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PTG III

PTG III: Transport Capacity, Completeness, and Incompleteness Theorems

Graham Fincham, Daniel Hilton

Reader summary

PTG III turns local focusing into a global obstruction. We define transport capacity, a non-negative measure on hypersurfaces compatible with the transport cone, and a notion of transport completeness for congruences. Capacity evolves with the expansion, so a focusing congruence collapses capacity to zero in finite parameter. The global focusing lemma combines this with PTG II's finite-parameter focusing to prove that twist-free transport generators with negative expansion on a hypersurface of finite capacity cannot be extended indefinitely. These are structural analogues of the Penrose and Hawking singularity theorems, established without any metric or causal structure.

Abstract

We develop a global theory of transport completeness in the metric-free framework of Phase Transport Geometry. Building on the finite-parameter focusing mechanism established in Phase Transport Geometry II, we introduce a capacity structure for hypersurfaces and define a notion of transport completeness for congruences. Using these constructions, we prove incompleteness theorems for twist-free transport generators under a non-defocusing condition. The results are purely geometric and require no metric, curvature tensor, or causal structure.

Falsifiable predictions

  1. 01
    Any hypersurface of finite transport capacity with strictly negative expansion lies at the start of an incomplete transport congruence.
  2. 02
    Localised regions of negative expansion suffice to force incompleteness; compactness of the initial hypersurface is not required.
  3. 03
    Transport incompleteness is a purely geometric phenomenon, independent of any metric, causal structure, or curvature tensor.

Full paper

Introduction

This paper extends the analytical results of PTG II into a global framework. The finite-parameter focusing theorem implies that twist-free transport congruences with negative initial expansion cannot be extended indefinitely. To convert this local divergence into a global obstruction, we introduce a notion of transport capacity for hypersurfaces and define transport completeness for congruences.

The main results are: a definition of transport capacity compatible with the transport cone structure; a global focusing lemma combining finite-parameter focusing with capacity collapse; and incompleteness theorems for twist-free transport generators under a non-defocusing condition. These are structural analogues of classical incompleteness theorems but require no metric or curvature assumptions.

Preliminaries

Transport generators are smooth vector fields lal^{a} with lal^{a}(p) in LpL_{p}. The expansion θ\theta of the congruence generated by lal^{a} satisfies finite-parameter focusing (PTG II): for twist-free lal^{a} with F(lal^{a}) \geq 0 and θ\theta(0) < 0, there is finite λ\lambda_{\star} with θ\theta \to -\infty as λλ\lambda \to \lambda_{\star}.

Transport capacity

Hypersurfaces

A smooth embedded hypersurface S is transversely admissible if LpL_{p} contains at least one vector transverse to S at each p in S.

Capacity density and measure

Let ρ(la)\rho(l^{a}) be a non-negative, degree-one homogeneous scalar density on admissible transport generators. The capacity measure on S is <<d\mu_{S \ρ\rho} := \rho(l^{a}) d\mu_{S}>>, where dμSd\mu_{S} is the induced hypersurface measure.

Transport capacity

J(S, l) :=:= \int over S of ρ(la)dμS\rho(l^{a}) d\mu_{S}. A hypersurface has finite transport capacity if this \int is finite.

Transport completeness

A transport generator lal^{a} is future transport complete if every \int curve starting on S is defined for all λ\lambda \geq 0.

Evolution of capacity

Capacity evolution

dJ/dlambda = \int over <<S_{\λ\lambda}>> of θρ(la)\theta \rho(l^{a}) dmu. Differentiate under the \int and use the definition of expansion.

Monotonicity

If θ\theta < 0 on <<S_{\λ\lambda}>>, then dJ/dlambda < 0.

Capacity collapse

If θ(λ)\theta(\lambda) \to -\infty as λλ\lambda \to \lambda_{\star}, then J(<<S_{\λ\lambda}>>, l) \to 0.

Global focusing lemma

Let S have finite transport capacity, and let lal^{a} be twist-free with F(lal^{a}) \geq 0 and θ\theta < 0 on S. Then the congruence is not future transport complete. Finite-parameter focusing forces capacity collapse; a transported hypersurface with zero capacity cannot exist as a smooth admissible hypersurface, so the congruence cannot be extended.

Incompleteness theorems

Compact initial hypersurfaces

If S is compact with finite transport capacity and θ\theta < 0 on S, then the congruence is not future transport complete.

Non-compact hypersurfaces

Compactness is unnecessary: finite capacity and θ\theta < 0 on S suffice.

Localised negative expansion

If θ\theta < 0 on a subset U of S of positive capacity, then the congruence is incomplete.

Discussion

We have introduced transport capacity and transport completeness and proved incompleteness theorems for twist-free transport generators. These results are structural analogues of classical incompleteness theorems but arise without any metric or curvature assumptions, and form the global geometric foundation for the boundary structures in PTG IV.

Suggested citation

@techreport{pdt_ptg_iii_2026,
  author      = {Fincham, Graham and Hilton, Daniel},
  title       = {PTG III: Transport Capacity, Completeness, and Incompleteness Theorems},
  institution = {Phase Differential Theory},
  year        = {2026},
  type        = {PDT working paper},
  number      = {PTG III}
}