- #1
PhDnotForMe
- 56
- 3
Hawking Radiation says that an antiparticle and particle spontaneously appear and annihilate each other everywhere, but at the horizon, if the antiparticle appearing inside the horizon and the particle appears outside, then the antiparticle is sucked in and the particle is emitted outward. Hawking radiation would be the particles being emitted away. The antiparticles are sucked in and, if the black hole is small enough, all the antiparticles will eventually completely annihilate the black hole.
What I am confused about is why would the black hole lose any mass at all. This relies on the premise that more often than not, the antiparticle will be the particle that appears on the inside of the horizon while the (regular) particle will be the particle to appear on the outside.
Intuitively, it would seem to me that 50% of the time, the antiparticle would appear on the inside while the other 50% of the time the (regular) particle would be the one to appear on the inside.
Why is it that the antiparticle is assumed to be the one appearing inside the horizon more than the (regular) particle?
What I am confused about is why would the black hole lose any mass at all. This relies on the premise that more often than not, the antiparticle will be the particle that appears on the inside of the horizon while the (regular) particle will be the particle to appear on the outside.
Intuitively, it would seem to me that 50% of the time, the antiparticle would appear on the inside while the other 50% of the time the (regular) particle would be the one to appear on the inside.
Why is it that the antiparticle is assumed to be the one appearing inside the horizon more than the (regular) particle?