2016
DOI: 10.1134/s0021364016190127
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Coexistence of the chiral superconductivity and noncollinear magnetic order in the ensemble of Hubbard fermions on a triangular lattice

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Cited by 14 publications
(6 citation statements)
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“…2a Additionally, a comparison of the ε 1,2 (µ) and n (µ) dependences implies that the topological transitions are characterized by the peculiarities of the ∂ n /∂µ behavior. Similar features were observed in the Kitaev chain model [54] and in the model of an electron ensemble on a triangular lattice in the phase of coexistence of superconductivity and magnetism [55]. We also note that the analysis of the ∂ n /∂µ singularities at V = 0 allows one to reconstruct the topological phase diagram of the system obtained in [41].…”
Section: Resultssupporting
confidence: 78%
“…2a Additionally, a comparison of the ε 1,2 (µ) and n (µ) dependences implies that the topological transitions are characterized by the peculiarities of the ∂ n /∂µ behavior. Similar features were observed in the Kitaev chain model [54] and in the model of an electron ensemble on a triangular lattice in the phase of coexistence of superconductivity and magnetism [55]. We also note that the analysis of the ∂ n /∂µ singularities at V = 0 allows one to reconstruct the topological phase diagram of the system obtained in [41].…”
Section: Resultssupporting
confidence: 78%
“…From Eq. (16) we conclude that the Majorana modes exist in the phases with odd N 3 . The transition to such phases is accompanied by the closing the gap in the bulk spectrum in an odd number of points in the Brillouin zone.…”
Section: The Topological Invariant N 3 Of a 2d Lattice And Its Connecsupporting
confidence: 52%
“…This assumption allows us to study the topological phases of the system in the relatively simple manner. However, it should be noted that the coexistence phase is caused not only by the proximity effect but also as a consequence of the internal electron interactions [16].…”
Section: Model and Methodsmentioning
confidence: 99%
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“…It can be seen from expression (18) for the triplet pairing terms that in the case of the ferromagnetic ordering with Q = 0 the effective triplet superconductivity induced from the spin-singlet channel, which is described by the second term in (18), is not realized since t − k = 0. Moreover, it is known that superconductivity is strongly destroyed by ferromagnetism while for antiferromagnetic and spiral structures it is only suppressed (see [108,[110][111][112][113][114][115][116][117][118][119][120][121][122][123][124][125][126] and references therein).…”
Section: D Casementioning
confidence: 99%