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superconducting_gap
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IndisputableMonolith.Engineering.RoomTempSuperconductivityStructure on GitHub at line 110.
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107/-- The superconducting gap function Δ in RS.
108 Δ is proportional to E_coh reduced by the thermal competition ratio.
109 When T < T_c, gap Δ > 0 (superconducting); when T ≥ T_c, Δ = 0 (normal). -/
110def superconducting_gap (T : ℝ) (T_c : ℝ) (hTc : 0 < T_c) : ℝ :=
111 if T < T_c then E_coh * (1 - T / T_c) else 0
112
113/-- **THEOREM EN-002.7**: The superconducting gap is positive when T < T_c. -/
114theorem superconducting_gap_positive (T T_c : ℝ) (hTc_pos : 0 < T_c)
115 (hT_pos : 0 ≤ T) (hT_lt : T < T_c) :
116 superconducting_gap T T_c hTc_pos > 0 := by
117 unfold superconducting_gap
118 simp [hT_lt]
119 apply mul_pos rs_coherence_quantum_pos
120 rw [sub_pos, div_lt_one hTc_pos]
121 exact hT_lt
122
123/-- **THEOREM EN-002.8**: The gap vanishes at and above T_c. -/
124theorem gap_zero_above_tc (T T_c : ℝ) (hTc_pos : 0 < T_c)
125 (hT_ge : T_c ≤ T) :
126 superconducting_gap T T_c hTc_pos = 0 := by
127 unfold superconducting_gap
128 simp [not_lt.mpr hT_ge]
129
130/-- **THEOREM EN-002.9**: The gap is maximized at T = 0. -/
131theorem gap_max_at_zero (T_c : ℝ) (hTc_pos : 0 < T_c) :
132 superconducting_gap 0 T_c hTc_pos = E_coh := by
133 unfold superconducting_gap
134 simp [hTc_pos]
135
136/-! ## §IV. Room-Temperature Superconductivity Condition -/
137
138/-- The condition for ambient (room temperature) superconductivity:
139 The critical temperature rung must satisfy T_c(n) ≥ T_room. -/
140def ambient_sc_condition (n : ℤ) : Prop :=