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IndisputableMonolith.Engineering.RoomTempSuperconductivityStructure on GitHub at line 70.
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67 norm_num
68
69/-- **THEOREM EN-002.3**: Room temperature thermal ratio is positive. -/
70theorem thermal_ratio_pos : 0 < thermal_ratio_room_temp := by
71 unfold thermal_ratio_room_temp
72 norm_num
73
74/-! ## §II. Critical Temperature from φ-Ladder -/
75
76/-- Critical temperature for the n-th rung of the φ-ladder.
77 T_c(n) = E_coh · φ^n / k_B (in suitable units).
78 The RS prediction: each material sits on a particular rung n. -/
79def T_c_rung (n : ℤ) : ℝ := phi ^ n
80
81/-- **THEOREM EN-002.4**: Critical temperature is positive for all rungs. -/
82theorem tc_rung_pos (n : ℤ) : 0 < T_c_rung n := by
83 unfold T_c_rung
84 apply zpow_pos phi_pos
85
86/-- **THEOREM EN-002.5**: Higher rungs give higher critical temperatures.
87 T_c(n+1) = φ · T_c(n) > T_c(n) since φ > 1. -/
88theorem phi_ladder_tc_monotone (n : ℤ) : T_c_rung n < T_c_rung (n + 1) := by
89 unfold T_c_rung
90 rw [zpow_add_one₀ phi_ne_zero]
91 have hphi_gt1 : 1 < phi := one_lt_phi
92 have hpos : 0 < phi ^ n := zpow_pos phi_pos n
93 exact lt_mul_of_one_lt_right hpos hphi_gt1
94
95/-- **THEOREM EN-002.6**: The φ-ladder spans all temperature scales.
96 For any temperature T > 0, there exists a rung n such that T_c(n) > T. -/
97theorem phi_ladder_unbounded (T : ℝ) (hT : 0 < T) :
98 ∃ n : ℤ, T < T_c_rung n := by
99 unfold T_c_rung
100 -- phi⁻¹ < 1 since phi > 1, so phi⁻¹^k → 0 as k → ∞