Phase Cycles and Lorentz-Dilation: An Action-Groupoid Extension of a Lightlike Functor

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Auteur principal: Meisner, Edward
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author Meisner, Edward
author_facet Meisner, Edward
contents <p>This paper presents the Lorentzian completion of the phase‑cycle/lightlike functor introduced in <em>Paper #1</em>. The earlier construction defined a category of phase cycles Pθ, a category Sc of lightlike intervals along a single null ray, and a functor Fθ:Pθ→Sc that is an isomorphism of thin groupoids. That functor is inherently limited to one null direction and pure rescaling morphisms.</p> <p>The present work introduces the minimal categorical enrichment needed to extend that construction to <strong>all nonzero Lorentzian interval vectors</strong>. Let (V,q) be a real 1+1-dimensional Lorentzian vector space and let</p> <div> <div>G=R>0×SO+(1,1)</div> </div> <p>act by positive dilation and Lorentz transformation. The source is enriched by adding a Lorentzian direction variable u∈V∖{0} and quotienting the redundant scale in the pair (Δθ,u). This yields the quotient space</p> <div> <div>Xθ=((0,∞)×(V∖{0}))/ ⁣∼,(Δθ,u)∼(rΔθ,u/r),</div> </div> <p>and the enriched phase‑cycle category Pθ=Xθ//G. The target is the Lorentz‑dilation action groupoid</p> <div> <div>SLor=(V∖{0})//G.</div> </div> <p>The main result is that the functor</p> <div> <div>Fθ([Δθ,u])=ΔθΔθPl u,Fθ(λ,Λ)=(λ,Λ),</div> </div> <p>is an <strong>isomorphism of action groupoids</strong></p> <div> <div>Pθ  ≅  SLor.</div> </div> <p>The lightlike functor of Paper #1 is recovered as the <strong>pure‑rescaling null‑ray slice</strong> of this enriched construction. The result is purely structural: no physical constants, dynamical laws, or curvature data are derived.</p>
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spellingShingle Phase Cycles and Lorentz-Dilation: An Action-Groupoid Extension of a Lightlike Functor
Meisner, Edward
category theory
action groupoids
Lorentzian geometry
Lorentz-dilation
phase cycles
thin groupoids
null rays
lightlike intervals
timelike and spacelike intervals
equivariant functors
Lorentz transformations
1+1 dimensional spacetime
structural mathematics
<p>This paper presents the Lorentzian completion of the phase‑cycle/lightlike functor introduced in <em>Paper #1</em>. The earlier construction defined a category of phase cycles Pθ, a category Sc of lightlike intervals along a single null ray, and a functor Fθ:Pθ→Sc that is an isomorphism of thin groupoids. That functor is inherently limited to one null direction and pure rescaling morphisms.</p> <p>The present work introduces the minimal categorical enrichment needed to extend that construction to <strong>all nonzero Lorentzian interval vectors</strong>. Let (V,q) be a real 1+1-dimensional Lorentzian vector space and let</p> <div> <div>G=R>0×SO+(1,1)</div> </div> <p>act by positive dilation and Lorentz transformation. The source is enriched by adding a Lorentzian direction variable u∈V∖{0} and quotienting the redundant scale in the pair (Δθ,u). This yields the quotient space</p> <div> <div>Xθ=((0,∞)×(V∖{0}))/ ⁣∼,(Δθ,u)∼(rΔθ,u/r),</div> </div> <p>and the enriched phase‑cycle category Pθ=Xθ//G. The target is the Lorentz‑dilation action groupoid</p> <div> <div>SLor=(V∖{0})//G.</div> </div> <p>The main result is that the functor</p> <div> <div>Fθ([Δθ,u])=ΔθΔθPl u,Fθ(λ,Λ)=(λ,Λ),</div> </div> <p>is an <strong>isomorphism of action groupoids</strong></p> <div> <div>Pθ  ≅  SLor.</div> </div> <p>The lightlike functor of Paper #1 is recovered as the <strong>pure‑rescaling null‑ray slice</strong> of this enriched construction. The result is purely structural: no physical constants, dynamical laws, or curvature data are derived.</p>
title Phase Cycles and Lorentz-Dilation: An Action-Groupoid Extension of a Lightlike Functor
topic category theory
action groupoids
Lorentzian geometry
Lorentz-dilation
phase cycles
thin groupoids
null rays
lightlike intervals
timelike and spacelike intervals
equivariant functors
Lorentz transformations
1+1 dimensional spacetime
structural mathematics
url https://doi.org/10.5281/zenodo.20316224