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Transition to Fulde-Ferrel-Larkin-Ovchinnikov phases near the tricritical point: an analytical study

机译:在三临界点附近转变为Fulde-Ferrel-Larkin-Ovchinnikov相的分析研究

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We explore analytically the nature of the transition to the Fulde-Ferrel-Larkin-Ovchinnikov superfluid phases in the vicinity of the tricritical point, where these phases begin to appear. We make use of an expansion of the free energy up to an overall sixth order, both in order parameter amplitude and in wavevector. We first explore the minimization of this free energy within a subspace, made of arbitrary superpositions of plane waves with wavevectors of different orientations but same modulus. We show that the standard second order FFLO phase transition is unstable and that a first order transition occurs at higher temperature. Within this subspace we prove that it is favorable to have a real order parameter and that, among these states, those with the smallest number of plane waves are preferred. This leads to an order parameter with an cos(q_0·r) dependence, in agreement with preceding work. Finally we show that the order parameter at the transition is only very slightly modified by higher harmonics contributions when the constraint of working within the above subspace is released.
机译:我们分析地探讨了在三临界点附近向Fulde-Ferrel-Larkin-Ovchinnikov超流体相过渡的性质,这些相开始出现。在阶跃参数振幅和波矢量中,我们利用自由能扩展到整个第六阶。我们首先探索子空间内这种自由能的最小化,该子空间由平面波的任意叠加与不同方向但模量相同的波矢组成。我们表明标准的二阶FFLO相变是不稳定的,并且一阶跃迁发生在较高的温度下。在该子空间内,我们证明了具有实阶参数是有利的,并且在这些状态中,首选平面波数量最少的状态。与先前的工作一致,这导致具有cos(q_0·r)依赖性的阶数参数。最后,我们表明,当释放在上述子空间内的工作约束时,过渡参数仅会被高次谐波贡献非常轻微地修改。

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