Manuscript Hawk01-A@1 · Hawk01-A.tex · section · 11979653

Paired occupation sectors and the early resource

An explicit Hawking-mode completion and its nonidentifiability › Paired occupation sectors and the early resource · lines 1456–1524

Hawk01-A@1#eq:pairisometries, Hawk01-A@1#eq:pairweights, Hawk01-A@1#eq:pLsum, Hawk01-A@1#eq:pLclosed, Hawk01-A@1#eq:weightscomplete, Hawk01-A@1#eq:earlykey

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For each , pair successive occupation vectors:

Both codewords have the same exact energy . For even , the single unpaired vector is . Set

and define the transferable weight

Thus

Let , and write

A stored early system and an internal key are initially in the fixed state

The key sectors are degenerate. A common early-system energy may be added to every term and does not affect the construction. The resource (eq:earlykey) is independent of and is explicitly priced as four orthogonal early states. Its preparation is an additional assumption; it is not derived from the Hawking spectrum. A shared classical key would suffice for the reduced channels below, so this construction is not offered as a theorem that specifically requires Hayden–Preskill entanglement.

The residual source contains orthogonal states of energy , and orthogonal two-dimensional residual subspaces with isometries for the unpaired even sectors, also at energy . Their existence is part of the declared source-sector dimension ledger.

Displayed formulas in this passage

  • Hawk01-A@1#eq:pairisometries · line 1459

  • Hawk01-A@1#eq:pairweights · line 1470

  • Hawk01-A@1#eq:pLsum · line 1477

  • Hawk01-A@1#eq:pLclosed · line 1477

  • Hawk01-A@1#eq:weightscomplete · line 1489

  • Hawk01-A@1#eq:earlykey · line 1502

  • unlabeled · line 1497

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