Encyclopedia Materials Materials High Tc Superconductor From Phi Ladder Critical Temp Mono

ARTICLE 3 claims 3 theorems

Materials High Tc Superconductor From Phi Ladder Critical Temp Mono

A machine-checked theorem proves that higher rungs on a golden-ratio ladder always mean higher critical temperatures, but it says nothing about real materials.

The monotone ladder

In condensed matter physics, the critical temperature Tc is the temperature below which a material becomes superconducting, losing all electrical resistance. The Recognition Science framework models Tc as a function of a discrete index k, called a rung, where the temperature is set by phi raised to the power k. Here phi is the golden ratio, approximately 1.618, a number that appears throughout mathematics and nature.

The framework's machine-checked library of formal theorems proves a simple monotonicity statement: for any natural number k, the critical temperature at rung k is strictly less than the critical temperature at rung k+1. In plain language, higher rungs always mean higher temperatures. The proof is short and mechanical: since phi is greater than 1, multiplying a positive power of phi by phi again makes it strictly larger. This is the declaration criticalTempMono.

The framework also defines five canonical families of high-temperature superconductors: cuprates, iron-based, nickelates, heavy fermion, and organic. A separate theorem proves there are exactly five such families. The framework's model places the phonon coupling, the vibration that mediates electron pairing, at a canonical band where the cost function J equals zero at unity, which it identifies as the equilibrium condition for superconductivity.

What criticalTempMono does not claim is any empirical prediction. It establishes a purely formal relationship between an index and a computed temperature within the framework's model. It does not assert that any real material's Tc follows this ladder, nor does it assign specific rung numbers to specific compounds. The docstring mentions a cuprate example (YBa2Cu3O7 at about 93 K) and a phonon timescale, but these are illustrative identifications, not theorems. The gap between the formal ladder and measured laboratory values remains a target for future work, not a result of this declaration.

THEOREM criticalTempMono · IndisputableMonolith/Materials/HighTcSuperconductorFromPhiLadder.lean
theorem criticalTempMono (k : ℕ) : criticalTemp k < criticalTemp (k + 1) := by
  unfold criticalTemp
  have hpos := pow_pos phi_pos k
  rw [pow_succ]
  linarith [mul_lt_mul_of_pos_left one_lt_phi hpos]
THEOREM highTcFamilyCount · IndisputableMonolith/Materials/HighTcSuperconductorFromPhiLadder.lean
theorem highTcFamilyCount : Fintype.card HighTcFamily = 5 := by decide
THEOREM phonon_coupling_canonical · IndisputableMonolith/Materials/HighTcSuperconductorFromPhiLadder.lean
/-- Phonon coupling at canonical band triggers superconductivity. -/
theorem phonon_coupling_canonical : Jcost 1 = 0 := Jcost_unit0

What this page does not claim

No real material's critical temperature is asserted to follow the phi-ladder. No specific rung number is assigned to any measured compound in this declaration. The framework does not prove that phonon coupling at the canonical band causes superconductivity in any physical system.

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/Materials/HighTcSuperconductorFromPhiLadder.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)

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