously. Nothing in the retained weak-field equations requires the causal graph to break every time the material boundary crosses a local region. 2.1 Matter-support transport CF218: ∂tχm + vm · ∇χm = 0 For a sharp transported support, χm is carried with the matter flow. The equation is kinematic bookkeeping: it says the occupied region moves with matter. It does not assert that the spacetime fabric itself moves with the body. 2.2 Rigid translation, rotation, and axial tilt CF219: vm(x,t) = V(t) + ω(t) × [x - X(t)] CF220: (ω × r) · n = 0 for n ∥ r For an ideal spherical boundary, axial rotation is tangent to the surface for any spin-axis direction. The same statement therefore remains true when the spin axis is tilted. Translation can move the matter-support boundary across local cells; rotation instead produces tangential momentum and circulation. 2.3 Full source, not occupancy alone CF221: T⁰⁰ ≈ ρc², T⁰ⁱ ≈ ρc vⁱ, Tⁱʲ ≈ ρ vⁱvʲ This is why reconnect/transport dynamics cannot be based on χm alone. Rotation and tilt can change the momentum-current and stress sectors even while an ideal spherical support is unchanged. In the G Model, the corresponding branch-space source is Hab = kaμ kbν Tμν. The full microscopic response of the causal network to Hab remains OPEN. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 3

G Model | Reconnection of Cells | Website Research Note 3. Why an ordinary matter surface is not automatically a topology surface A tempting early interpretation was: matter enters a local region, the previous connection breaks; matter leaves, the region reconnects. The later moving-matter and weak-field audits show that this is too strong as a fundamental law. 3.1 Matter can be absent while the fabric remains disturbed State Meaning Reconnect implication (χm,M)=(0,0) No local matter; neutral fabric. Ordinary neutral region. Source loading is present; no (1,M≠0) Matter present; fabric deformed. automatic graph change follows. Direct proof that matter exit does Matter absent locally; deformation (0,M≠0) not force instantaneous persists. neutralization. Matter present while M is neutral Occupancy and deformation are (1,0) in a special/equalized state. logically distinct. 3.2 Weak-field boundary continuity CF222: [M]S = 0, [∂nM]S = 0, [∇²M]S = CΣ(c³Tc²/ℏ)[ρ]S Under the retained weak source equation and in the absence of a delta-function surface layer, M and its normal derivative can remain continuous across an ordinary density boundary even though the source term ∇²M changes. A mandatory graph break at every matter surface would introduce an additional microscopic discontinuity that the weak-field solution does not require. Retained conclusion: the material boundary marks where direct source support changes. It is not, by itself, an Xyz boundary or a graph-topology boundary. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 4

G Model | Reconnection of Cells | Website Research Note 4. Celal Dynamic Reconnect: what it actually does Celal Dynamic Reconnect is the strongest exact reconnect result presently available for ordinary neighboring cells. Its job is not to create or delete links. Its job is to decide how the four branches of one deformed cell should correspond to the branches of a neighboring deformed cell. Cxy(Π) = 1/2 || γx - Πᵀ γy Π ||F² ΠCelal ∈ arg minΠ∈S₄ Cxy(Π) Here γx and γy are the local branch Gram matrices and Π is a tetrahedral branch permutation. The minimizing correspondence is exact in the centered physical sector, modulo the expected Klein-four V4 degeneracy. 4.1 Why this is a natural ordinary reconnect rule  It compares invariant local geometry rather than arbitrary branch labels.  It introduces no new fitted dimensional coefficient.  It is relational: a branch number is not treated as an absolute physical identity across different cells.  It is compatible with the Jadvyga requirement that absolute local orientation not become an observable preferred direction in the accepted invariant sector.  It can operate continuously while matter, rotation, tilt, and neighboring geometry change. 4.2 Inter-cell transport Ωyx = Ky Πyx Kx⁻¹ When matched frames have compatible Gram structure, Ωyx is Lorentz transport on the matched branch frames. This provides the natural bridge between local reorientation and neighbor-to- neighbor comparison. A full action-derived evolution equation for Kx or Ωyx is still OPEN. Celal status: EXACT geometric selection on an existing centered link. It is not yet a physical link- birth/link-death law. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 5

