4.8 Article

Extract the Degradation Information in Squeezed States with Machine Learning

期刊

PHYSICAL REVIEW LETTERS
卷 128, 期 7, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.128.073604

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资金

  1. Ministry of Science and Technology of Taiwan [108-2923-M-007-001-MY3, 109-2112-M-007-019-MY3, 110-2123-M-007-002]
  2. Office of Naval Research Global
  3. Institute for Cosmic Ray Research (ICRR)
  4. University of Tokyo

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This study demonstrates fast, robust quantum state tomography using machine learning, achieving high fidelity reconstruction with a neural network. It also reveals degradation information in low and high noisy scenarios, showcasing the potential of machine learning in quantum state analysis.
In order to leverage the full power of quantum noise squeezing with unavoidable decoherence, a complete understanding of the degradation in the purity of squeezed light is demanded. By implementing machine-learning architecture with a convolutional neural network, we illustrate a fast, robust, and precise quantum state tomography for continuous variables, through the experimentally measured data generated from the balanced homodyne detectors. Compared with the maximum likelihood estimation method, which suffers from time-consuming and overfitting problems, a well-trained machine fed with squeezed vacuum and squeezed thermal states can complete the task of reconstruction of the density matrix in less than one second. Moreover, the resulting fidelity remains as high as 0.99 even when the antisqueezing level is higher than 20 dB. Compared with the phase noise and loss mechanisms coupled from the environment and surrounding vacuum, experimentally, the degradation information is unveiled with machine learning for low and high noisy scenarios, i.e., with the antisqueezing levels at 12 dB and 18 dB, respectively. Our neural network enhanced quantum state tomography provides the metrics to give physical descriptions of every feature observed in the quantum state with a single scan measurement just by varying the local oscillator phase from 0 to 2 pi and paves a way of exploring large-scale quantum systems in real time.

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