Physics – Condensed Matter – Strongly Correlated Electrons
Scientific paper
2011-10-13
Phys. Rev. B 85, 035110 (2012)
Physics
Condensed Matter
Strongly Correlated Electrons
11 pages, 8 figures; brief clarifying comments added; few new references; this version is accepted in Phys. Rev. B
Scientific paper
10.1103/PhysRevB.85.035110
A one-dimensional Ising model in a transverse field can be mapped onto a system of spinless fermions with p-wave superconductivity. In the weak-coupling BCS regime, it exhibits a zero energy Majorana mode at each end of the chain. Here, we consider a variation of the model, which represents a superconductor with longer ranged kinetic energy and pairing amplitudes, as is likely to occur in more realistic systems. It possesses a richer zero temperature phase diagram and has several quantum phase transitions. From an exact solution of the model these phases can be classified according to the number of Majorana zero modes of an open chain: 0, 1, or 2 at each end. The model posseses a multicritical point where phases with 0, 1, and 2 Majorana end modes meet. The number of Majorana modes at each end of the chain is identical to the topological winding number of the Anderson's pseudospin vector that describes the BCS Hamiltonian. The topological classification of the phases requires a unitary time-reversal symmetry to be present. When this symmetry is broken, only the number of Majorana end modes modulo 2 can be used to distinguish two phases. In one of the regimes, the wave functions of the two phase shifted Majorana zero modes decays exponentially in space but but in an oscillatory manner. The wavelength of oscillation is identical to the asymptotic connected spin-spin correlation of the XY-model in a transverse field to which our model is dual.
Chakravarty Sudip
Chung Suk Bum
Hsu Chen-Hsuan
Mandal Ipsita
Niu Yuezhen
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