theorem
proved
iqhe_conductance_integer
show as:
view math explainer →
open explainer
Generate a durable explainer page for this declaration.
open lean source
IndisputableMonolith.Physics.QuantumHallEffect on GitHub at line 63.
browse module
All declarations in this module, on Recognition.
explainer page
depends on
formal source
60def iqhe_filling (n : ℕ) : ℚ := n
61
62/-- For IQHE: σ_xy = ν × e²/h with ν ∈ ℤ. -/
63theorem iqhe_conductance_integer (n : ℕ) :
64 ∃ σ : ℕ, σ = n := ⟨n, rfl⟩
65
66/-- The von Klitzing constant R_K = h/e² is the resistance quantum. -/
67-- R_K ≈ 25812.807 Ω (exact in the 2019 SI revision)
68abbrev von_klitzing_constant : ℝ := 25812.807 -- Ohms
69
70/-- R_K is positive. -/
71theorem RK_positive : 0 < von_klitzing_constant := by norm_num
72
73/-! ## Landau Levels -/
74
75/-- **LANDAU QUANTIZATION**: E_n = ℏω_c(n + 1/2)
76 The factor 1/2 is the zero-point energy of spin-1/2 fermions.
77 In RS: the 1/2 comes from the 4-tick (half-period) fermionic phase. -/
78noncomputable def landau_energy (n : ℕ) (ω_c : ℝ) : ℝ :=
79 ω_c * (n + 1/2)
80
81/-- Landau levels are equally spaced. -/
82theorem landau_spacing (n : ℕ) (ω_c : ℝ) (hω : 0 < ω_c) :
83 landau_energy (n+1) ω_c - landau_energy n ω_c = ω_c := by
84 unfold landau_energy
85 push_cast
86 ring
87
88/-- Zero-point energy is 1/2 ℏω_c — the fermionic half-period contribution. -/
89theorem zero_point_energy (ω_c : ℝ) :
90 landau_energy 0 ω_c = ω_c / 2 := by
91 unfold landau_energy
92 ring
93