Why the earlier ledgers cannot supply H4

comparison is still required. The SYK–scalar evaporation model of Gaikwad, Kaushal, Mandal, and Wadia has its own preparation, low-energy, and large-$N$ assumptions GaikwadEtAl. Its geometrical conclusions and its reconstruction of microstate labels using repeated processes are not automatically a deterministic one-copy decoder for an arbitrary reference-entangled finite code. Such a bridge requires the four same-model obligations above.

Likewise, a horizonless asymptotic geometry by itself does not prove complete residual constancy. A CPTP decoder by itself does not construct a local radiation receiver.