I really don't think that this should become a name-calling thread so it should end soon; maybe there is no "firm" answer at this point.(?)
Perhaps there is a confusion about the semantics of the term "both particles can escape". Maybe it should be changed into "Two particles can escape", but several sites do mention that "both particles can escape", such as seen in:
http://www.alcyone.com/max/physics/laws/h.html
where it states:
"Hawking radiation (S.W. Hawking; 1973)
The theory that black holes emit radiation like any other hot body. Virtual particle-antiparticle pairs are constantly being created in supposedly empty space. Occasionally, a pair will be created just outside the event horizon of a black hole. There are three possibilities:
both particles are captured by the hole;
both particles escape the hole;
one particle escapes while the other is captured."
In that simple quote, the "both particles can escape" stands out like a sore thumb. The apparent problem is that most sites, like the one above, always mention that case # 2 is resolved by all that has been described so far, with one of the particles re-entering the EH and returning the "borrowed" energy, just like Ambitwistor has been saying all along. On that most common description I will agree 100%.
But, if changed into "two particles can escape", I know that I have read somewhere (that I can't find now) that the following (verbal) scenario can, and sometimes does, happen. This is from old memory and I have no math to "back it up":
(1)
Two virtual particles are created just outside the EH, very short-lived based on frequency and seperation; they exist for a very short time.
(2) Both particles re-combine and annihilate. No energy has yet been "returned" to the BH and is still unaccounted for at this point.
(3) On annihilation, the energy gained from the BH is converted into an electron and a positron, each traveling away in different directions. The BH is still waiting for equilibrium. The electron and positron are now
real particles.
(4) Any "lost" energy caused by the escape of the real particles is then returned to equilibrium
by the loss of mass of the BH equivalent to the energy of the escaping real particles. With both particles escaping, it just happens to be a little more mass than if just one had escaped; same process. At this point the black hole is back to equilibrium, and happy.
(5) Real particles which can be observed can only have positive energies. QM only allows the creation and destruction of virtual particles with
arbitrary energies. Virtual particles are not in the final state; They must finish their interactions before energies can be measaured, and the time scale is given by Heisenberg's uncertainty principle, delta E * delta t >= h/2pi. Negative-energy particles cannot "propagate". (
This part I did find!)
(6) Since
both have positive energies, there is no requirement for a replacement of any negative energy anywhere. That has already been done by the BH's mass loss.
That scenario is as much as I can remember on the subject. I might have left out an important point or three, or it could be that this has since been dumped or disproven. Either way, that is as far as I can go on this subject without more references.
Labguy