Chinese Optics Letters, Volume. 21, Issue 8, 082701(2023)

Surpassing the standard quantum limit of optical imaging via deep learning

Miao Cai1, Zhi-Xiang Li1, Hao-Dong Wu1, Ya-Ping Ruan1, Lei Tang1, Jiang-Shan Tang1, Ming-Yuan Chen1, Han Zhang1,2, Ke-Yu Xia1,4,5、*, Min Xiao1,2,3, and Yan-Qing Lu1
Author Affiliations
  • 1College of Engineering and Applied Sciences, National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210023, China
  • 2School of Physics, Nanjing University, Nanjing 210023, China
  • 3Department of Physics, University of Arkansas, Fayetteville, Arkansas 72701, USA
  • 4Hefei National Laboratory, Hefei 230088, China
  • 5Jiangsu Key Laboratory of Artificial Functional Materials, Nanjing University, Nanjing 210023, China
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    Figures & Tables(4)
    (a) Schematic of the noise2noise protocol. Both the inputs and targets during training are noisy data, and the loss function is L2 loss. With this protocol, the well-trained DL neural network can denoise the input noisy signal. (b) Diagram model for U-net. The structure includes two parts: the contracting part (left yellow area) and the expansive part (right pink area). Each slab represents a layer in the neural network. Colors indicate different types of layers, as shown by legends. (c) Schematic of data set preparation process. First, we randomly choose m frames from the original image data set {D(o)}. These frames generate a new image through accumulation and min-max normalization. This procedure is repeated N(r) times to obtain the regrouped image data set, including N(r) frames. Then, the new data set is used for training.
    Single-photon coincidence imaging of an Airy pattern. (a) Experimental setup. QWP, quarter-wave plate; HWP, half-wave plate; PBS, polarizing beam splitter; M, mirror; SPCM, single-photon counting module; PM, phase modulation; SLM, spatial light modulator; DM, dichroic mirror; DPBS, dual-wavelength PBS; DHWP, dual-wavelength HWP. An SLM is used as a scattering object to generate the Airy pattern. (b) Images accumulated over 1, 50, 500, and 5000 frames, respectively. The exposure time are Δte = 0.2 s. (c) Positions of the pixels (red points) that are chosen to calculate the variance in (d); (d) variance of the photon-number distribution versus the mean photon number n¯photon. A linear function (red line), σ2=59.19n¯photon−19.15, fits the variance well.
    Original and DL-enhanced Airy patterns for exposure time (a) Δte = 0.1 s and (b) 0.5 s, respectively; left column, top view of the original and DL-enhanced Airy patterns; middle column, projecting the Airy pattern to the y direction (side view); right column, brightness profiles along the red lines in the Airy pattern in left column. Red arrows are guides to the eye for the peaks appearing in the DL-enhanced images but indistinguishable in the original ones. Red curves in (b) represent the envelope of a theoretical Airy pattern.
    SNRs for the direct accumulation and the DL-based scheme. (a) Original image showing the areas for calculating SNR. The red dot indicates the center of the main peak of the Airy pattern. The red box surrounds a pure noise area. (b) SNR(1) versus the exposure time Δte; (c) SNR(2) versus the regroup size m.
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    Miao Cai, Zhi-Xiang Li, Hao-Dong Wu, Ya-Ping Ruan, Lei Tang, Jiang-Shan Tang, Ming-Yuan Chen, Han Zhang, Ke-Yu Xia, Min Xiao, Yan-Qing Lu, "Surpassing the standard quantum limit of optical imaging via deep learning," Chin. Opt. Lett. 21, 082701 (2023)

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    Paper Information

    Category: Quantum Optics and Quantum Information

    Received: Mar. 6, 2023

    Accepted: Apr. 23, 2023

    Posted: Apr. 24, 2023

    Published Online: Aug. 11, 2023

    The Author Email: Ke-Yu Xia (keyu.xia@nju.edu.cn)

    DOI:10.3788/COL202321.082701

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