http://arxiv.org/abs/1311.0537
Two particles can collide inside a black hole in such a way that the energy E_{c.m.} in their centre of mass frame becomes as large as one likes. We show that this effect can be understood with the help of simple analogy with particle collision in the flat space-time. We also expand our previous results and demonstrate new scenarios with unbound E_{c.m.}. In contrast to the previous scenarios which required proximity of collision to the bifurcation point, now this is not necessary. Full classification of scenarios with unbound E_{c.m.} is suggested.
Tue, 5 Nov 13
65/73
You must be logged in to post a comment.