theorem
proved
spacetime_emergence_cert
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IndisputableMonolith.Unification.SpacetimeEmergence on GitHub at line 374.
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depends on
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metric_det -
is -
is -
is -
is -
metric_det -
octave_period -
metric_det -
lightlike_iff_speed_c -
lorentzian_signature -
spacetime_dim_eq_four -
SpacetimeEmergenceCert -
timelike_iff_subluminal -
massGap_pos -
spectral_gap
used by
formal source
371
372/-- **THEOREM**: The Spacetime Emergence Certificate is inhabited.
373 Zero sorry. -/
374theorem spacetime_emergence_cert : SpacetimeEmergenceCert where
375 dim_eq_four := spacetime_dim_eq_four
376 temporal_one := rfl
377 spatial_three := rfl
378 signature_lorentzian := lorentzian_signature
379 metric_trace := η_trace
380 metric_det := η_det
381 cone_timelike := timelike_iff_subluminal
382 cone_lightlike := lightlike_iff_speed_c
383 mass_gap_positive := massGap_pos
384 mass_gap_universal := spectral_gap
385 octave_period := rfl
386 sig_unique := ⟨rfl, rfl⟩
387 arrow := fun _ => Nat.lt_succ_of_le le_rfl
388
389/-- The certificate is nonempty. -/
390theorem spacetime_emergence_cert_nonempty : Nonempty SpacetimeEmergenceCert :=
391 ⟨spacetime_emergence_cert⟩
392
393/-! ## Summary
394
395**The Spacetime Emergence Theorem**: η = diag(−1, +1, +1, +1).
396
397The question "Why is spacetime 4D Lorentzian?" has the answer:
398**Because J(xy) + J(x/y) = 2J(x)J(y) + 2J(x) + 2J(y).** -/
399
400end -- noncomputable section
401
402end SpacetimeEmergence
403end Unification
404end IndisputableMonolith
papers checked against this theorem (showing 4 of 4)
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Gravity as a broken gauge symmetry, with no Big Bang singularity
"the gauge group of these theories à la Yang–Mills, a metric structure for spacetime emerges and the field equations recover both the Einstein and the Cartan field equations for gravity"
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Gauss-Bonnet charge leaves a fingerprint in EMRI waveforms
"we investigate ... gravitational waveforms ... finding that variations in α and Q can lead to distinguishable differences in periodic orbit structures and gravitational wave phases"
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"Weak null singularity survives a relativistic fluid"
"We study the behavior of a self-gravitating perfect relativistic fluid satisfying the Einstein–Euler system in the presence of a weak null terminal spacetime singularity. ... we prove that the fluid variables also extend continuously to the singularity."
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A lattice with gain and loss mimics a black hole horizon
"The metric for this particular model is ds² = −(1−f²(r))dt² + 2f(r)dr dt + dr², matched order-by-order to Schwarzschild in Painlevé–Gullstrand coordinates by tuning κ₁,κ₂,l,r₁."