Macroscopic Angular Momentum States of Bose-Einstein Condensates in Toroidal Traps
arXiv:cond-mat/9711295
Abstract
We consider a Bose-Einstein condensate (BEC) of $N$ atoms of repulsive interaction $\sim U_0$, in an elliptical trap, axially pierced by a Gaussian-intensity laser beam, forming an effective (quasi-2D) toroidal trap with minimum at radial distance $Ï= Ï_p$. The macroscopic angular momentum states $Ψ_l(Ï,θ) \sim \sqrt{N}Φ_l(Ï) e^{i l θ}$ for integer $l$ spread up to $Ï\lesssim Ï_{max} \sim (NU_0)^{1/4} \gg Ï_p$. The spreading lowers rotational energies, so estimated low metastability barriers can support large $l \lesssim l_{max} \sim (NU_0)^{1/4}, \lesssim 10$ for typical parameters. The $l$-dependent density profile $|Φ_l(Ï)|^2 - |Φ_0(Ï)|^2$ is a signature of BEC rotation. Results are insensitive to off-axis laser displacements $Ï_0$, for $Ï_0/Ï_{max} \ll 1$.
4 pages, 2 figures (included), submitted to Phys. Rev. Lett