Encyclopedia Chemistry Chemistry Superconducting Tc Bcs Ratio Approx
ARTICLE 6 claims 3 theorems 1 measured
Chemistry Superconducting Tc Bcs Ratio Approx
A machine-checked theorem places a phi-derived approximation to the BCS gap ratio between 1.7 and 2.1, a range that brackets the measured value.
The BCS ratio approximation
The BCS ratio is a number from the standard theory of superconductivity. In the Bardeen-Cooper-Schrieffer (BCS) theory, the energy gap Δ at absolute zero and the critical temperature Tc at which superconductivity disappears are linked by the ratio 2Δ₀/kTc. In the weak-coupling limit, this ratio equals π/e^γ, where γ is the Euler-Mascheroni constant, which evaluates to about 1.764. The ratio is a benchmark: real superconductors that follow BCS theory cluster near this value.
In the Recognition Science framework, the same ratio is approximated using the golden ratio φ, about 1.618. The framework defines the quantity bcsDeltaTcRatio as 2 times the natural logarithm of φ, plus 1. Since log(φ) is about 0.481, this gives 2(0.481) + 1, which is about 1.96. The framework's machine-checked library of formal theorems proves a theorem called bcs_ratio_approx: the value lies strictly between 1.7 and 2.1. This is a narrow band, and the measured BCS value of about 1.764 sits inside it.
What the theorem does not claim is as important as what it proves. The theorem does not prove that the BCS ratio equals 2 log(φ) + 1 exactly. It proves only the bracketing inequality, that the expression falls between 1.7 and 2.1. The framework does not claim to derive the BCS ratio from first principles; it offers a phi-based approximation that lands in the right ballpark. The definition of bcsDeltaTcRatio is a modeling choice, not a forced result, and the numerical agreement with the measured value is an empirical check, not a theorem.
The broader context in the framework is a ladder of superconducting families. The framework assigns each family a step on a phi-power ladder, with conventional superconductors at step 6, MgB2 at step 5, iron-based at step 4, cuprates at step 3, and a hypothetical room-temperature family at step 1. The critical temperature for a family is modeled as the reference temperature 300 K times (1/φ) raised to the step. This makes cuprates higher in Tc than conventional superconductors, and the ratio between cuprate and conventional Tc is proved to be exactly φ³. These ordering theorems are proved in the library; the mapping of families to steps is a definitional choice.
The practical lesson for a reader is that the framework offers a compact, checkable way to see why superconducting families fall in the order they do, and why the BCS ratio sits near 1.96 rather than far from 1.764. The approximation is not a derivation of BCS theory, and the framework does not claim to explain the microscopic mechanism of phonon-mediated pairing. It claims a structural pattern: phi-scaling organizes the family ordering, and a phi-based expression brackets the classic BCS ratio.
MEASURED bcsDeltaTcRatio · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- The BCS weak-coupling ratio Δ/Tc ≈ 1.76 is related to φ. -/
noncomputable def bcsDeltaTcRatio : ℝ := 2 * Real.log Constants.phi + 1
MODEL bcsDeltaTcRatio · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- The BCS weak-coupling ratio Δ/Tc ≈ 1.76 is related to φ. -/
noncomputable def bcsDeltaTcRatio : ℝ := 2 * Real.log Constants.phi + 1
THEOREM bcs_ratio_approx · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- The BCS ratio is approximately 1.96 (2*log(φ) + 1).
log(φ) ≈ 0.481, so 2*log(φ) + 1 ≈ 1.96
The actual BCS ratio is 2Δ₀/kTc = π/e^γ ≈ 1.764 for weak coupling.
Our φ-derived approximation is in the right ballpark. -/
theorem bcs_ratio_approx : (1.7 : ℝ) < bcsDeltaTcRatio ∧ bcsDeltaTcRatio < (2.1 : ℝ) := by
dsimp [bcsDeltaTcRatio]
-- Use proven bounds from Numerics.Interval.Log: 0.48 < log(φ) < 0.483
-- Constants.phi = (1 + √5)/2 = Real.goldenRatio
have h_phi_eq : Constants.phi = Real.goldenRatio := rfl
rw [h_phi_eq]
have hlo : (0.48 : ℝ) < Real.log Real.goldenRatio := Numerics.log_phi_gt_048
have hhi : Real.log Real.goldenRatio < (0.483 : ℝ) := Numerics.log_phi_lt_0483
constructor
· -- 1.7 < 2 * log(φ) + 1 ⟺ 0.35 < log(φ)
-- Since 0.48 > 0.35, we have log(φ) > 0.48 > 0.35
linarith
· -- 2 * log(φ) + 1 < 2.1 ⟺ log(φ) < 0.55
-- Since log(φ) < 0.483 < 0.55, we have the result
linarith
THEOREM bcs_ratio_approx · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- The BCS ratio is approximately 1.96 (2*log(φ) + 1).
log(φ) ≈ 0.481, so 2*log(φ) + 1 ≈ 1.96
The actual BCS ratio is 2Δ₀/kTc = π/e^γ ≈ 1.764 for weak coupling.
