Equation 32 · A Horizon Is a Toll Booth, Not a Loophole
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A concrete number anchors the scale before the subtler chaining question is addressed. A superconducting transmon-style qubit with a transition frequency near 5\, carries a local energy gap H-=hf3.310^{-24}\, . Substituted into the instantaneous rate 2( H-)/ , this gives an upper ceiling of roughly 210^{10} orthogonal state changes per proper second; over one proper microsecond of continuous operation, 210^4 . Real superconducting processors run single-qubit gates in tens of nanoseconds, a realized rate several orders of magnitude below this ceiling. The Levitin-Toffoli bound is, in…
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A concrete number anchors the scale before the subtler chaining question is addressed. A superconducting transmon-style qubit with a transition frequency near 5\, carries a local energy gap H-=hf3.310^{-24}\, . Substituted into the instantaneous rate 2( H-)/ , this gives an upper ceiling of roughly 210^{10} orthogonal state changes per proper second; over one proper microsecond of continuous operation, 210^4 . Real superconducting processors run single-qubit gates in tens of nanoseconds, a realized rate several orders of magnitude below this ceiling. The Levitin-Toffoli bound is, in present hardware, nowhere near the binding constraint on gate speed — a fact worth stating before any horizon-based argument is allowed to treat this bound as the scarce resource being redistributed by gravity, when ordinary control engineering has not yet come close to spending what flat spacetime already allows.
Sources cited in the article section
- [3] Quantum Limits to Dynamical Evolution ↗
- [5] Ultimate Physical Limits to Computation ↗
- [4] Energy-Time Uncertainty Relation for Driven Quantum Systems ↗
These citations give research context. Read each source to check which claims it supports.
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