Manuscript Hawk01-B@1 · Hawk01-B.tex · section · cfa976f1

Sequential conserving interface

Sequential conserving interface · lines 637–687

Hawk01-B@1#eq:cutoffenergy, Hawk01-B@1#eq:residualdimensions

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One finite field realization uses distinct neutral scalar species of equal dispersion in the same regulated s-wave energy mode. No additional conserved flavor number is imposed, and the specified couplings may mix the degenerate species. This is an artificial but explicit field-sector choice, not an identification of known astrophysical particles.

Exact energy conservation below concerns this energy-eigenmode regulator. A finite-time wavepacket is not an exact energy eigenmode. Replacing these sectors by finite-time collected packets requires a separate spectral-width and channel-error certificate.

and energy budget. The initial source energy is , and

The code is degenerate within that initial sector. Its logical Hamiltonian is zero after subtraction of the common sector energy.

. At prefix , the construction uses

The first summands record completed transfer time and key. The last summands contain a pending encrypted logical system. The growth of this particular ledger is disclosed; no claim that it models a decreasing black-hole microstate dimension is made.

The required finite isometries can be embedded in a larger fixed energy-sector Hilbert space and extended to block-energy-conserving unitaries on prepared source-plus-vacuum ports. Unused orthogonal states are included in that embedding. This finite-dimensional extension does not supply a local gravitational Hamiltonian.

Displayed formulas in this passage

  • Hawk01-B@1#eq:cutoffenergy · line 653

  • Hawk01-B@1#eq:residualdimensions · line 663

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