def
definition
rotationPhase
show as:
view math explainer →
open explainer
Read the cached plain-language explainer.
open lean source
IndisputableMonolith.Foundation.SpinStatistics on GitHub at line 39.
browse module
All declarations in this module, on Recognition.
explainer page
depends on
used by
formal source
36def IsBosonic (period : ℕ) : Prop := period % 4 = 0 ∧ period ≠ 4
37
38/-- The phase accumulated under a 2π rotation (4-tick advance). -/
39noncomputable def rotationPhase (period : ℕ) : ℂ :=
40 phaseExp ⟨4 % 8, by norm_num⟩
41
42/-- **KEY**: For fermions (4-tick period), the 2π rotation gives phase -1. -/
43theorem fermion_rotation_phase_neg_one :
44 rotationPhase 4 = -1 := by
45 unfold rotationPhase
46 exact phase_4_is_minus_one
47
48/-- For bosons (8-tick period), the 2π rotation gives phase +1 (via two half-cycles). -/
49theorem boson_rotation_phase_pos_one :
50 phaseExp ⟨0, by norm_num⟩ = 1 := phase_0_is_one
51
52/-! ## Exchange Statistics -/
53
54/-- Two-particle exchange involves one 2π rotation of the relative coordinate,
55 contributing the rotation phase. For fermions: -1. For bosons: +1.
56
57 This is the fundamental RS derivation of the exchange sign. -/
58theorem exchange_sign_fermion :
59 rotationPhase 4 = -1 := fermion_rotation_phase_neg_one
60
61theorem exchange_sign_boson :
62 phaseExp ⟨0, by norm_num⟩ * phaseExp ⟨0, by norm_num⟩ = 1 := by
63 rw [phase_0_is_one]; ring
64
65/-! ## The Spin-Statistics Theorem -/
66
67/-- **SPIN-STATISTICS THEOREM** (RS version):
68 The exchange sign of a two-particle state equals the rotation phase
69 of each particle under 2π rotation.