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  1. Hawking found that the black hole temperature was T = κ/(2π), so ǫ = 1/(2π) and hence η = 1/4. This gives the famous Bekenstein-Hawking formula for the entropy

  2. Hawking has theorized that during pair produc-tion occurring just outside the event horizon, a black hole slowly loses mass or evaporates as particles are radiated away. This, now known as “Hawking radia-tion,” was initially described to many in his first popular book A Brief History of Time. In this

  3. C. The spectrum of Hawking radiation We want to equate hA "( )A "( 0)i vac:subtr: to an integral of the type Eq. (16) without the +1 2 contribution due to vacuum uctuations (which we have already subtracted). It is easiest to do this if we use the identity: sinhx x = Y1 n=1 1 + x2 (ˇn)2 ; (22)

  4. black hole radiation. In 1974, Stephen Hawking showed that black holes, which are objects that light cannot escape from and hence classically are at absolute zero, do radiate at temperature T H= ~c3 8ˇGMk b; (1.0.1) when quantum mechanical e ects are taken into account. The presence of both gravitational and quantum mechanical constants re

  5. Hawking radiation is the theoretical emission released outside a black hole's event horizon. This is counterintuitive because once ordinary electromagnetic radiation is inside the event horizon, it cannot escape. It is named after the physicist Stephen Hawking, who developed a theoretical argument for its existence in 1974. [1]

  6. 25 Μαΐ 2022 · In 1974, Stephen Hawking theoretically discovered that black holes emit thermal radiation and have a characteristic temperature, known as the Hawking temperature. The aim of this paper is to present a simple heuristic derivation of the Hawking temperature, based on the Heisenberg uncertainty principle.

  7. Hawking radiation is a key effect in quantum gravity. There are various derivations, including Hawking’s origi-nal one [1] calculating Bogoliubov coefficients, which have shown that the radiation is thermal with a blackbody spectrum at a temperature given by the surface gravity, TH = 2 . Derivations have been found also using. 1⁄4.

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