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Field theoretical model of multilayered Josephson junction and dynamics of Josephson vortices

机译:多层约瑟夫森结的场理论模型和约瑟夫森涡旋动力学

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Multilayered Josephson junctions are modeled in the context of a field theory, and dynamics of Josephson vortices trapped inside insulators are studied. Starting from a theory consisting of complex and real scalar fields coupled to a U(1) gauge field which admit parallel N - 1 domain-wall solutions, Josephson couplings are introduced weakly between the complex scalar fields. The N - 1 domain walls behave as insulators separating N superconductors, where one of the complex scalar fields has a gap. We construct the effective Lagrangian on the domain walls, which reduces to a coupled sine-Gordon model for well-separated walls and contains more interactions for walls at short distance. We then construct sine-Gordon solitons emerging in an effective theory in which we identify Josephson vortices carrying singly quantized magnetic fluxes. When two neighboring superconductors tend to have the same phase, the ground state does not change with the positions of domain walls (the width of superconductors). On the other hand, when two neighboring superconductors tend to have p-phase differences, the ground state has a phase transition depending on the positions of domain walls; when the two walls are close to each other (one superconductor is thin), frustration occurs because of the coupling between the two superconductors besides the thin superconductor. Focusing on the case of three superconductors separated by two insulators, we find for the former case that the interaction between two Josephson vortices on different insulators changes its nature, i.e., attractive or repulsive, depending on the positions of the domain walls. In the latter case, there emerges fractional Josephson vortices when two degenerate ground states appear due to spontaneous charge-symmetry breaking, and the number of the Josephson vortices varies with the position of the domain walls. Our predictions should be verified in multilayered Josephson junctions.
机译:在场论的背景下对多层约瑟夫森结进行了建模,并研究了被困在绝缘子内部的约瑟夫森涡旋的动力学。从包含复数和实数标量场以及允许平行N-1域壁解的U(1)规范场组成的理论开始,约瑟夫森耦合在复数标量场之间被弱引入。 N-1个畴壁充当隔离N个超导体的绝缘体,其中复杂的标量场之一具有间隙。我们在畴壁上构造有效的拉格朗日模型,对于分离良好的壁,它简化为耦合正弦-戈登模型,并且对于短距离的壁包含更多的相互作用。然后,我们构造一个有效理论中出现的正弦-戈登孤子,在其中我们识别出带有单个量化磁通量的约瑟夫森涡旋。当两个相邻的超导体倾向于具有相同的相位时,基态不会随畴壁的位置(超导体的宽度)而变化。另一方面,当两个相邻的超导体趋于具有p相差时,基态根据畴壁的位置而具有相变。当两个壁彼此靠近时(一个超导体很薄),由于除了薄超导体之外的两个超导体之间的耦合,所以会产生挫败感。着眼于三个超导体被两个绝缘体隔开的情况,对于前一种情况,我们发现两个约瑟夫森涡流在不同绝缘体上的相互作用会改变其性质,即取决于畴壁的位置,是吸引性的还是排斥性的。在后一种情况下,由于自发的电荷对称性破坏而出现两个简并的基态时,会出现分数约瑟夫森涡旋,并且约瑟夫森涡旋的数量随畴壁的位置而变化。我们的预测应该在多层约瑟夫森结中得到验证。

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