Encyclopedia Qft Qft Renormalization Group Rs
ARTICLE 3 claims 2 theorems 1 model
Qft Renormalization Group Rs
The renormalization group describes how physical quantities change with observation scale; Recognition Science models this with a cost function that vanishes when masses match energies.
The Renormalization Group in RS
The renormalization group is a standard tool in quantum field theory. It tracks how coupling constants, masses, and other parameters flow as the energy scale of an experiment changes. In quantum chromodynamics, the one-loop beta function predicts asymptotic freedom: the strong force weakens at high energies. The coefficient b_0 = 11N_c/3 - 2N_f/3, where N_c is the number of colors and N_f the number of flavors, determines this flow.
In Recognition Science, the framework models this same structure through a recognition cost, a measure of the price reality pays to distinguish two quantities. The module defines domainCost(m, e) = Jcost(m/e), where Jcost(x) = (x + 1/x)/2 - 1. This cost vanishes when the mass m equals the energy e, is nonnegative for positive inputs, and the canonical threshold phi - 3/2 is positive. These three facts are proved in the machine-checked library of formal theorems.
The research note attached to the module records an intended identification: colors N_c = 3 as the configuration dimension, flavors N_f = 6 as twice that, giving b_0 = 7 = 2^3 - 1. The note calls this exact, but the formal proofs establish nothing specific to quantum chromodynamics. The definition of domainCost uses only the ratio m/e, without reference to colors, flavors, or any QFT quantity.
What the module actually establishes is a template. The three proved facts about domainCost hold for any positive m and e. The structure RGFlowCert packages these properties, and cert_inhabited shows such a certificate exists. This is a general statement about the cost function, not a theorem about the renormalization group. The bridge from the cost template to QFT's beta function remains open.
MODEL domainCost · IndisputableMonolith/QFT/Renormalization_Group_RS.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)
THEOREM domainCost_at_eq · domainCost_nonneg · canonicalThreshold_pos · IndisputableMonolith/QFT/Renormalization_Group_RS.lean
theorem domainCost_at_eq (r : ℝ) (h : r ≠ 0) : domainCost r r = 0 := by
unfold domainCost; rw [div_self h]; exact Jcost_unit0
theorem domainCost_nonneg (m e : ℝ) (hm : 0 < m) (he : 0 < e) : 0 ≤ domainCost m e := by
unfold domainCost; exact Jcost_nonneg (div_pos hm he)
theorem canonicalThreshold_pos : 0 < canonicalThreshold := by
unfold canonicalThreshold; linarith [phi_gt_onePointFive]
THEOREM domainCost · IndisputableMonolith/QFT/Renormalization_Group_RS.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)
What this page does not claim
The module does not prove b_0 = 7 for QCD. The research note's color and flavor identification is not a formal result. No claim is made that the renormalization group flow in nature follows Jcost.
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/QFT/Renormalization_Group_RS.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 definition of m and e in QFT's own terms would make domainCost a theorem about the renormalization group?
- Does the cost template Jcost(m/e) connect to the beta function through a deeper forcing chain?
- How does the canonical threshold phi - 3/2 relate to asymptotic freedom?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
MODEL domainCost · IndisputableMonolith/QFT/Renormalization_Group_RS.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)The module defines domainCost(m, e) = Jcost(m/e), where Jcost(x) = (x + 1/x)/2 - 1. domainCost · IndisputableMonolith/QFT/Renormalization_Group_RS.leanTHEOREM domainCost_at_eq · domainCost_nonneg · canonicalThreshold_pos · IndisputableMonolith/QFT/Renormalization_Group_RS.lean
theorem domainCost_at_eq (r : ℝ) (h : r ≠ 0) : domainCost r r = 0 := by unfold domainCost; rw [div_self h]; exact Jcost_unit0theorem domainCost_nonneg (m e : ℝ) (hm : 0 < m) (he : 0 < e) : 0 ≤ domainCost m e := by unfold domainCost; exact Jcost_nonneg (div_pos hm he)theorem canonicalThreshold_pos : 0 < canonicalThreshold := by unfold canonicalThreshold; linarith [phi_gt_onePointFive]This cost vanishes when the mass m equals the energy e, is nonnegative for positive inputs, and the canonical threshold phi - 3/2 is positive. domainCost_at_eq · domainCost_nonneg · canonicalThreshold_pos · IndisputableMonolith/QFT/Renormalization_Group_RS.leanTHEOREM domainCost · IndisputableMonolith/QFT/Renormalization_Group_RS.lean
def domainCost (m e : ℝ) : ℝ := Jcost (m / e)The formal proofs establish nothing specific to quantum chromodynamics. domainCost · IndisputableMonolith/QFT/Renormalization_Group_RS.lean