Quantum Memory with CRIB in an Asymmetric Optical Cavity

2013 ◽  
Vol 42 (6) ◽  
pp. 727-731
Author(s):  
高微 GAO Wei ◽  
王明锋 WANG Ming-feng ◽  
郑亦庄 ZHENG Yi-zhuang
2018 ◽  
Vol 190 ◽  
pp. 03007
Author(s):  
Mansur Minnegaliev ◽  
Konstantin Gerasimov ◽  
Ravil Urmancheev ◽  
Sergey Moiseev

We demonstrated a photon echo quantum memory for weak input optical pulses on the ROSE protocol in a Tm3+:Y3Al5O12 crystal placed in impedance-matched optical cavity. The quantum efficiency of 21% for a storage of time of 36 µs was achieved for single light pulses.


2022 ◽  
Vol 71 (2) ◽  
pp. 020301-020301
Author(s):  
Ma Teng-fei ◽  
◽  
Wang Min-jie ◽  
Wang Sheng-zhi ◽  
Jiao Hao-le ◽  
...  

2017 ◽  
Vol 123 (1) ◽  
pp. 83-88 ◽  
Author(s):  
N. G. Veselkova ◽  
I. V. Sokolov

2013 ◽  
Vol 52 (6) ◽  
pp. 2092-2098 ◽  
Author(s):  
Wei Gao ◽  
Xiao-Dong Tan ◽  
Ming-Feng Wang ◽  
Yi-Zhuang Zheng

2020 ◽  
Vol 18 (05) ◽  
pp. 2050027
Author(s):  
Vikas Singh Chauhan ◽  
Dixith Manchaiah ◽  
Sumit Bhushan ◽  
Rohit Kumar ◽  
Raghavan K. Easwaran

In this paper, we present a theoretical proposal to realize Quantum Memory (QM) for storage of blue light pulses (420 nm) using Electromagnetically Induced Transparency (EIT). Three-level lambda-type EIT configuration system is solved in a fully quantum mechanical approach. Storing blue light has the potential application in the field of underwater quantum communication as it experiences less attenuation inside the sea water. Our model works by exciting the relevant transitions of [Formula: see text]Rb atoms using a three-level lambda-type configuration in a Two-Dimensional Magneto-Optical Trap (2D MOT) with an optical cavity inside it. We have estimated Optical Depth inside the cavity (ODc) of [Formula: see text], group velocity ([Formula: see text]) [Formula: see text][Formula: see text]ms[Formula: see text], Delay Bandwidth Product(DBP) of 23 and maximum storage efficiency as [Formula: see text] in our system.


2015 ◽  
Vol 3 (21) ◽  
pp. 5377-5382 ◽  
Author(s):  
Kyu-Tae Lee ◽  
Masanori Fukuda ◽  
Suneel Joglekar ◽  
L. Jay Guo

Optical cavity-integrated perovskite solar cells capable of creating distinctive semitransparent colors with high efficiencies are demonstrated.


Nanophotonics ◽  
2020 ◽  
Vol 9 (5) ◽  
pp. 1081-1086 ◽  
Author(s):  
Abdoulaye Ndao ◽  
Liyi Hsu ◽  
Wei Cai ◽  
Jeongho Ha ◽  
Junhee Park ◽  
...  

AbstractOne of the key challenges in biology is to understand how individual cells process information and respond to perturbations. However, most of the existing single-cell analysis methods can only provide a glimpse of cell properties at specific time points and are unable to provide cell secretion and protein analysis at single-cell resolution. To address the limits of existing methods and to accelerate discoveries from single-cell studies, we propose and experimentally demonstrate a new sensor based on bound states in the continuum to quantify exosome secretion from a single cell. Our optical sensors demonstrate high-sensitivity refractive index detection. Because of the strong overlap between the medium supporting the mode and the analytes, such an optical cavity has a figure of merit of 677 and sensitivity of 440 nm/RIU. Such results facilitate technological progress for highly conducive optical sensors for different biomedical applications.


Crystals ◽  
2021 ◽  
Vol 11 (5) ◽  
pp. 462
Author(s):  
Ji Xia ◽  
Fuyin Wang ◽  
Chunyan Cao ◽  
Zhengliang Hu ◽  
Heng Yang ◽  
...  

Optomechanical nanocavities open a new hybrid platform such that the interaction between an optical cavity and mechanical oscillator can be achieved on a nanophotonic scale. Owing to attractive advantages such as ultrasmall mass, high optical quality, small mode volume and flexible mechanics, a pair of coupled photonic crystal nanobeam (PCN) cavities are utilized in this paper to establish an optomechanical nanosystem, thus enabling strong optomechanical coupling effects. In coupled PCN cavities, one nanobeam with a mass meff~3 pg works as an in-plane movable mechanical oscillator at a fundamental frequency of . The other nanobeam couples light to excite optical fundamental supermodes at and 1554.464 nm with a larger than 4 × 104. Because of the optomechanical backaction arising from an optical force, abundant optomechanical phenomena in the unresolved sideband are observed in the movable nanobeam. Moreover, benefiting from the in-plane movement of the flexible nanobeam, we achieved a maximum displacement of the movable nanobeam as 1468 . These characteristics indicate that this optomechanical nanocavity is capable of ultrasensitive motion measurements.


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