Abstract:
The perturbative Lee-Huang-Yang (LHY) interaction proportional to n
3/2
, where n is the density, creates an infinitely repulsive potential at the center of a Bose-Einstein condensate (BEC) with net attraction, which stops the
collapse to form a self-bound state in a dipolar BEC and in a binary BEC. However, recent microscopic calculations
of the non-perturbative beyond-mean-field (BMF) interaction indicate that the LHY interaction is valid only for very
small values of gas parameter x. We show that a realistic non-perturbative BMF interaction can stop collapse and form
a self-bound state only in a weakly attractive binary BEC with small x values (x / 0.01), whereas the perturbative
LHY interaction stops collapse for all attractions. We demonstrate these aspects using an analytic BMF interaction
with appropriate weak-coupling LHY and strong coupling limits.