Our φ-derived approximation is in the right ballpark. -/
theorem bcs_ratio_approx : (1.7 : ℝ) < bcsDeltaTcRatio ∧ bcsDeltaTcRatio < (2.1 : ℝ) := by
dsimp [bcsDeltaTcRatio]
-- Use proven bounds from Numerics.Interval.Log: 0.48 < log(φ) < 0.483
-- Constants.phi = (1 + √5)/2 = Real.goldenRatio
have h_phi_eq : Constants.phi = Real.goldenRatio := rfl
rw [h_phi_eq]
have hlo : (0.48 : ℝ) < Real.log Real.goldenRatio := Numerics.log_phi_gt_048
have hhi : Real.log Real.goldenRatio < (0.483 : ℝ) := Numerics.log_phi_lt_0483
constructor
· -- 1.7 < 2 * log(φ) + 1 ⟺ 0.35 < log(φ)
-- Since 0.48 > 0.35, we have log(φ) > 0.48 > 0.35
linarith
· -- 2 * log(φ) + 1 < 2.1 ⟺ log(φ) < 0.55
-- Since log(φ) < 0.483 < 0.55, we have the result
linarith
MODEL tcFamilyK · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- Tc prediction in Kelvin for a family. -/
noncomputable def tcFamilyK (f : SuperconductorFamily) : ℝ :=
tcReferenceK * tcFamily f
THEOREM cuprate_conventional_ratio · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- Ratio between cuprate and conventional Tc follows φ^3.
(1/φ)^3 / (1/φ)^6 = φ^6 / φ^3 = φ^3 -/
theorem cuprate_conventional_ratio :
tcFamily .cuprate / tcFamily .conventional = Constants.phi ^ 3 := by
dsimp [tcFamily, tc_phonon, familyLadderStep]
-- (1/φ)^3 / (1/φ)^6 = φ^6/φ^3 = φ^3
have hφpos : 0 < Constants.phi := Constants.phi_pos
have hφne : Constants.phi ≠ 0 := ne_of_gt hφpos
have h3 : Constants.phi ^ 3 ≠ 0 := pow_ne_zero 3 hφne
have h6 : Constants.phi ^ 6 ≠ 0 := pow_ne_zero 6 hφne
field_simp
What this page does not claim
The BCS ratio is exactly 2 log(φ) + 1; the theorem only proves a bracketing inequality. The framework derives the BCS ratio from first principles; the expression is a modeling choice. The phi-ladder family classification explains the microscopic pairing mechanism in any superconductor.
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/Chemistry/SuperconductingTc.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 microscopic mechanism would explain why the phi-ladder steps correspond to physical superconducting families?
- Does the phi-based approximation to the BCS ratio improve with a more refined model of the energy gap?
- What empirical data would falsify the phi-ladder ordering of superconducting families?
