Abstract

Two-mode entangled state is an important quantum resource for quantum information. In this paper, the amplification of a single mode of two-mode entangled state (single-mode amplification scheme) and two modes of two-mode entangled state (two-mode amplification scheme) are theoretically proposed. Here, the optical beam splitter model is used to simulate the vacuum noise introduced by the loss in the optical transmission process. By utilizing the positivity under partial transpose criterion, we analyze the effect of the gain of the four-wave mixing process on the entanglement degree of the initial two-mode entangled state in two different amplification schemes. In these two schemes, we set the gain of the initial two-mode entangled state generation process to be 1.5, 2.5 and 50.0 respectively, and then change the gain of the amplification process in a certain range. We also set the transmission efficiency of the amplified beams for each of the two schemes to be a definite value. The results show that the entanglement of the initial two-mode entangled state decreases with the gain increasing under the condition of specific transmission loss in two schemes. When the gain does not exceed a certain value, the entanglement of the initial two-mode entangled state can be maintained. Then, with the increase of the gain, the entanglement of the initial two-mode entangled state will disappear. Moreover, the entanglement of the initial two-mode entangled state of the two-mode amplification scheme disappears faster than that of the single-mode amplification scheme. Our theoretical results pave the way for the experimental realization of the amplification of two-mode entangled state based on four-wave mixing process.

Highlights

  • The results show that the entanglement of the initial two-mode entangled state decreases with the gain increasing under the condition of specific transmission loss in two schemes

  • 结果表明在特定的真空场噪声影 响下, 当放大 Einstein-Podolsky-Rosen s (EPR) 光束的强度增益处于一定范围 内时, 单模放大方案和双模放大方案中初始双模纠 缠态的纠缠特性可以保持, 并且增益越大, 纠缠越 弱直至纠缠消失

Read more

Summary

Introduction

* 国家自然科学基金 (批准号: 11874155, 91436211, 11374140)、国家重点基础研究发展计划 (批准号: 2016YFA0302103)、上海市 年, 美国 Lett 研究组 [24] 利用四波混频过程实现了 EPR 纠缠光束延迟, 证明了铷原子池可以作为信 息存储器对信息进行短时间存储. 其中 G1 是第一个四波混频过程 (FWM1) 的增益, a0 和b0 是真空注入, a1 和b1 是第一个四波混频过程 产生的探针光束和共轭光束, v1 和 v2 表示真空场 的湮灭算符, η1 和 η2 分别表示 a1 和b1的传输效率. (FWM2) 的种子光, 与泵浦光束 Pump2 注入到第二 个热 85Rb 蒸气池中, 产生放大后的探针光束 a2.

Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call