G Model | Reconnection of Cells | Website Research Note 5. Xyz Law: the causal-integrity boundary Xyz should now be understood as the exceptional causal-integrity test, not as an ordinary matter- surface trigger. It tells us when the centered four-null causal basis reaches rank loss. 5.1 Exact Gram-triangle theorem A12=A34=xLc², A13=A24=yLc², A14=A23=zLc² -det(γ/Lc²) = (x+y+z)(-x+y+z)(x-y+z)(x+y-z) = 16 Atri² For positive x, y, z, the ordinary one-negative/three-positive Lorentzian cell exists while the strict triangle inequalities hold. The Xyz boundary occurs when the auxiliary triangle becomes degenerate and det γ → 0. 5.2 Causal-integrity margin χXyz = min{s - 2α, s - 2β, s - 2γ} Condition Meaning Current interpretation Ordinary Lorentzian four-null Ordinary causal evolution may χXyz > 0 region. remain on the existing relations. At boundary but not attempting an The retained phase may remain χXyz = 0, DτχXyz ≥ 0 outward crossing. admissible. Smooth ordinary continuation Actual evolution attempts to leave cannot remain unchanged; an χXyz = 0, DτχXyz < 0 the retained 1+3 domain. admissible intervention is required. Important correction: the general outward-crossing statement no longer depends on the old exponential Causal Re-Equalization law. That older law can still provide a special boundary-flow example if assumed, but the controlling Xyz statement is geometric/kinematic. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 6

G Model | Reconnection of Cells | Website Research Note 6. What Xyz identifies - and what it still does not determine 6.1 Failed mode and the 2+2 causal cut ux = (1, 1, -1, -1), γ ux = 0 k1 + k2 - k3 - k4 = 0 cx = Bᵀux ∝ (0, ±2, ±2, ±2, ±2, 0) Pgrad cx = cx, Pcirc cx = 0 At a simple Xyz edge, the failed Hadamard mode identifies a 2+2 partition of the four branches. In the six-channel incidence/Hodge decomposition, the selected cut is pure gradient. This is an exact statement about which local causal mode degenerates. 6.2 Two exact local no-go results  Permutation cannot repair rank loss: det(ΠᵀγΠ)=det γ. Celal can change correspondence but cannot make a singular Gram matrix nonsingular by relabeling alone.  An isolated K4 cell already contains all C(4,2)=6 internal pair links. There is no unused internal edge to add inside the same unchanged four-vertex cell. Therefore a genuine post-Xyz repair, if the theory requires one, must involve neighboring cells, a change in cell decomposition, or another microscopic phase. 6.3 Candidate-action clue, not a unique move V4,x = (2/3)Lc⁴ sqrt(|det γx| / |det γ0|) Within the current candidate dual-area action, det γx → 0 drives the local four-volume weight and candidate dual-area weight toward zero if the normalized holonomy remains finite. This makes Xyz a structurally natural exceptional locus, but it does not uniquely select the physical post-Xyz move. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 7

G Model | Reconnection of Cells | Website Research Note 7. The current reconnect architecture The clearest way to summarize the current result is to separate ordinary dynamics from exceptional causal-integrity failure. 7.1 Ordinary layer Moving matter changes ρ, momentum current, stress, and therefore Hab. Local geometry and neighbor relations can evolve continuously. Jadvyga removes an absolute local orientation from accepted invariants; Ωyx transports matched frames; Celal chooses the least-discontinuous branch correspondence. As long as χXyz>0, no topology change is required by the current mathematics. 7.2 Exceptional layer If the actual dynamics reaches χXyz=0 and attempts DτχXyz<0, the ordinary four-null phase cannot simply continue unchanged. At that point the model requires an admissible intervention. The nature of that intervention - re-cellulation, topology update, or another microscopic phase - remains OPEN. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 8

