2016
DOI: 10.1103/physrevb.93.205137
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Topological quasi-one-dimensional state of interacting spinless electrons

Abstract: By decreasing the transversal confinement potential in interacting one-dimensional spinless electrons and populating the second energetically lowest sub-band, for not too strong interactions system transitions into a quasi-one-dimensional state with dominant superconducting correlations and one gapless mode. By combining effective field theory approach and numerical density matrix renormalization group simulations we show that this quasi-one-dimensional state is a topological state that hosts zero-energy edge … Show more

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Cited by 11 publications
(5 citation statements)
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References 42 publications
(66 reference statements)
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“…Examples include structural transitions of dipolar particles in an elongated trap [1] and in ion traps [2][3][4][5], one-dimensional Fermi gas with attractive interactions [6], coupled bosonic chains [7,8], insulator-metal transition induced by a tilted magnetic field in graphene [9], and spin polarized electrons in a one-dimensional quantum wire near a conductance plateau transition [10][11][12][13]. This transition also occurs in certain lattice models of fermions [14].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Examples include structural transitions of dipolar particles in an elongated trap [1] and in ion traps [2][3][4][5], one-dimensional Fermi gas with attractive interactions [6], coupled bosonic chains [7,8], insulator-metal transition induced by a tilted magnetic field in graphene [9], and spin polarized electrons in a one-dimensional quantum wire near a conductance plateau transition [10][11][12][13]. This transition also occurs in certain lattice models of fermions [14].…”
Section: Introductionmentioning
confidence: 99%
“…(A4) and exapnding b = 1 + d for infinitesimal d , we obtain the values for z and η B given in Eqs. ( 12)- (13).…”
mentioning
confidence: 99%
“…It is believed that the fidelity F (h, h + δh) can characterize the quantum phase transition [55][56][57][58][59][60][61][62] due to the qualitative differences of the ground state |ψ(h) at the phase transition point h = h c . Alternatively, a more convenient quantity -fidelity susceptibility χ F (h) that appears as the leading quadratic term in the expansion of ground-state fidelity F (h, h + δh) is defined as…”
mentioning
confidence: 99%
“…In the wellbore cleaning problem of extended-reach drillings with high-inclination sections, D hyd , D hyd and D hyd are chosen as the basic physical quantities, and all other quantities can be obtained by these three basic quantities; the three basic measures chosen are the mass basic measure [M], the time basic measure [T], and the distance basic measure [L] (Sun, 2013) [16]. We can know that n = 13 and m = 3 according to the Π theorem, so there exist n − m = 10 dimensionless physical quantities.…”
Section: Symbols Of Variablesmentioning
confidence: 99%