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Equation 64 · Part 2 · The Bit Comes Back Before the Bearing

Symbol β

t∗  ∼  β2π ln⁡S,β≡ℏkBTH=8πGMc3,t_* \;\sim\; \frac{\beta}{2\pi}\,\ln S, \qquad \beta \equiv \frac{\hbar}{k_BT_H} = \frac{8\pi GM}{c^3},
β\beta

What this part means

β occurs above the fraction bar. The numerator is divided by the entire denominator below it.

Its job in the formula

β occurs above the fraction bar. The numerator is divided by the entire denominator below it.

The passage around this formula

…the bound this conjecture leans on: the exponential growth rate of an out-of-time-order correlator, the operational signature of chaos, cannot exceed λL\lambda_L ≤\le 2π\pi/β\beta for a thermal system at inverse temperature β\beta , with a black hole horizon saturating the bound [ 3 ] . Combining a Lyapunov-limited spread over ln⁡\ln S e-foldings of the hole’s Bekenstein-Hawking entropy S gives the estimate t∗  ∼  β2π ln⁡S,β≡ℏkBTH=8πGMc3t_* \;\sim\; \frac{\beta}{2\pi}\,\ln S, \qquad \beta \equiv \frac{\hbar}{k_BT_H} = \frac{8\pi GM}{c^3}. where the second equality for a Schwarzschild hole follows directly from Hawking’s temperature…

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Sources cited in the surrounding passage

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