Manuscript Hawk02-E@1 · Hawk02-E.tex · theorem · 4841592b
Theorem: Exact microscopic conservation and bounded reservoir energy
Complete channels and exact microscopic accounting › Energy ledger · lines 772–832 · proof included or linked
Hawk02-E@1#thm:energy, Hawk02-E@1#eq:energy-conservation, Hawk02-E@1#eq:bath-energy-bound, Hawk02-E@1#eq:source-current, Hawk02-E@1#eq:interaction-energy
For every logical input, define
Then
Uniformly in the logical input and time,
The source current, with positive sign for loss from the source, is
Consequently,
No sign is asserted for either current at every time.
Proof. The initially prepared vectors belong to . Autonomous unitary evolution preserves the total Hamiltonian expectation. The initial bath and interaction means vanish, giving (eq:energy-conservation).
The form inequality (eq:lower-H) gives
which proves (eq:bath-energy-bound).
The particle-sector bounds established in Section sec:regulator also show that these prepared evolved vectors have finite moments of every fixed particle-number order on bounded time intervals. Since is bounded on the one-particle band, the commutator expectations can be obtained by finite-particle approximation. Differentiation gives . Differentiating (eq:energy-conservation) proves (eq:interaction-energy).
Displayed formulas in this passage
Hawk02-E@1#eq:energy-conservation · line 783
Hawk02-E@1#eq:bath-energy-bound · line 788
Hawk02-E@1#eq:source-current · line 794
Hawk02-E@1#eq:interaction-energy · line 801
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