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Equation 93 · Part 3 · The Bit Comes Back Before the Bearing

Symbol pi

t∗∼(β/2π)ln⁡St_* \sim (\beta/2\pi)\ln S
π\pi

What this part means

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

Its job in the formula

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

The passage around this formula

One honest caveat belongs here rather than in a footnote. The estimate t∗t_* ∼\sim (β\beta/2π\pi)ln⁡\ln S treats emission as though every mode escaped with equal ease, when a real Schwarzschild hole’s greybody factors suppress low-angular-momentum, long-wavelength quanta relative to a naive blackbody count. That suppression changes the effective rate at which new, usable radiation becomes available by an order-one-to-few numerical factor; it does not change the logarithmic scaling in S that makes t∗t_* so much shorter than the hole’s own light-crossing or evaporation timescales, and it is exactly the kind of correction the fast-scrambling conjecture was framed to survive [ 2 ] . The millisecond figure…

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