2021
DOI: 10.48550/arxiv.2101.01472
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Entanglement transfer via Chiral Quantum Walk on a Triangular Chain

Abstract: We investigate the chiral quantum walk (CQW) for entanglement transfer on a triangular chain. We specifically consider two and three site Bell and W type entanglement cases, respectively. Using concurrence as quantum entanglement measure, together with the Bures distance and trace distance as the measures of the fidelity of the state transfer, we evaluate the success of the entanglement transfer. We compare the entangled state transfer time and quality in CQW against continuous-time quantum random walk. Furthe… Show more

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Cited by 1 publication
(4 citation statements)
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“…The Y-junction graph, in which the phases on the edge-weights can not be gauged away as in Section 2 due to the loop nature, can bring novel phenomena in quantum walks such as directed currents [38], non-reciprocal transmission [35], and quantum transport enhancement [39]. It was paid close attention recently both in theories [16,21,27,39] and experiments [36,[40][41][42][43]. The Y-junction graph can be realized in experiments by high-dimensional photonic quantum states, multiple concatenated interferometers, or dimension-dependent losses [37].…”
Section: Controlled Transport On Y-junction Graphmentioning
confidence: 99%
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“…The Y-junction graph, in which the phases on the edge-weights can not be gauged away as in Section 2 due to the loop nature, can bring novel phenomena in quantum walks such as directed currents [38], non-reciprocal transmission [35], and quantum transport enhancement [39]. It was paid close attention recently both in theories [16,21,27,39] and experiments [36,[40][41][42][43]. The Y-junction graph can be realized in experiments by high-dimensional photonic quantum states, multiple concatenated interferometers, or dimension-dependent losses [37].…”
Section: Controlled Transport On Y-junction Graphmentioning
confidence: 99%
“…the fact Ξ(θ) = N 2 + O(1) has been used above and phase β is defined by β ≡ f (k 0 , 0) − f (k 0 , ω). The above equation indicates that main contributions of the summations in (27) come from terms around q, p = N k 0 π , since they decay to zero very fast when the integer q or p moves away. In the same spirit, we learn that around q, p = N k 0 π , one has Moreover, by Taylor expansion of the spectra around q, p → N k 0 π , we obtain e it(Ep−ǫq) ≈ e it•2 sin k 0…”
Section: Scattering Theory On Latticementioning
confidence: 99%
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