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N⊥≲2×104N_\perp\lesssim2\times10^4

Why this formula appears here

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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N⊥N_\perp

Symbol N_perp

NpN_perp is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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Published contexts (1)

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N⊥≲2×104N_\perp\lesssim2\times10^4

Equation 33 · Evolutionary Physics

A Horizon Is a Toll Booth, Not a Loophole

This mathematical expression combines the displayed quantities; its precise role follows from the surrounding article text.

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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