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Lorentz Invariance as a Regime Constraint

This section interprets Lorentz invariance not as a fundamental axiom,
but as a regime-level constraint that characterizes a specific class of closure-stable realizations within the Dimensional Emergence Framework (DEF).

DEF does not assume Lorentz invariance.
It explains under which structural conditions Lorentz-invariant descriptions become admissible.


Lorentz invariance in conventional physics

Section titled “Lorentz invariance in conventional physics”

In relativistic physics, Lorentz invariance expresses the requirement that:

  • physical laws are invariant under changes of inertial reference frame,
  • spacetime admits a fixed invariant interval,
  • and no preferred frame exists.

These properties are usually postulated at the foundational level.


Within DEF, Lorentz invariance is reinterpreted as a constraint on regime realization, not on ontology.

Specifically, Lorentz-invariant regimes are those in which:

  • Existence-side relations (Structure · Space),
  • and Happening-side relations (Exchange · Dynamics),

remain symmetrically coupled under transformation.

This corresponds directly to the Core constraint:

(S · R) ≡ (X̂ · D)


Lorentz invariance emerges when:

  • constraint tension between Existence and Happening is minimized,
  • no operative mode dominates under transformation,
  • and phase ordering admits reversible traversal without divergence.

In this view, Lorentz symmetry is not primary.
It is a stable equilibrium configuration of constraint satisfaction.


In Lorentz-invariant regimes:

  • relational structure admits metric interpretation,
  • phase ordering can be coordinatized as time,
  • and exchange–dynamics coupling can be represented geometrically.

The Minkowski metric is thus understood as a representation of balanced kernel coupling,
not as a fundamental geometric substrate.


DEF naturally allows for regimes in which Lorentz invariance fails.

Such breakdown may occur when:

  • constraint tension becomes asymmetric,
  • one dimension (Existence or Happening) dominates,
  • or phase resolution cannot restore symmetry.

Examples include:

  • extreme interaction regimes,
  • non-equilibrium transitions,
  • or structurally divergent configurations.

In DEF, Lorentz violation signals regime transition, not inconsistency.


Observers embedded in Lorentz-invariant regimes will:

  • measure invariant light speed,
  • observe relativistic time dilation,
  • and infer spacetime symmetry.

Observers in non-Lorentz regimes may:

  • lack global time ordering,
  • observe anisotropic propagation,
  • or fail to coordinatize interactions spacetime-wise.

Lorentz invariance thus conditions what can be observed, not what can exist.


This interpretation does not modify relativistic physics.

It situates Lorentz invariance within a broader structural framework,
in which symmetry is a consequence of closure and constraint balance.


Lorentz invariance is therefore understood as a regime constraint
that identifies a particularly stable and symmetric realization of the DEF kernel.