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在弱合的斯-爱因斯坦凝结体中观察动量空间约瑟夫森效应
Annesh Mukhopadhyay1, Xi-Wang Luo2,3,4, Colby Schimelfenig1
1Department of Physics and Astronomy, <a href="https://ror.org/05dk0ce17">Washington State University</a>, Pullman, Washington 99164-2814, USA.
Physical review letters
|June 21, 2024
概括
我们实验观察了波斯-爱因斯坦凝聚体 (BEC) 中的动量空间约瑟夫森效应,使用自旋轨道合. 这种异国情调的现象类似于Josephson效应,为量子模拟和传感开辟了新的途径.
科学领域:
- 原子,分子和光学物理学
- 凝聚物质物理学 凝聚物质物理学
- 量子模拟的量子模拟
背景情况:
- 动量空间约瑟夫森效应涉及在离散动量状态下波斯-爱因斯坦凝聚体 (BECs) 之间的超电流.
- 在BEC中,旋转轨道合提供了一个探索奇特量子现象的平台.
研究的目的:
- 为了实验观察动量空间约瑟夫森效应在BEC与拉曼诱导的自旋轨道合.
- 为了研究与ac约瑟夫森效应类似的连贯旋转动量振荡.
- 为了探索约瑟夫森等离子频率与博戈卢布夫间隙之间的联系.
主要方法:
- 使用带有拉曼诱导自旋轨道合的BEC.
- 实现带最小值之间的道化,使用光学格子动量.
- 通过突然灭拉曼调节,诱导连贯振荡.
主要成果:
- 在不同的参数模式下观察到等离子体和正规约瑟夫逊振荡.
- 实验结果与理论模型和数值模拟一致,突出非线性相互作用.
- 测量的约瑟夫森血频率提供了博戈利乌博夫的零准时差.
结论:
- 该研究成功地在可控制的实验设置中证明了动量空间约瑟夫森效应.
- 这些发现建立了约瑟夫森振荡与基本性质 (如伪金石模式质量) 之间的联系.
- 这项工作为使用动量状态作为合成自由度的量子模拟和传感提供了一个新的平台.
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