Manuscript Hawk02-C@2 · Hawk02-C.tex · section · bb332d66

Exact emission, Volterra dynamics, and recovery

Exact emission, Volterra dynamics, and recovery · lines 812–830

The explicit-decoder and Bell-witness architecture agrees with the supplied comparison records in Hawk01-B and Hawk02-B CheungHawk01B ({thm:optima}) CheungHawk02B. No constant or leakage convention is imported.

For every code input, the exact expectation ledger is

ω_{0} = ω_{0} q (t) + \int_{0}^{\infty} ν ∣ f_{t} (ν) ∣^{2} d ν + 2 Re (A (t) ⟨ g, f_{t} ⟩) .

The interaction-energy term is not discarded in the general model.

Displayed formulas in this passage

unlabeled · line 821
$ω_{0} = ω_{0} q (t) + \int_{0}^{\infty} ν ∣ f_{t} (ν) ∣^{2} d ν + 2 Re (A (t) ⟨ g, f_{t} ⟩) .$

Nearby in this section

section: Exact emission, Volterra dynamics, and recovery
theorem: Theorem: Hamiltonian-derived complete emission