02:08:07	David Marsh:	comment: just to agree with Chanda Schive et al is THE real classic here, and it’s the same picture for the QCD axion on small scales (e.g. Eggemeir’s simulations)
02:14:11	asimina arvanitaki:	I am a bit confused: in your paper you claim that relaxation due to self interactions depends on a single power of the coupling. Gravitational relaxation depends on the square of the coupling and it is enhanced because it is a long range interaction. Why are they different?
02:20:57	David Marsh:	AFAIK the sign of g determines the condensate size (linear in g), but both cases are attractive in the GPP equations (coupling squared). Jiajun Chen studied this in simulations, but there is an update to the paper clarifying this, still to appear. (I hope I said this correctly)