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Equation 29 · A Horizon Is a Toll Booth, Not a Loophole

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5 GHz5\,\mathrm{GHz}

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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\,GHz\mathrm{GHz} carries a local energy gap ⟨\langle H⟩\rangle-E0E_0=hf≈\approx3.3×\times10^{-24}\,J\mathrm J . Substituted into the instantaneous rate 2(⟨\langle H⟩\rangle-E0E_0)/π\piℏ\hbar , this gives an upper ceiling of roughly 2×\times10^{10} orthogonal state changes per proper second; over one proper microsecond of continuous operation, N⊥N_\perp≲\lesssim2×\times10^4 . 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\,GHz\mathrm{GHz} carries a local energy gap ⟨\langle H⟩\rangle-E0E_0=hf≈\approx3.3×\times10^{-24}\,J\mathrm J . Substituted into the instantaneous rate 2(⟨\langle H⟩\rangle-E0E_0)/π\piℏ\hbar , this gives an upper ceiling of roughly 2×\times10^{10} orthogonal state changes per proper second; over one proper microsecond of continuous operation, N⊥N_\perp≲\lesssim2×\times10^4 . 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.

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