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Three Roads To Quantum Gravity

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BLACK HOLES ARE HOT<br />

89<br />

The other moves away from the<br />

black hole. It is correlated with the<br />

one lost beyond the horizon. Because<br />

of this its properties are random.<br />

The result is that heat is generated<br />

One falls in and<br />

disappears behind<br />

the horizon.<br />

All information<br />

about it is<br />

apparently lost<br />

to outside<br />

observers<br />

A pair of photons are<br />

created just outside the<br />

horizon, in a correlated<br />

state as in the EPR<br />

experiment<br />

time<br />

space<br />

Horizon<br />

Singularity<br />

FIGURE 18<br />

Radiation from black holes, as discovered by Stephen Hawking. The photon<br />

that travels away from the black hole has random properties and motion<br />

because it is correlated, as in one of the photons in Figure 17, with the one<br />

lost behind the horizon. Because observers outside the horizon cannot<br />

recover the information that the infalling photon carries, the outmoving<br />

photon appears to have a thermal motion, like a molecule in a hot gas. The<br />

result is that the radiation leaving the black hole has a non-zero temperature.<br />

It also has an entropy, which is a measure of the missing information.<br />

consistent with the fact that there is no hidden region, so no<br />

horizon. But with the black hole there are an in®nite number<br />

of observers who agree that there is a horizon, beyond which<br />

they cannot see. And this is not just a consequence of their<br />

motion, for all observers who do not fall through the horizon<br />

will agree that the black hole and its horizon are there. This<br />

means that all observers who are far from a black hole will<br />

agree that it has a temperature and an entropy.

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