-
量子技术, 比如量子通信、量子计算, 具有经典技术所不具有的优势. 但是, 作为量子技术基本元素的量子态往往极为脆弱, 很容易受到外界环境的影响而丢失, 而且量子态的制造和量子操作往往是概率性的. 这种概率性使得远距离量子通信和大规模的量子计算很难实现, 除非有量子存储器将这些随机产生的量子态缓存并同步起来. 在过去的十几年中, 量子存储在各种各样的存储方案中得到了研究, 而且已经从最初的原理性演示逐步发展到了如今的近乎可实用化. 现如今, 量子存储领域追求的是可实用化, 而判断一个存储器是否可以实用化的基本标准是: 高存储效率、低噪音、长寿命(或者大的时间带宽积)和室温条件下运行. 通过介绍多个具有代表性的存储方案, 本文给出了量子存储领域的研究现状和发展趋势. 其中基于室温原子系综的宽带量子存储因其装置简单、实用性更强而广受关注. 但是由于噪音问题, 直到最近才在实验室中实现可工作在室温环境中的宽带FORD (far off-resonance Duan-Lukin-Cirac-Zoller)量子存储和梯形量子存储. 本文对多种存储方案的工作原理、优缺点进行了介绍, 对FORD方案之所以能够成功进行了分析, 还对量子存储的降噪方法进行了总结.
-
关键词:
- 量子存储/
- 量子信息/
- 远失谐Duan-Lukin-Cirac-Zoller方案/
- 室温原子
Quantum technologies, for example, quantum communication and quantum computation, promise spectacular quantum enhanced advantages beyond what can be done classically. However, quantum states, as the element of quantum technologies, are very fragile and easily get lost to the environment, and meanwhile, their generation and quantum operations are mostly probabilistic. These problems make it exponentially hard to build long-distance quantum channels for quantum communication and large quantum systems for quantum computing. Quantum memory allows quantum states to be stored and retrieved in a programmable fashion, therefore providing an elegant solution to the probabilistic nature and associated limitation by coordinating asynchronous events. In the past decades, enormous advances in quantum memory have been made by developing various storage protocols and their physical implementations, and the quantum memory has gradually evolved from the initial conceptual demonstration to a nearly practical one. Aiming at being practicable for efficient synchronisation and physical scalability, an ideal quantum memory should meet several key features known as high efficiency, low noise level, large time bandwidth product (lifetime divided by pulse duration) and operating at room temperature. Here, we present the research status and development trends of this field by introducing some typical storage protocols. Among these protocols, a room-temperature broadband quantum memory is the most attractive due to its simplicity and practicability. However, at room temperature, noise becomes dominant and is a bottleneck problem that has impeded the realization of a real room-temperature broadband quantum memory in the last decades. Recently, the noise problem has been solved in two memory protocols, i.e. FORD (far off-resonance Duan-Lukin-Cirac-Zoller) protocol and ORCA (off-resonant cascaded absorption) protocol. In this paper, the working principles, the merits and demerits of various quantum memory protocols are illustrated. Furthermore, the approaches to eliminating noise and the applications of quantum memory are summarized.-
Keywords:
- quantum memory/
- quantum information/
- far off-resonance Duan-Lukin-Cirac-Zoller protocol/
- room-temperature atoms
[1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] [17] [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] [29] [30] [31] [32] [33] [34] [35] [36] [37] [38] [39] [40] [41] [42] [43] [44] [45] [46] [47] [48] [49] [50] [51] [52] [53] [54] [55] [56] [57] [58] [59] [60] [61] [62] [63] [64] [65] [66] [67] [68] [69] [70] [71] [72] [73] [74] [75] [76] [77] [78] [79] [80] [81] [82] [83] [84] -
具有代表性的工作 存储方案 存储器温度 互关联函数g(2) 带宽 时间带宽积 1 Phys. Rev. Lett.110083601 (2013) EIT 300 μK ≤2 <5 MHz 74 2 Nature438837 (2005) EIT 303—320 K 2—3 ~1 MHz ~1 3 Nature438833 (2005) EIT ~100 μK 8.5 12 MHz 120 4 Nat. Photon.5628 (2011) EIT ~100 μK 10 5.5 MHz 13 5 Phys. Rev. A75040101 (2007) DLCZ 333 K 1.3 1 MHz NA 6 Nat. Phys.595 (2009) DLCZ 100 μK 37 <10 MHz <10000 7 Opt. Lett.37142 (2012) DLCZ 310 K 4 1 MHz 5 8 Nat. Photon.10381 (2016) DLCZ ~100 μK ~37 <10 MHz <2200000 9 Nature461241 (2009) GEM 300K ≤2 1 MHz NA 10 Nat. Commun.174 (2011) GEM 351 K ≤2 ~1 MHz ≤10 11 Optica3100 (2016) GEM 100 μK ≤2 <10 MHz 84 12 Nat. Photon.4218 (2010) Far off-resonance Raman 335.5 K ≤2 1.5 GHz 18 13 Phys. Rev. Lett.107053603 (2011) Far off-resonance Raman 335.5 K ≤2 1.5 GHz 2250 14 Phys. Rev. Lett.116090501 (2016) Far off-resonance Raman 343 K ≤2 1 GHz 95 15 Nat. Photon.9332 (2015) Raman memory ~100 μK 13.6 140 MHz 200 16 Nature432482 (2004) Off-resonant Faraday interaction 300 K ≤2 NA NA 17 Phys. Rev. A97042316 (2018) Off-resonant cascaded absorption (ORCA) 364 K 120 1 GHz 5 18 Commun. Phys.155 (2018) Far off-resonance DLCZ (FORD) 334 K 28 537 MHz 700 
下载:
导出CSV
-
[1] [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] [17] [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] [29] [30] [31] [32] [33] [34] [35] [36] [37] [38] [39] [40] [41] [42] [43] [44] [45] [46] [47] [48] [49] [50] [51] [52] [53] [54] [55] [56] [57] [58] [59] [60] [61] [62] [63] [64] [65] [66] [67] [68] [69] [70] [71] [72] [73] [74] [75] [76] [77] [78] [79] [80] [81] [82] [83] [84]
下载:
计量
- 文章访问数:23119
- PDF下载量:883
- 被引次数:0