2021
DOI: 10.1016/j.physleta.2020.127035
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Detecting topological edge states with the dynamics of a qubit

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Cited by 10 publications
(17 citation statements)
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“…Therefore, the occupation-measurable via the current flowing through a quantum point contact close to the dot region [43]-constitutes a simple experimental probe and an alternative to the method presented in Ref. 31, where the decoherence of a double dot has been proposed as an edge-state detector. We note that spectral and transport characteristics of quantum dots were also used in the context of Majorana bound state detection [44][45][46][47].…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Therefore, the occupation-measurable via the current flowing through a quantum point contact close to the dot region [43]-constitutes a simple experimental probe and an alternative to the method presented in Ref. 31, where the decoherence of a double dot has been proposed as an edge-state detector. We note that spectral and transport characteristics of quantum dots were also used in the context of Majorana bound state detection [44][45][46][47].…”
Section: Discussionmentioning
confidence: 99%
“…Apart from the original polymer system, the SSH model was realized experimentally and the topological edge states were detected in more controllable settings such as cold atoms [20][21][22][23], electronic states in artificial atomic lattices [24] or superlattices [25], mechanical chains [26], and photonic systems [27][28][29]. Among theoretically predicted signatures of the topological edge states are effects in the entanglement entropy [30], in the decoherence of a coupled qubit [31], and in transport and noise characteristics in non-equilibrium settings where a current is driven through an SSH chain [32][33][34][35][36]. However, to the best of our knowledge, the archetypal mesoscopic setup of a quantum dot coupled to leads has not yet been studied if the latter are modeled as SSH chains.…”
Section: Introductionmentioning
confidence: 99%
“…which clearly shows the Θ(L 2 ) scaling for large L. Moreover, the Fock basis is an optimal measurement basis, as the ground state of SSH Hamiltonian has real coefficients in that basis [59]. Such a measurement can be performed by measuring the number operator ĉ † j,m ĉ j,m for each fermionic mode.…”
mentioning
confidence: 99%
“…For λ<λ c = 1, the normalized edge state solution is given by [59] |ψ SSH edge = |φ z=−λ |u , where |φ z is given by Eq. ( 2) and |u = [1 0] T .…”
mentioning
confidence: 99%
“…. , M. In contrast, the topological edge eigenstates read[75,76] j+1 sinh[κa(M + 1 − j)] ± sinh[κaj] , ( A . 5 ) where κ fulfills v sinh[κ(M + 1)a] = w sinh[κMa] and N 0 = (w sinh(2κaM)/2v sinh(κa)) − (M + 1) is a normalization constant.…”
mentioning
confidence: 99%