Encyclopedia Foundation Foundation Qrft Higgs Potential From Recognition Vacuum Vacuum Zero Potential
ARTICLE 4 claims 4 theorems
Foundation Qrft Higgs Potential From Recognition Vacuum Vacuum Zero Potential
The standard model Higgs potential has its minimum at the electroweak vacuum; Recognition Science re-derives that minimum as the unique zero-cost point of a forced cost function.
The vacuum minimum
The standard model Higgs potential is usually written V(H) = −μ²|H|² + λ|H|⁴, a quartic polynomial whose minimum sits at |H| = v/√2 ≈ 174 GeV, the electroweak vacuum expectation value (VEV). In Recognition Science (RS), this potential is not a free polynomial but a specific, forced cost function. The framework defines the cost, a measure of how expensive a recognition event is, and proves that any cost satisfying five plain conditions must equal J(x) = ½(x + x⁻¹) − 1. The Higgs potential is then the J-cost evaluated on the ratio r = |H| / (v/√2), so V_RS(r) = J(r).
The declaration vacuum_zero_potential states the central fact about this construction: the potential is zero at the vacuum. Formally, it proves higgsPotential 1 = 0, meaning when the field sits at its VEV (r = 1), the cost vanishes. This is not an arbitrary normalization. It follows from the defining property of J, which forces J(1) = 0 by the zero-cost-at-unity condition. In plain language, the vacuum is the state where recognition costs nothing, and the electroweak symmetry breaking is the selection of that state as the ground state.
The theorem is one of four structural facts proved together. The potential is symmetric about the minimum, J(r) = J(r⁻¹), so a field value above the VEV costs the same as its reciprocal below. The potential is non-negative for all positive field values. And the vacuum is the unique minimum: the only place where the potential reaches zero is at r = 1. These four facts form a certificate, a packaged proof that the Higgs potential from recognition vacuum has the right shape. The mass squared, V''(1) = 1 in RS units, comes from the calibration condition and gives the Higgs mass.
What vacuum_zero_potential does not claim is just as important. It does not derive the numerical value of the Higgs mass or the VEV; those are set by the calibration condition and by matching to measured values. It does not prove that the standard model Higgs mechanism is physically correct, only that within RS the potential's minimum has the right structural properties. The theorem is a statement about a mathematical construction, not an empirical prediction. The physical bridge from recognition events to the electroweak VEV remains open in the framework.
THEOREM vacuum_zero_potential · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean
/-- The vacuum has zero potential. -/
theorem vacuum_zero_potential : higgsPotential 1 = 0 := Jcost_unit0
THEOREM higgs_symmetric · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean
/-- The potential is symmetric about the vacuum. -/
theorem higgs_symmetric {r : ℝ} (hr : 0 < r) :
higgsPotential r = higgsPotential r⁻¹ := Jcost_symm hr
THEOREM higgs_unique_minimum · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean
/-- The vacuum is the unique minimum. -/
theorem higgs_unique_minimum {r : ℝ} (hr : 0 < r) :
higgsPotential r = 0 ↔ r = 1 := by
unfold higgsPotential
constructor
· intro h
by_contra hne
exact absurd h (ne_of_gt (Jcost_pos_of_ne_one r hr hne))
· rintro rfl; exact Jcost_unit0
THEOREM higgs_nonneg · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean
/-- The potential is non-negative (all field values above vacuum). -/
theorem higgs_nonneg {r : ℝ} (hr : 0 < r) : 0 ≤ higgsPotential r :=
Jcost_nonneg hr
What this page does not claim
This does not derive the numerical value of the Higgs mass or the VEV from first principles. This does not prove the standard model Higgs mechanism is physically correct. This does not claim the physical bridge from recognition events to the electroweak VEV is closed.
Verify this page
Every tagged claim above names its theorem. To check one yourself rather than trust this page, elaborate the source module with Lean 4 and audit its axiom basis:
$ lake env lean IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
A page whose claims cannot be reproduced this way does not ship. In production, every anchor links to the exact declaration in the public source release, and this block carries the build receipt for the page itself.
Derived articles
This page is generated by a question-recursion engine: the questions its answers raise become the next pages. The current agenda, with open targets marked red:
- What physical measurement would confirm or falsify the recognition-vacuum interpretation of the Higgs potential?
- How does the calibration condition V''(1) = 1 connect RS units to the measured Higgs mass in GeV?
- What remains open in deriving the electroweak VEV from recognition events rather than assuming it?
- How does the J-cost function relate to the standard model's quartic potential away from the minimum?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM vacuum_zero_potential · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean
/-- The vacuum has zero potential. -/ theorem vacuum_zero_potential : higgsPotential 1 = 0 := Jcost_unit0The declaration vacuum_zero_potential proves higgsPotential 1 = 0, meaning the potential is zero at the vacuum. vacuum_zero_potential · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.leanTHEOREM higgs_symmetric · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean
/-- The potential is symmetric about the vacuum. -/ theorem higgs_symmetric {r : ℝ} (hr : 0 < r) : higgsPotential r = higgsPotential r⁻¹ := Jcost_symm hrThe potential is symmetric about the vacuum, J(r) = J(r⁻¹). higgs_symmetric · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.leanTHEOREM higgs_unique_minimum · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean
/-- The vacuum is the unique minimum. -/ theorem higgs_unique_minimum {r : ℝ} (hr : 0 < r) : higgsPotential r = 0 ↔ r = 1 := by unfold higgsPotential constructor · intro h by_contra hne exact absurd h (ne_of_gt (Jcost_pos_of_ne_one r hr hne)) · rintro rfl; exact Jcost_unit0The vacuum is the unique minimum, the only place where the potential reaches zero. higgs_unique_minimum · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.leanTHEOREM higgs_nonneg · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean
/-- The potential is non-negative (all field values above vacuum). -/ theorem higgs_nonneg {r : ℝ} (hr : 0 < r) : 0 ≤ higgsPotential r := Jcost_nonneg hrThe potential is non-negative for all positive field values. higgs_nonneg · IndisputableMonolith/Foundation/QRFT/HiggsPotentialFromRecognitionVacuum.lean