- Can the framework derive the McMillan equation exponent from phi, as its docstring predicts?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
MEASURED bcsDeltaTcRatio · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- The BCS weak-coupling ratio Δ/Tc ≈ 1.76 is related to φ. -/ noncomputable def bcsDeltaTcRatio : ℝ := 2 * Real.log Constants.phi + 1The BCS ratio in the weak-coupling limit equals π/e^γ, where γ is the Euler-Mascheroni constant, which evaluates to about 1.764. bcsDeltaTcRatio · IndisputableMonolith/Chemistry/SuperconductingTc.leanMODEL bcsDeltaTcRatio · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- The BCS weak-coupling ratio Δ/Tc ≈ 1.76 is related to φ. -/ noncomputable def bcsDeltaTcRatio : ℝ := 2 * Real.log Constants.phi + 1In the Recognition Science framework, the same ratio is approximated using the golden ratio φ, about 1.618. bcsDeltaTcRatio · IndisputableMonolith/Chemistry/SuperconductingTc.leanTHEOREM bcs_ratio_approx · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- The BCS ratio is approximately 1.96 (2*log(φ) + 1). log(φ) ≈ 0.481, so 2*log(φ) + 1 ≈ 1.96 The actual BCS ratio is 2Δ₀/kTc = π/e^γ ≈ 1.764 for weak coupling. Our φ-derived approximation is in the right ballpark. -/ theorem bcs_ratio_approx : (1.7 : ℝ) < bcsDeltaTcRatio ∧ bcsDeltaTcRatio < (2.1 : ℝ) := by dsimp [bcsDeltaTcRatio] -- Use proven bounds from Numerics.Interval.Log: 0.48 < log(φ) < 0.483 -- Constants.phi = (1 + √5)/2 = Real.goldenRatio have h_phi_eq : Constants.phi = Real.goldenRatio := rfl rw [h_phi_eq] have hlo : (0.48 : ℝ) < Real.log Real.goldenRatio := Numerics.log_phi_gt_048 have hhi : Real.log Real.goldenRatio < (0.483 : ℝ) := Numerics.log_phi_lt_0483 constructor · -- 1.7 < 2 * log(φ) + 1 ⟺ 0.35 < log(φ) -- Since 0.48 > 0.35, we have log(φ) > 0.48 > 0.35 linarith · -- 2 * log(φ) + 1 < 2.1 ⟺ log(φ) < 0.55 -- Since log(φ) < 0.483 < 0.55, we have the result linarithThe framework's machine-checked library of formal theorems proves a theorem called bcs_ratio_approx: the value lies strictly between 1.7 and 2.1. bcs_ratio_approx · IndisputableMonolith/Chemistry/SuperconductingTc.leanTHEOREM bcs_ratio_approx · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- The BCS ratio is approximately 1.96 (2*log(φ) + 1). log(φ) ≈ 0.481, so 2*log(φ) + 1 ≈ 1.96 The actual BCS ratio is 2Δ₀/kTc = π/e^γ ≈ 1.764 for weak coupling. Our φ-derived approximation is in the right ballpark. -/ theorem bcs_ratio_approx : (1.7 : ℝ) < bcsDeltaTcRatio ∧ bcsDeltaTcRatio < (2.1 : ℝ) := by dsimp [bcsDeltaTcRatio] -- Use proven bounds from Numerics.Interval.Log: 0.48 < log(φ) < 0.483 -- Constants.phi = (1 + √5)/2 = Real.goldenRatio have h_phi_eq : Constants.phi = Real.goldenRatio := rfl rw [h_phi_eq] have hlo : (0.48 : ℝ) < Real.log Real.goldenRatio := Numerics.log_phi_gt_048 have hhi : Real.log Real.goldenRatio < (0.483 : ℝ) := Numerics.log_phi_lt_0483 constructor · -- 1.7 < 2 * log(φ) + 1 ⟺ 0.35 < log(φ) -- Since 0.48 > 0.35, we have log(φ) > 0.48 > 0.35 linarith · -- 2 * log(φ) + 1 < 2.1 ⟺ log(φ) < 0.55 -- Since log(φ) < 0.483 < 0.55, we have the result linarithThe theorem does not prove that the BCS ratio equals 2 log(φ) + 1 exactly. bcs_ratio_approx · IndisputableMonolith/Chemistry/SuperconductingTc.leanMODEL tcFamilyK · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- Tc prediction in Kelvin for a family. -/ noncomputable def tcFamilyK (f : SuperconductorFamily) : ℝ := tcReferenceK * tcFamily fThe critical temperature for a family is modeled as the reference temperature 300 K times (1/φ) raised to the step. tcFamilyK · IndisputableMonolith/Chemistry/SuperconductingTc.leanTHEOREM cuprate_conventional_ratio · IndisputableMonolith/Chemistry/SuperconductingTc.lean
/-- Ratio between cuprate and conventional Tc follows φ^3. (1/φ)^3 / (1/φ)^6 = φ^6 / φ^3 = φ^3 -/ theorem cuprate_conventional_ratio : tcFamily .cuprate / tcFamily .conventional = Constants.phi ^ 3 := by dsimp [tcFamily, tc_phonon, familyLadderStep] -- (1/φ)^3 / (1/φ)^6 = φ^6/φ^3 = φ^3 have hφpos : 0 < Constants.phi := Constants.phi_pos have hφne : Constants.phi ≠ 0 := ne_of_gt hφpos have h3 : Constants.phi ^ 3 ≠ 0 := pow_ne_zero 3 hφne have h6 : Constants.phi ^ 6 ≠ 0 := pow_ne_zero 6 hφne field_simpThe ratio between cuprate and conventional Tc is proved to be exactly φ³. cuprate_conventional_ratio · IndisputableMonolith/Chemistry/SuperconductingTc.lean