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.
Structural reinterpretation in DEF
Section titled “Structural reinterpretation in DEF”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)
Symmetry as constraint satisfaction
Section titled “Symmetry as constraint satisfaction”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.
Metric emergence
Section titled “Metric emergence”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.
Breakdown of Lorentz invariance
Section titled “Breakdown of Lorentz invariance”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.
Relation to observation
Section titled “Relation to observation”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.