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Journal of Yanbian University

Probabilistic teleportation of an arbitrary three-particle state via an arbitrary five-particle state and an EPR pair

Ying Wang

Published Jan 1, 2005• 0 citations
OpenAlex

Abstract

A scheme of teleportation of an arbitrary three-particle state is presented when a non-maximal arbitrary five-particle state and an EPR pair are used as quantum channels. We show that teleportation can be successfully (realized) with a certain probability by performing three Bell-state measurements on the sender's side and by (introducing) an auxiliary particle and performing a unitary transformation the Hadamard operation and measurement result, conditioning on the other possible receiver's side.

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理论物理通讯:英文版•Jan 1, 2004•0 citations
A scheme of teleportation of an arbitrary three-particle state is presented when a non-maximal arbitrary five-particle state and an EPR pair are used as quantum channels. We show that teleportation can be successfully (realized) with a certain probability by performing three Bell-state measurements on the sender's side and by (introducing) an auxiliary particle and performing a unitary transformation the Hadamard operation and measurement result, conditioning on the other possible receiver's side.
We present a scheme to probabilistically teleport an arbitrary and unknown two-particle state via a nonmaximally entangled EPR pair and a non-maximally entangled GHZ state as the quantum channel. With the help of Bell-state measurements and Hadamard measurement, an arbitrary two-particle state can be perfectly teleported if a receiver introduces a collective unitary transformation. The unitary transformation is given uniquely. Also, we present a quantum circuit for realizing the teleportation successfully.
A scheme for teleporting an arbitrary and unknown three-particle state from a sender to either one of two receivers is proposed. The quantum channel is composed of a two-particle non-maximally entangled state and two three-particle non-maximally entangled W states. An arbitrary three-particle state can be perfectly teleported probabilistically if the sender performs three generalized Bell-state measurements and sends to the two receivers the classical result of these measurements and either one of the two receivers adopts an appropriate unitary transformation conditioned on the suitable measurement outcomes of the other receiver. All kinds of unitary transformations are given in detail.
A scheme for teleporting an arbitrary three-particle W state from a sender to either of the two receivers is proposed,where the three three-particle W states quantum channel are taken as quantum channels.There are two ways to realize the intention of teleportation.It is proved that,for such maximally entangled quantum channels,there is still a certain probability of successful teleportation if the sender performs three generalized Bell-state measurements while either of the two receivers performs an appropriate unitary transformation with the help of the other suitable measurements in the basis of {|0,|1} and classical information;on the other hand,the probability of successful teleportation is not affected by the order of operations.The present scheme may be directly generalized to teleport an unknown N-particle W state from a sender to either of the two receivers by using N W states as quantum channels,as well as performing N Bell measurements.
We present a scheme to teleport an unknown three-particle entangled state from a sender to either one of two receivers. The partial three-particle entangled state and the three-particle entangled W state are considered as the quantum channels. An unknown three-particle entangled state can be perfectly teleported probabilistically by performing two generalized Bell measurements and the Hadamard operation at the sender's side and introducing an appropriate unitary transformation in each receiver's laboratory conditioned on the simple measurement outcome of the other. All kinds of unitary transformations are given in details. This scheme can be directly generalized to teleport an unknown three-particle entangled state from a sender to any one of N receivers by the partial three-particle entangled state and the ( N + 1)-particle entangled W state.