Remote Preparation of General One-, Two- and Three-Qubit States via χ-Type Entangled States

2020 ◽  
Vol 59 (12) ◽  
pp. 3789-3803
Author(s):  
Jia-Yin Peng
2019 ◽  
Vol 18 (4) ◽  
Author(s):  
Yang Xue ◽  
Lei Shi ◽  
Xinyu Da ◽  
Kaihang Zhou ◽  
Lihua Ma ◽  
...  

2019 ◽  
Vol 18 (8) ◽  
Author(s):  
Jiahua Wei ◽  
Lei Shi ◽  
Shanghong Zhao ◽  
Kaihang Zhou ◽  
Longqiang Yu ◽  
...  

2017 ◽  
Vol 16 (10) ◽  
Author(s):  
Jiahua Wei ◽  
Lei Shi ◽  
Lihua Ma ◽  
Yang Xue ◽  
Xuchun Zhuang ◽  
...  

2017 ◽  
Vol 15 (07) ◽  
pp. 1750049 ◽  
Author(s):  
Y. Akbari-Kourbolagh

We present sufficient criteria for the entanglement of three-qubit states. For some special families of states, the criteria are also necessary for the entanglement. They are formulated as simple sets of inequalities for the mean values of certain observables defined as tensor products of Pauli matrices. The criteria are good indicators of the entanglement in the vicinity of three-qubit GHZ and W states and enjoy the capability of detecting the entangled states with positive partial transpositions. Furthermore, they improve the best known result for the case of W state mixed with the white noise. The efficiency of the criteria is illustrated through several examples.


2013 ◽  
Vol 27 (22) ◽  
pp. 1350160 ◽  
Author(s):  
JIA-YIN PENG ◽  
MING-XING LUO ◽  
ZHI-WEN MO ◽  
ZHI-GUO QU

The protocols for jointly preparing three-particle state from a spatially separated multi-sender to one receiver are presented in this paper. The first scheme with two senders is proposed and shown to be a flexible deterministically. And then it is generalized to the multi-sender with improved success probability, by only adding some classical communications.


2011 ◽  
Vol 09 (07n08) ◽  
pp. 1635-1642 ◽  
Author(s):  
A. GÜN ◽  
A. GENÇTEN

In quantum information processing, spin-3/2 electron or nuclear spin states are known as two-qubit states. For SI (S = 3/2, I = 1/2) spin system, there are eight three-qubit states. In this study, first, three-qubit CNOT logic gates are obtained. Then three-qubit entangled states are obtained by using the matrix representation of Hadamard and three-qubit CNOT logic gates. By considering single 31P@C60 molecule as SI (S = 3/2, I = 1/2) spin system, three-qubit entangled states are also obtained using the magnetic resonance pulse sequences of Hadamard and CNOT logic gates.


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