G Model | Reconnection of Cells | Website Research Note 8. Causal Re-Equalization: retained mathematics, revised physical role The older local tracking equation remains mathematically useful, but it should not be presented as the fundamental microscopic reconnect law. Tc dq/dτ = -(I - P)(q - qeq) e(τ) = e(0) exp[-3τ/(2Tc)], τrec = 2Tc/3 If the candidate equation is adopted, its centered exponential solution, recovery operator, spectral decomposition, semigroup property, and Lyapunov monotonicity are exact within that candidate. However, the current microscopic action does not derive this irreversible first-order relaxation; it provides curvature/derivative stiffness rather than an automatic local friction-like decay. 8.1 Current status of the old recovery formulas Item Mathematical status Physical status now Effective / historical tracking CF157 / CF087 evolution Defined candidate equation. candidate; not fundamental reconnect dynamics. Do not treat τrec as a Exponential decay and τrec Exact given CF157. fundamental topology time. Retained as useful mathematics Recovery semigroup / projectors / Exact given the candidate law. and possible coarse-grained Lyapunov decay phenomenology. Exact given CF157 and fixed Special example only; not the CF206 boundary-flow formula common mode. general Xyz trigger. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 9

G Model | Reconnection of Cells | Website Research Note 9. Why this is currently the most natural G Model route "Most natural" here does not mean experimentally proved or mathematically unique. It means that, among the routes examined so far, this architecture adds the fewest unsupported assumptions while preserving the largest number of retained exact and conditional results. Reason Why it matters Ordinary weak-field solutions need not develop a Continuity first topology discontinuity at matter surfaces. Rotation, tilt, momentum currents, and stress enter Full source sensitivity through Tμν / Hab, not just through the occupancy indicator. Celal compares invariant geometry and does not Relational rather than absolute matching depend on fixed global branch labels. The Celal mismatch criterion requires no new No fitted reconnect coefficient dimensional tuning. Xyz is defined by the Gram rank/signature structure, Invariant exceptional trigger not by an arbitrary density or surface threshold. Graph/cell reorganization is invoked only when the Conservative use of topology ordinary four-null phase runs out of admissible continuation. Permutation cannot repair rank loss and K4 has no Existing no-go results are respected spare internal edge. Any future post-Xyz law must still satisfy the four- Conservation remains a gate component source-continuity requirements. 9.1 Routes considered but not adopted as the fundamental law Route Current verdict Rejected as a universal topology rule. Matter support and M are distinct; ordinary weak boundaries can be Break/reconnect at every matter-surface crossing smooth; rotation can change source currents without changing support. Impossible by itself because determinant/rank is Pure Celal permutation as Xyz repair permutation invariant. Add one new edge inside the same K4 cell Impossible because all six pair links already exist. Not adopted. It introduces conservation and action- Physical branch exchange / graph 2-switch selection questions that are not yet resolved. A natural candidate only if an additional face-sharing 2↔3 Pachner move tetrahedral simplicial-complex assumption is made; not currently forced by the native action. Not action-derived; retained only as Exponential local recovery as fundamental dynamics effective/historical tracking candidate. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 10

G Model | Reconnection of Cells | Website Research Note 10. Element-by-element reference Element Role Current status Why it is needed Separates direct matter BOOKKEEPING / χm Matter-support indicator. occupancy from fabric kinematic transport deformation. Dimensionless fabric Allows exterior or Retained model state M deformation / clock residual deformation variable variable. where matter is absent. Carries energy, Full matter source and Exact representation; Tμν / Hab momentum, rotation, tilt, branch-space encoding. dynamics open pressure, and stress. Defines the local causal Local four-branch frame Kx Geometric state basis and allows inter- matrix. cell transport. Carries rank/signature Invariant branch Gram γx Exact local geometry information and enters matrix. Celal/Xyz. Lets neighboring cells Tetrahedral branch Discrete relational label compare branches Π permutation. map without absolute label identity. Measures geometric Cxy(Π) Celal mismatch cost. Definition discontinuity between matched neighbors. Provides ordinary Minimum-discontinuity EXACT geometric ΠCelal relational reconnect on branch correspondence. selection in stated sector existing links. Conditional/geometric; Moves matched local Inter-cell branch-frame Ωyx Lorentz when Grams frame information transporter. match between neighbors. Monitors whether Definition from exact Xyz ordinary four-null χXyz Causal-integrity margin. geometry Lorentzian phase remains valid. Distinguishes merely Directional change along Microscopic law still touching Xyz from DτχXyz actual dynamics. OPEN attempting an outward crossing. Conservation gate for Four-component source- Exact representational Cb any future finite-cell divergence defect. capacity dynamics. The central missing Allowed post-Xyz object needed for a Radmissible OPEN continuation set. complete physical re- cellulation law. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 11

