I'm struggling to understand the Bose enhancement in reheating. I've read that:
- At the end of inflation, the inflaton field, ϕ, is something like a condensate with excitations of a single momentum, say pμ=(mϕ,0) in the rest frame.
- The inflatons decay into pairs of bosons, say bb, with qμ=(mϕ/2,±→p), with →p fixed by conservation of energy.
- The Fock space of the b field is filled with states of momentum →p.
- This results in "Bose enhancement" of the decay ϕ→bb.
Why do the large occupation numbers for the final state b enhance the decay rate ϕ→bb? Also, why can we assume that the inflaton field is like a condensate with excitations of the same momenta?
I've seen some arguments with matrix elements,
|⟨nϕ−1,nk+1,n−k+1|a†ka†−kaϕ|nϕ,nk,n−k⟩|2∝nkn−k
but I find them surprising. Is there a physical/intuitive way to understand the enhancement? Is it reasonable to think of the CPT process? I suppose I find it intuitive that bb→ϕ with ϕ at threshold could be enhanced by high occupation numbers for the correct b momenta.
This post imported from StackExchange Physics at 2014-04-13 14:41 (UCT), posted by SE-user innisfree