Implementing Deutsch-Jozsa Algorithm with Superconducting Quantum Interference Devices in Cavity QED

2009 ◽  
Vol 48 (8) ◽  
pp. 2384-2389 ◽  
Author(s):  
Hong-Fu Wang ◽  
Shou Zhang ◽  
Yong-Fang Zhao
2011 ◽  
Vol 25 (21) ◽  
pp. 2915-2924 ◽  
Author(s):  
ANSHOU ZHENG ◽  
YONGJIN CHENG ◽  
JIBIN LIU ◽  
XICHENG WANG ◽  
YUAN ZHENG

An alternative scheme is proposed in this paper to realize an n-qubit Fredkin gate with superconducting quantum-interference device (SQUID) in cavity QED. The multiqubit logical gate is essentially accomplished by a sequence of operations on only two SQUIDs in a large-detuned cavity. In the scheme, the two logical states of a qubit are presented by the two lowest states of a SQUID and the cavity is always in vacuum state so that the limit on the cavity is not serious.


2010 ◽  
Vol 08 (08) ◽  
pp. 1337-1345
Author(s):  
BAO-LONG FANG ◽  
ZHEN YANG ◽  
LIU YE

We present a scheme for implementing a Toffoli gate. The superconducting quantum interference devices are coupled to a resonant cavity with nonidentical SQUID–cavity coupling constants. So only one interaction between SQUID and cavity is required, and a Toffoli gate can be obtained. The method can be generalized to the N-qubit case easily and the scheme is insensitive to systematic coupling error.


2010 ◽  
Vol 39 (3) ◽  
pp. 537-542
Author(s):  
朱艳 ZHU Yan ◽  
顾永建 GU Yong-jian ◽  
徐舟 XU Zhou ◽  
谢琳 XIE Lin ◽  
马丽珍 MA Li-zhen

2011 ◽  
Vol 09 (01) ◽  
pp. 563-570
Author(s):  
ZHIMING ZHAN

We propose a method for realizing quantum logic gates and cluster states with superconducting quantum-interference devices (SQUIDs) in cavity QED via Raman transition. In this proposal, quantum logic gates and cluster states are realized by using only two lower flux states of the SQUID system and the excited state would not be excited. Therefore, the effect of decoherence caused by the levels of the SQUID system is possibly minimized.


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