论文标题
基于空腔QED和相干状态的无内存量子中继器
Memoryless quantum repeaters based on cavity-QED and coherent states
论文作者
论文摘要
提议一种基于旋转对称的骨器代码(RSBC)对通道丢失(RSBC)对通道丢失的量子中继器方案(RSBC),提议在没有记忆和高时钟速率的情况下将原子纠缠状态分布在长距离上。在此方案中,受控的旋转门,即,在放置在空腔中的原子状态下的传播光模式的相移,为纠缠状态的制剂和误差综合征鉴定提供了一种机制。然后可以将分布式纠缠对纠缠对进行量子键分布(QKD)。为了评估该中继器协议的性能,定量研究了RSBC-MULTI-COMPONTER CAT代码的明确实例。数值模拟表明,如果站点之间的足够小(小于0.1km或0.01 km)和相当低的局部损失(高达0.1%),则几乎可以接近统一的量子通信的总忠诚度和量子通信的成功概率。秘密密钥速率可能会相应地高,这是每个频道使用,击败无中继器绑定,并且由于无内存方案的时钟速率相对较高。从这些结果中可以预测,如果采用更高的损失代码,则更大的基本距离也可能使忠诚度和成功概率接近统一。基于空腔的设置,可以在室温和光频率下实现此方案。
A quantum repeater scheme based on cavity-QED and quantum error correction of channel loss via rotation-symmetric bosonic codes (RSBC) is proposed to distribute atomic entangled states over long distances without memories and at high clock rates. In this scheme, controlled rotation gates, i.e., phase shifts of the propagating light modes conditioned upon the state of an atom placed in a cavity, provide a mechanism both for the entangled-state preparations and for the error syndrome identifications. The distributed entangled pairs can then be used for quantum key distribution (QKD). In order to assess the performance of this repeater protocol, an explicit instance of RSBC--multi-component cat codes are studied quantitatively. A numerical simulation shows that the total fidelity and the success probability for quantum communication over a long distance (such as 1000km) both can almost approach unity provided a small enough elementary distance between stations (smaller than 0.1km or 0.01km) and rather low local losses (up to 0.1%) are considered. Secret key rates can become correspondingly high, both per channel use, beating the repeaterless bound, and per second thanks to the relatively high clock rates of the memoryless scheme. It is predicted from these results that a larger elementary distance might also keep both the fidelity and the success probability close to unity if higher-loss codes are employed. Based upon the cavity-QED setting, this scheme can be realized at room temperature and at optical frequencies.