Virtual Particle Creation Rate Near an Event Horizon

tampora
Messages
6
Reaction score
0
In class, our instructor talked about a pecularity of black holes. When virtual particles come into existence for an instant at the event horizon, sometimes one is trapped by the black hole, while the other is able to escape.

My question is, what determines the rate at which particles are created and ejected? Specifically, how come some particular black hole results in the creation of 10 particles per second, instead of 1000?

It seems like "drawing something from nothing" in the case of particle/antiparticle pairs could happen at an infinite rate, so why does it settle at whatever rate it really is?
 
Physics news on Phys.org
It's all about quantum field theory. While vacuum is constantly in this boiling state of particles and anti-particles, the rate at which something can actually interact with these, such as gravity of the black hole, is finite. Of course, there is connection between this rate and the quantity known as the biggest mistake of theoretical physics. So to say that it's completely understood would be a lie. But the theory still predicts a finite rate of radiation.
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...

Similar threads

Back
Top