论文标题
通过在零和非零的温度下搅拌在“赛道”原子电路中产生流动
Producing flow in "racetrack" atom circuits by stirring at zero and non-zero temperature
论文作者
论文摘要
我们介绍了一项研究,该研究如何通过用宽矩形屏障搅拌在“赛道”潜力中限制在“赛道”潜力中的Bose-Einstein冷凝物中产生宏观流动。该潜力由两个半圆道频道组成,这些通道由长度$ l $的直道隔开,如果$ l = 0 $,则是环的潜力。我们介绍了一系列模拟的结果,其中赛道冷凝物在不同的屏障高度,搅拌速度,赛马场几何形状和温度的不同条件下与屏障搅拌。我们发现,搅拌很容易在环和非环几何形状中产生循环,但是产生的确切流量很复杂。因此,我们还研究了在搅拌过程中产生流动的机制。我们发现,循环是由涡流/抗涡流对的互换,该涡流对最初是由抑制密度抑郁密度区域中冷凝物的回流产生的。当屏障强度达到临界值时,许多这些涡旋 - 换事件发生了快速连续的事件,因此产生的循环的流速足以超过屏障的搅拌速度。最初位于涡旋交换中涉及的涡流中的流量通过在涡旋交换过程中产生的成对的干扰转化为跑步周围的宏观流动。每对由一个涡流/抗涡流对组成,沿抗刺激方向移动,并在搅拌方向上移动一个压缩波。这种使流量机制的图片将使搅拌时间表的设计产生所需的流量。
We present a study of how macroscopic flow can be produced in Bose-Einstein condensate confined in a "racetrack" potential by stirring with a wide rectangular barrier. This potential consists of two half-circle channels separated by straight channels of length $L$ and is a ring potential if $L=0$. We present the results of a large set of simulations where racetrack condensates stirred with a barrier under varying conditions of barrier height, stir speed, racetrack geometry, and temperature. We found that stirring was readily able to produce circulation in ring and non-ring geometries but that the exact amount of flow produced was complicated. We therefore also studied the mechanism by which flow was produced in the stirring process. We found that circulation was induced by the swap of a vortex/anti-vortex pair that was initially created by backflow of the condensate in the region of depressed density by the barrier. When the barrier strength reached a critical value a number of these vortex-swap events occurred in rapid succession so that flow speed of the circulation produced was enough to exceed the stir speed of the barrier. Flow that was initially localized in the vortices involved in the vortex swap was converted into macroscopic flow around the racetrack by pairs of disturbances each generated during the vortex swap. Each pair consisted of a vortex/anti-vortex pair moving in the anti-stir direction and a compression wave moving in the stir direction. This picture of the mechanism for making flow will enable the design of stirring schedules that create a desired amount of flow.