2019
DOI: 10.1007/s11128-019-2254-1
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Robust and efficient transport of two-qubit entanglement via disordered spin chains

Abstract: We investigate how robust is the modified XX spin-1/2 chain of [R. G. Rigolin, Phys. Lett. A 382, 2586 (2018)] in transmitting entanglement when several types of disorder and noise are present. First, we consider how deviations about the optimal settings that lead to almost perfect transmission of a maximally entangled two-qubit state affect the entanglement reaching the other side of the chain. Those deviations are modeled by static, dynamic, and fluctuating disorder. We then study how spurious or undesired … Show more

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Cited by 13 publications
(24 citation statements)
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“…In Refs. [ 17 , 18 ] each spin of the sender (receiver) block is coupled to the edges of the 1D quantum wire allowing for the transfer of a Bell state when operating in the single-excitation subspace. A similar geometry is adopted in Refs.…”
Section: The Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…In Refs. [ 17 , 18 ] each spin of the sender (receiver) block is coupled to the edges of the 1D quantum wire allowing for the transfer of a Bell state when operating in the single-excitation subspace. A similar geometry is adopted in Refs.…”
Section: The Modelmentioning
confidence: 99%
“…While a great amount of work has been devoted to the routing of the quantum state of a single qubit [ 3 , 4 , 5 , 6 , 7 , 8 , 9 , 10 , 11 ], where the fidelity of the transfer protocol can be expressed in terms of the transition amplitude of a single excitation between a sender and a receiver location [ 12 ], the routing of a multiple qubit state is a far less investigated scenario. Although several protocols have been proposed both for two-qubit and multi-partite entangled quantum state transfer [ 13 , 14 , 15 , 16 , 17 , 18 , 19 , 20 , 21 , 22 ], their extension to a routing configuration on an arbitrary network is not straightforward. One reason being that almost all the proposed protocols rely on the quantum channel possessing mirror-symmetry, which, allowing for multiple receivers at arbitrary positions, is difficult to attain: in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…In Refs. [18,19] each spin of the sender (receiver) block is coupled to the edges of the 1D quantum wire allowing for the transfer of a Bell state when operating in the single-excitation subspace. A similar geometry is adopted in Refs.…”
Section: The Modelmentioning
confidence: 99%
“…While a great amount of work has been devoted to the routing of the quantum state of a single qubit [4][5][6][7][8][9][10][11][12], where the fidelity of the transfer protocol can be expressed in terms of the transition amplitude of a single excitation between a sender and a receiver location [13], the routing of a multiple qubit state is a far less investigated scenario. Although several protocols have been proposed both for two-qubit and multi-partite entangled quantum state transfer [14][15][16][17][18][19][20][21][22][23], their extension to a routing configuration on an arbitrary network is not straightforward. One reason being that almost all the proposed protocols rely on the quantum channel possessing mirror-symmetry, which, allowing for multiple receivers at arbitrary positions, is difficult to attain: in Ref.…”
Section: Introductionmentioning
confidence: 99%
“…A prototypical quantum channel is embodied by a quantum spin- 1 2 chain, with the sender and receiver located at its edges [13,14]. Whereas, the transfer of twoqubit entanglement has been extensively investigated via spin chain [15,16,17,18,19], multipartite entanglement transfer between the edges of a spin chain has not yet been addressed. In this paper, we build on the perturbatively perfect excitations transfer scheme [20] which has already been successfully adopted for one-and two-qubit quantum state transfer protocols [21,22,23].…”
Section: Introductionmentioning
confidence: 99%