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Pairing of fermionic lithium-6 throughout the BEC-BCS crossover.

机译:在整个BEC-BCS交换中,对铁离子锂6进行配对。

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The pairing of fermionic particles is an essential ingredient of superconductivity and of the superfluidity of 3He. While such phenomena are accurately described by BCS theory in the limit of weak pairing strength, a complete understanding remains elusive when pairing strength is increased, such as in high temperature superconductors. We create ultracold gases of trapped fermionic 6Li atoms, through which we directly observe fermionic pairing. In our system, there are no impurities whatsoever, and parameters such as the number and temperature of the trapped atoms are precisely and independently controlled. In addition, a Feshbach resonance enables the continuous tuning of interaction strength and sign between the paired atoms. This control allows us to observe the smooth crossover of a molecular Bose Einstein condensate (MBEC) to a superfluid of weakly interacting Cooper pairs. With these tools, we have performed several fundamental measurements of pairing in fermionic systems.; We use optical molecular spectroscopy to precisely measure the closed-channel contribution to the many body state of paired 6Li atoms within a broad Feshbach resonance. The magnitude of this contribution is small, and supports the concept of universality for the description of broad Feshbach resonances. Moreover, the dynamics of the excitation provide clear evidence for pairing across the BEC-BCS crossover, and for the first time, into the weakly interacting BCS regime.; We also prepare a polarized Fermi gas with unequal numbers of two spin states of 6Li atoms. The real-space densities of the polarized, strongly-interacting, two-component Fermi gas reveal two low temperature regimes. At the lowest temperatures, the gas separates into a phase with a uniformly paired superfluid core surrounded by a shell of normal, unpaired atoms. This phase separation is accompanied by a spatial deformation of the core. At higher temperatures, the uniformly paired core persists, though it does not deform. This temperature dependence is consistent with a tri-critical point in the phase diagram. These measurements of pairing in a polarized Fermi gas are relevant to predictions of exotic phases of quark matter and magnetized superconductors.
机译:铁离子颗粒的配对是3He超导性和超流动性的重要组成部分。虽然BCS理论在弱配对强度的极限中准确地描述了这种现象,但是当增加配对强度时(例如在高温超导体中),仍然很难完全理解。我们产生捕获的铁离子6Li原子的超冷气体,通过它们我们直接观察到铁离子配对。在我们的系统中,没有任何杂质,并且诸如被俘获原子的数量和温度之类的参数可以精确且独立地控制。此外,Feshbach共振使成对原子之间的相互作用强度和符号连续可调。这种控制使我们能够观察到分子玻色爱因斯坦凝聚物(MBEC)与弱相互作用的库珀对的超流体的平滑过渡。使用这些工具,我们已经完成了一些在费米离子系统中配对的基本测量。我们使用光学分子光谱法来精确测量闭路对广泛的Feshbach共振中成对6Li原子的许多体态的贡献。这种贡献的大小很小,并且支持通用性的概念来描述广泛的Feshbach共振。此外,激发的动力学为跨BEC-BCS交叉配对以及首次与弱相互作用的BCS配对配对提供了明确的证据。我们还准备了一个极化费米气体,其两个6Li原子的自旋态数不等。极化的强相互作用的两组分费米气体的实际空间密度显示出两种低温状态。在最低温度下,气体分离成具有均匀成对的超流体核的相,该核被正常的未成对原子的壳包围。这种相分离伴随着芯的空间变形。在较高的温度下,均匀配对的纤芯会保留,尽管它不会变形。该温度依赖性与相图中的三临界点一致。极化费米气体中的配对测量与夸克物质和磁化超导体奇异相的预测有关。

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