Physikalisches Institut der Universität Heidelberg, Heidelberg, Germany.
Max Planck Institute of Quantum Optics, Garching, Germany.
Nature. 2022 Jun;606(7913):287-291. doi: 10.1038/s41586-022-04678-1. Epub 2022 Jun 8.
The formation of strongly correlated fermion pairs is fundamental for the emergence of fermionic superfluidity and superconductivity. For instance, Cooper pairs made of two electrons of opposite spin and momentum at the Fermi surface of the system are a key ingredient of Bardeen-Cooper-Schrieffer (BCS) theory-the microscopic explanation of the emergence of conventional superconductivity. Understanding the mechanism behind pair formation is an ongoing challenge in the study of many strongly correlated fermionic systems. Controllable many-body systems that host Cooper pairs would thus be desirable. Here we directly observe Cooper pairs in a mesoscopic two-dimensional Fermi gas. We apply an imaging scheme that enables us to extract the full in situ momentum distribution of a strongly interacting Fermi gas with single-particle and spin resolution. Our ultracold gas enables us to freely tune between a completely non-interacting, unpaired system and weak attractions, where we find Cooper pair correlations at the Fermi surface. When increasing the attractive interactions even further, the pairs gradually turn into deeply bound molecules that break up the Fermi surface. Our mesoscopic system is closely related to the physics of nuclei, superconducting grains or quantum dots. With the precise control over the interactions, particle number and potential landscape in our experiment, the observables we establish in this work provide an approach for answering longstanding questions concerning not only such mesoscopic systems but also their connection to the macroscopic world.
强关联费米子对的形成对于费米超流和超导的出现是至关重要的。例如,系统费米面处由两个自旋相反、动量相反的电子组成的库珀对是巴丁-库珀-施里弗(BCS)理论的关键组成部分——这一理论对常规超导现象的微观解释。理解对形成的机制是许多强关联费米子系统研究中的一个持续挑战。因此,具有库珀对的可控多体系统是人们所期望的。在这里,我们直接观察到介观二维费米气体中的库珀对。我们应用一种成像方案,使我们能够以单粒子和自旋分辨率提取强相互作用费米气体的完整原位动量分布。我们的超冷气体使我们能够在完全非相互作用、不成对的系统和弱吸引之间自由切换,在那里我们在费米面处发现了库珀对相关。当进一步增加吸引力时,这些对逐渐变成深度束缚的分子,打破费米面。我们的介观系统与核物理、超导颗粒或量子点的物理密切相关。通过对我们实验中相互作用、粒子数和势场的精确控制,我们在这项工作中确立的可观测量提供了一种方法,可以回答不仅关于这些介观系统,而且关于它们与宏观世界的联系的长期存在的问题。