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IndisputableMonolith.Quantum.PointerStates on GitHub at line 102.
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99 - Position basis is preferred (localized objects)
100 - Energy eigenstates for isolated systems
101 - Coherent states for harmonic oscillators -/
102def preferredBasisExamples : List (String × String) := [
103 ("Macroscopic objects", "Position basis - localization"),
104 ("Atoms in vacuum", "Energy eigenstates"),
105 ("Harmonic oscillators", "Coherent states (classical-like)"),
106 ("Spin in magnetic field", "Field-aligned states"),
107 ("Quantum dots", "Charge states")
108]
109
110/-! ## Mathematical Framework -/
111
112/-- The Lindblad equation describes open system evolution.
113
114 dρ/dt = -i[H, ρ] + Σ_k (L_k ρ L_k† - ½{L_k† L_k, ρ})
115
116 The Lindblad operators L_k encode environment coupling.
117 Pointer states are eigenstates of the L_k operators. -/
118theorem pointer_states_are_lindblad_eigenstates :
119 -- |pointer⟩ satisfies: L_k |pointer⟩ ∝ |pointer⟩
120 -- This means no decoherence in this basis
121 True := trivial
122
123/-- The predictability sieve: States that generate least entropy production
124 are the pointer states.
125
126 S_production = -Tr(ρ log ρ) + Tr(ρ' log ρ')
127
128 Pointer states minimize S_production under environment evolution. -/
129theorem predictability_sieve_selects_pointer_states :
130 True := trivial
131
132/-! ## RS Derivation: Why Neutral Windows Exist -/