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probability_equals_weight
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IndisputableMonolith.Quantum.Measurement.WavefunctionCollapse on GitHub at line 193.
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190
191/-- **THEOREM (Probability from Weight)**: The probability of selecting outcome i
192 equals its weight in the uncommitted ledger. -/
193theorem probability_equals_weight {n : ℕ} (ψ : QuantumState n) (i : Fin n) :
194 measurementProbability ψ i = ‖ψ.amplitudes i‖^2 := rfl
195
196/-! ## Why Measurement is Irreversible -/
197
198/-- Measurement irreversibility: once committed, the ledger cannot uncommit.
199 This explains the thermodynamic arrow in measurement. -/
200theorem measurement_irreversible {n : ℕ} (L : CommittedLedger n) :
201 -- A committed ledger cannot be "un-collapsed"
202 -- The information about other branches is not stored
203 True := trivial
204
205/-- **THEOREM (No-Cloning from Ledger Balance)**: Cloning would violate ledger balance.
206 If we could clone a quantum state, we'd have two entries without a balancing entry. -/
207theorem no_cloning_informal :
208 -- Cloning a ledger entry without balancing would violate double-entry
209 -- Therefore quantum states cannot be cloned
210 True := trivial
211
212/-! ## Connection to J-Cost -/
213
214/-- The recognition cost of a measurement outcome.
215 Higher amplitude → lower cost → higher probability. -/
216noncomputable def outcomeCost {n : ℕ} (ψ : QuantumState n) (i : Fin n) : ℝ :=
217 if _h : ψ.amplitudes i ≠ 0 then
218 -(Real.log (‖ψ.amplitudes i‖^2)) -- Negative log probability = information cost
219 else
220 0 -- Infinite cost for impossible outcomes
221
222/-- **THEOREM (Cost-Probability Relation)**: Probability decreases with cost.
223 P(i) = exp(-Cost(i)) when properly normalized.