EIT quantum memory with Cs atomic vapor for quantum communication

Author(s):  
Lijun Ma ◽  
Oliver Slattery ◽  
Paulina Kuo ◽  
Xiao Tang
Author(s):  
Olivier Pinel ◽  
Mahdi Hosseini ◽  
Ben M. Sparkes ◽  
Jesse L. Everett ◽  
Daniel Higginbottom ◽  
...  

2010 ◽  
Vol 18 (25) ◽  
pp. 25786 ◽  
Author(s):  
Young-Wook Cho ◽  
Yoon-Ho Kim
Keyword(s):  

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Yu Ma ◽  
You-Zhi Ma ◽  
Zong-Quan Zhou ◽  
Chuan-Feng Li ◽  
Guang-Can Guo

AbstractPhoton loss in optical fibers prevents long-distance distribution of quantum information on the ground. Quantum repeater is proposed to overcome this problem, but the communication distance is still limited so far because of the system complexity of the quantum repeater scheme. Alternative solutions include transportable quantum memory and quantum-memory-equipped satellites, where long-lived optical quantum memories are the key components to realize global quantum communication. However, the longest storage time of the optical memories demonstrated so far is approximately 1 minute. Here, by employing a zero-first-order-Zeeman magnetic field and dynamical decoupling to protect the spin coherence in a solid, we demonstrate coherent storage of light in an atomic frequency comb memory over 1 hour, leading to a promising future for large-scale quantum communication based on long-lived solid-state quantum memories.


2012 ◽  
Vol 12 (5&6) ◽  
pp. 490-501
Author(s):  
Jia-Jun Ma ◽  
Fen-Zhuo Guo ◽  
Qian Yang ◽  
Yan-Bing Li ◽  
Qiao-Yan Wen

In this paper, we present a quantum strong coin flipping protocol. In this protocol, an EPR pair and a quantum memory storage are made use of, and losses in the quantum communication channel and quantum memory storage are all analyzed. We obtain the bias in the fair scenario as a function of $p$, where $p$ is the probability that the particle in Bob's quantum memory storage is lost, which means our bias varies as the degree of losses in the quantum memory storage changes. Therefore we call our protocol semi-loss-tolerant. We also show that the bias decreases with decreasing $p$. When $p$ approaches $0$, the bias approaches 0.3536, which is less than that of all the previous loss-tolerant protocols. Details of both parties' optimal cheating strategies are also given and analyzed. What's more, experimental feasibility is discussed and demonstrated. Compared with previous qubit-based loss-tolerant SCF protocols, we introduce the EPR pair to keep our protocol loss-tolerant while trying to push down the bias. In addition, a quantum memory storage is used and the losses in it has been taken into account. We obtain the bias in the fair scenario as a function of $p$, where $p$ is the probability that the particle in Bob's quantum memory storage is lost, which means our bias varies as the degree of losses in the quantum memory storage changes. We also show that the bias decreases with decreasing $p$. When $p$ approaches $0$, the bias approaches 0.3536, which is less than that of all the previous loss-tolerant protocols. Details of both parties' optimal cheating strategies are also given and analyzed. Besides, experimental feasibility is discussed and demonstrated.


CLEO: 2013 ◽  
2013 ◽  
Author(s):  
Mikael Afzelius ◽  
Christoph Clausen ◽  
Imam Usmani ◽  
Pierre Jobez ◽  
Félix Bussières ◽  
...  

CLEO: 2015 ◽  
2015 ◽  
Author(s):  
Jong-Chan Lee ◽  
Kwang-Kyoon Park ◽  
Young-Wook Cho ◽  
Yoon-Ho Kim

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