scholarly journals Single-step implementation of a multiple-target-qubit controlled phase gate without need of classical pulses

2014 ◽  
Vol 39 (11) ◽  
pp. 3312 ◽  
Author(s):  
Chui-Ping Yang ◽  
Qi-Ping Su ◽  
Feng-Yang Zhang ◽  
Shi-Biao Zheng
2021 ◽  
Vol 11 (1) ◽  
Author(s):  
S. U. Shringarpure ◽  
J. D. Franson

AbstractKnill, Laflamme, and Milburn showed that linear optics techniques could be used to implement a nonlinear sign gate. They also showed that two of their nonlinear sign gates could be combined to implement a controlled-phase gate, which has a number of practical applications. Here we describe an alternative implementation of a controlled-phase gate for a single-rail target qubit that only requires the use of a single nonlinear sign gate. This gives a much higher average probability of success when the required ancilla photons are generated using heralding techniques. This implementation of a controlled-phase gate destroys the control qubit, which is acceptable in a number of applications where the control qubit would have been destroyed in any event, such as in a postselection process.


2018 ◽  
Vol 14 (2) ◽  
Author(s):  
You-Ji Fan ◽  
Zhen-Fei Zheng ◽  
Yu Zhang ◽  
Dao-Ming Lu ◽  
Chui-Ping Yang

2018 ◽  
Vol 17 (9) ◽  
Author(s):  
Tong Liu ◽  
Bao-Qing Guo ◽  
Yang Zhang ◽  
Chang-Shui Yu ◽  
Wei-Ning Zhang

2010 ◽  
Vol 10 (9&10) ◽  
pp. 821-828
Author(s):  
Yan Xia ◽  
Jie Song ◽  
Zhen-Biao Yang ◽  
Shi-Biao Zheng

We propose a protocol to controlled implement the two-photon controlled phase gate within a network by using interference of polarized photons. The realization of this protocol is appealing due to the fact that the quantum state of light is robust against the decoherence, and photons are ideal carriers for transmitting quantum information over long distances. The proposed setup involves simple linear optical elements and the conventional photon detectors that only distinguish the vacuum and nonvacuum Fock number states. This can greatly simplify the experimental realization of a linear optical quantum computer.


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