2016
DOI: 10.1088/1674-1056/25/8/080307
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Transferring information through a mixed-five-spin chain channel

Abstract: We initially introduce one-dimensional mixed-five-spin chain with Ising-XY model which includes mixture of spins-1/2 and spins-1. Here, it is considered that nearest spins (1, 1/2) have Ising-type interaction and nearest spins (1/2, 1/2) have both XY -type and Dzyaloshinskii-Moriya (DM) interactions together. Nearest spins (1, 1) have XX Heisenberg interaction. This system is in the vicinity of an external homogeneous magnetic field B in thermal equilibrium state. We promote the quantum information transmittin… Show more

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Cited by 2 publications
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“…) that describe the noise channels A and B, with ๐‘ = 1โˆ’exp(โˆ’๐œ…๐‘ก), where ๐œ… is the phase damping rate, and 0 โ‰ค ๐‘ โ‰ค 1. The evolved state of such a bipartite (sub)system under phase flip channel is described as a completely positive trace preserving map โ„ณ[๐œŒ(A B)] = โˆ‘๏ธ€ ๐‘–,๐‘— [47] we proved that a mixed-spin chain with the two adjacent mixed-three-spin (1/2, 1, 1/2) cells can be an ideal memory-less channel for transferring quantum information). Figure 1 depicts the concurrence and GGQD behaviors versus the magnetic field under the phase flip channel.…”
mentioning
confidence: 94%
“…) that describe the noise channels A and B, with ๐‘ = 1โˆ’exp(โˆ’๐œ…๐‘ก), where ๐œ… is the phase damping rate, and 0 โ‰ค ๐‘ โ‰ค 1. The evolved state of such a bipartite (sub)system under phase flip channel is described as a completely positive trace preserving map โ„ณ[๐œŒ(A B)] = โˆ‘๏ธ€ ๐‘–,๐‘— [47] we proved that a mixed-spin chain with the two adjacent mixed-three-spin (1/2, 1, 1/2) cells can be an ideal memory-less channel for transferring quantum information). Figure 1 depicts the concurrence and GGQD behaviors versus the magnetic field under the phase flip channel.…”
mentioning
confidence: 94%