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Equation 15 · A Horizon Is a Toll Booth, Not a Loophole

What does this equation mean?

N≤2πℏ(⟨H⟩−E0)tN \leq \frac{2}{\pi\hbar}\left(\langle H\rangle-E_0\right) t

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This equation states a bound: one expression must stay on the indicated side of the other under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.

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NN

Symbol N

N 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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π\pi

Symbol pi

pi occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

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HH

Symbol H

H 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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E0E_0

Symbol E_0

the ground-state energy of H [ 2 , 1 ].

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tt

Symbol t

t 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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fraction

fraction

Divide the expression above the line by the one below it.

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subtraction

subtraction

Subtract the following term or group from the preceding one. A leading minus marks a negative quantity.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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22

Numerator: 2

The complete quantity above the fraction bar.

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πℏ\pi\hbar

Denominator: pihbar

The complete quantity below the fraction bar; it must be nonzero for this division.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction.

What the article says around this equation

where ⟨\langle H⟩\rangle is the mean energy in the evolving state and E0E_0 is the ground-state energy of H [ 2 , 1 ] . Inverting this gives a maximum rate of orthogonal state changes per unit proper time, 2(⟨\langle H⟩\rangle-E0E_0)/π\piℏ\hbar , and Giovannetti, Lloyd, and Maccone showed that for a periodic evolution this rate integrates cleanly: a system with mean energy ⟨\langle H⟩\rangle-E0E_0 above its ground state can pass through at most N≤2πℏ(⟨H⟩−E0)tN \leq \frac{2}{\pi\hbar}\left(\langle H\rangle-E_0\right) t. mutually orthogonal states in elapsed time t [ 3 ] . Lloyd used the same bound to price computation itself: no amount of clever engineering lets a system with energy E execute logical operations faster than about 2E/π\piℏ\hbar per second, a…
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where ⟨\langle H⟩\rangle is the mean energy in the evolving state and E0E_0 is the ground-state energy of H [ 2 , 1 ] . Inverting this gives a maximum rate of orthogonal state changes per unit proper time, 2(⟨\langle H⟩\rangle-E0E_0)/π\piℏ\hbar , and Giovannetti, Lloyd, and Maccone showed that for a periodic evolution this rate integrates cleanly: a system with mean energy ⟨\langle H⟩\rangle-E0E_0 above its ground state can pass through at most N≤2πℏ(⟨H⟩−E0)tN \leq \frac{2}{\pi\hbar}\left(\langle H\rangle-E_0\right) t. mutually orthogonal states in elapsed time t [ 3 ] . Lloyd used the same bound to price computation itself: no amount of clever engineering lets a system with energy E execute logical operations faster than about 2E/π\piℏ\hbar per second, a ceiling with nothing to do with any particular hardware [ 5 ] .

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