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Proposed method to realize the $p$-wave superfluid state using a $s$-wave superfluid Fermi gas with a synthetic spin-orbit interaction

机译:建议使用a实现$ p $ -wave超流体状态的方法   $ s $ -wave superfluid费米气体,具有合成自旋轨道相互作用

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摘要

We theoretically propose an idea to reach the $p$-wave superfluid phase in anultracold Fermi gas. The key of our idea is that the pairing symmetry of aFermi superfluid is fully dominated by the symmetry of the superfluid orderparameter, which is essentially given by the product of a pair amplitude and apairing interaction. Noting this, in our proposal, we first prepare a $p$-wavepair amplitude by, not using a $p$-wave interaction, but using the phenomenonthat a $p$-wave pair amplitude is induced in an $s$-wave superfluid Fermi gaswith antisymmetric spin-orbit interaction. In this case, although the system isstill in the $s$-wave superfluid state with the $s$-wave superfluid orderparameter, when one suddenly replaces the $s$-wave interaction by anappropriate $p$-wave one (which is possible in cold Fermi gases by using aFeshbach resonance technique), the product of the $p$-wave interaction and the$p$-wave pair amplitude that has already been prepared in the spin-orbitcoupled $s$-wave superfluid state immediately gives a finite $p$-wavesuperfluid order parameter. Thus, at least just after this manipulation, thesystem is in the $p$-wave superfluid state, being characterized by theartificially produced $p$-wave superfluid parameter. In this paper, to assessour idea, we evaluate the $p$-wave pair amplitude in a spin-orbit coupled$s$-wave superfluid Fermi gas at $T=0$. We determine the region where a large$p$-wave pair amplitude is obtained in the phase diagram with respect to thestrengths of the $s$-wave pairing interaction and the spin-orbit coupling. Wealso discuss the accessibility of this optimal region on the viewpoint of thesuperfluid phase transition temperature. Since the achievement of a $p$-wavesuperfluid Fermi gas is one of the most crucial issues in cold atom physics,our proposal would be useful for this exciting challenge.
机译:我们从理论上提出了一种在超极费米气体中达到$ p $波超流体相的想法。我们想法的关键是,费米超流体的配对对称性完全由超流体阶数参数的对称性决定,该对称性基本上由对振幅和配对相互作用的乘积给出。注意,在我们的建议中,我们首先通过不使用$ p $波相互作用,而是使用在$ s $波中感应出$ p $波对幅度的现象来准备$ p $波对幅度。具有反对称自旋轨道相互作用的超流体费米气体。在这种情况下,尽管系统仍以$ s $ -wave超流体阶数参数处于$ s $ -wave超流体状态,但当系统突然将$ s $ -wave交互作用替换为适当的$ p $ -wave一时(可能的)通过使用Feshbach共振技术在冷费米气体中),已经在自旋耦合的s $波超流体状态下制备的$ p $波相互作用和$ p $波对振幅的乘积立即给出有限的$ p $ -wavesuperfluid阶参数。因此,至少在这种操纵之后,系统处于$ p $波超流体状态,其特征在于人工产生的$ p $波超流体参数。在本文中,为了评估我们的想法,我们在$ T = 0 $的情况下,评估了自旋轨道耦合的波与波超流体费米气体中的波对波振幅。我们在相位图中确定相对于$ s $波对相互作用和自旋轨道耦合强度的大$ p $波对振幅的区域。我们还从超流体相变温度的角度讨论了该最佳区域的可及性。由于获得$ p $波超流体费米气体是冷原子物理学中最关键的问题之一,因此我们的建议对这一激动人心的挑战很有用。

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    Yamaguchi, T.; Ohashi, Y.;

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