G Model | Reconnection of Cells | Website Research Note 11. What would complete or falsify the reconnect program? The current architecture is deliberately incomplete at the point where the mathematics stops being unique. The next advance must be more than a plausible graph move: it must be derived from native dynamics and must preserve the retained constraints. 11.1 Completion tests  Derive the continuous finite-cell evolution law for Kx, γx, or Ωyx from the microscopic action/neighbor dynamics rather than inserting a phenomenological relaxation equation.  Show that the ordinary evolution is Lorentz-covariant and does not generate an observable preferred microscopic orientation.  Derive the admissible post-Xyz continuation set Radmissible from native action, causal-integrity, incidence/Hodge, and conservation requirements.  Prove that a chosen post-Xyz update preserves the appropriate four-component source continuity whenever the incoming state satisfies it.  Show that the long-wavelength limit preserves the retained mean-defect/Poisson behavior and the current spin-2 compatibility results.  Re-test Light Theory propagation on the resulting dynamic network, especially at finite cell scale / high wave number. 11.2 Clear failure conditions  If the proposed ordinary transport requires topology discontinuities at smooth matter boundaries that the retained weak-field equations do not support, the proposal fails.  If a post-Xyz rule depends on an absolute spatial direction or frame, it conflicts with the accepted Jadvyga/Lorentz program.  If the update violates source conservation or the exact incidence/Hodge identities, it cannot be accepted as the physical reconnect law.  If a purported Xyz repair is only a permutation, it fails because rank loss is unchanged.  If a new coefficient is introduced only to force a desired macroscopic result, it violates the G Model no-arbitrary-closure rule. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 12

G Model | Reconnection of Cells | Website Research Note 12. Website summary: Reconnection of Cells Public-facing summary: In the G Model, neighboring spacetime cells are not assumed to break apart whenever matter moves. Matter changes the local source and fabric state continuously. Neighboring cells can continually rematch their causal branches through the Celal minimum- discontinuity rule. The Xyz Law acts as a separate causal-integrity test: if a local four-null cell reaches rank loss and actual dynamics tries to cross out of the allowed Lorentzian phase, ordinary continuation can no longer remain unchanged. The exact physical re-cellulation/topology/phase move after that point is still an open research problem. Current status at a glance Component Status Meaning Matter-support advection, rigid EXACT under stated kinematic Ordinary source motion is rotation, spherical tangency assumptions separated from graph topology. EXACT in stated centered existing- Natural ordinary relational Celal branch correspondence link sector reconnect. Xyz Gram/Heron rank-loss Invariant causal-integrity EXACT theorem boundary. Xyz failed mode and 2+2 Identifies the degenerating causal EXACT incidence cut mode. Useful mathematics if assumed; Causal Re-Equalization EFFECTIVE / HISTORICAL not fundamental reconnect exponential law CANDIDATE dynamics. Continuous action-derived network Needed for full microscopic OPEN evolution dynamics. Post-Xyz Radmissible and physical Main unresolved reconnect OPEN re-cellulation law problem. Scientific boundary. This document describes the present internal status of a proposed theoretical framework. Exact statements are exact only within the declared mathematical construction. Conditional and open items are not experimental validation or established laws of nature. Source basis This website research note is based on the current G Model manuscript, "G Model - Current Research Manuscript," 13 September 2026, including the official formula register CF001-CF222 and its latest causal-integrity / moving-matter clarification. It preserves the manuscript status language: EXACT, CONDITIONAL, CALIBRATED, OPEN, REJECTED, and effective/candidate where applicable. Gurbuz Dolu | 13 September 2026 | Current manuscript basis: CF001-CF222 | Page 13