2017
DOI: 10.1016/j.jmmm.2016.12.093
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Majorana zero modes in the coexistence phase of chiral superconductivity and 120°-type magnetic order on the triangular lattice

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Cited by 12 publications
(8 citation statements)
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“…It is sufficient that all of the zero modes shown in Figure 1 are the edge ones. This is an important difference from the case ∆ 21 = 0 considered in [17] where the continual region with the bulk gapless excitations is appeared in the space of the parameters h and µ. As the result the zero energy modes of the system with the cylinder topology which are found in this region are not the edge ones and represent the bulk excitations modified due to the boundary effects.…”
Section: Hamiltonian Symmetry and Z 2 Topological Invariantmentioning
confidence: 73%
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“…It is sufficient that all of the zero modes shown in Figure 1 are the edge ones. This is an important difference from the case ∆ 21 = 0 considered in [17] where the continual region with the bulk gapless excitations is appeared in the space of the parameters h and µ. As the result the zero energy modes of the system with the cylinder topology which are found in this region are not the edge ones and represent the bulk excitations modified due to the boundary effects.…”
Section: Hamiltonian Symmetry and Z 2 Topological Invariantmentioning
confidence: 73%
“…I f m is the parameter of the exchange interaction, being considered within the two coordination spheres. An important difference of the system (1) from the model studied in [17] is the consideration of superconducting pairings between nearest neighbors. Hereinafter, the model is considered both in the case of periodic boundary conditions along the direction a 2 (the cylinder topology), and in the case of periodic boundary conditions in two spatial directions (the torus topology).…”
Section: Model and Methodsmentioning
confidence: 99%
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“…Впоследствии для такой фазы в рамках квадратичного гамильтониана были най-дены условия реализации майорановских мод [8].…”
Section: Introductionunclassified