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

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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

  • unlabeled · line 775

  • unlabeled · line 817

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