|<em>P</em>|<sub>max</sub> as a function of λ<sub><em>z</em></sub> for the case of negative scattering length and cylindrical symmetry for <em>G</em> = −0.03 and <em>G</em> = 0

2013-08-19T00:00:00Z (GMT) by Wei Qi Zhaoxin Liang Zhidong Zhang
<p><strong>Figure 9.</strong> |<em>P</em>|<sub>max</sub> as a function of λ<sub><em>z</em></sub> for the case of negative scattering length and cylindrical symmetry for <em>G</em> = −0.03 and <em>G</em> = 0.</p> <p><strong>Abstract</strong></p> <p>We take into account the higher-order corrections in two-body scattering interactions within a mean-field description, and investigate the stability conditions and collective excitations of a harmonically trapped Bose–Einstein condensate (BEC). Our results show that the presence of higher-order corrections causes drastic changes to the stability condition of a BEC. In particular, we predict that with the help of the higher-order interaction, a BEC can now collapse even for positive scattering lengths; whereas, a usually unstable BEC with a negative scattering length can be stabilized by positive higher-order effects. The low-lying collective excitations are significantly modified as well, compared to those without the higher-order corrections. The conditions for a possible experimental scenario are also proposed.</p>