• Laser & Optoelectronics Progress
  • Vol. 59, Issue 11, 1100001 (2022)
Zhongzhong Qin1, Meihong Wang1, Rong Ma1、2, and Xiaolong Su1、*
Author Affiliations
  • 1State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Opto-Electronics, Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, Shanxi , China
  • 2College of Physics and Electronic Engineering, Shanxi University, Taiyuan 030006, Shanxi , China
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    DOI: 10.3788/LOP202259.1100001 Cite this Article Set citation alerts
    Zhongzhong Qin, Meihong Wang, Rong Ma, Xiaolong Su. Progress of the Squeezed States of Light and Their Application[J]. Laser & Optoelectronics Progress, 2022, 59(11): 1100001 Copy Citation Text show less
    Wigner functions of quantum states. (a) Vacuum state; (b) coherent state; (c)(d) amplitude quadrature and phase quadrature squeezed vacuum states; (e)(f) amplitude quadrature and phase quadrature squeezed coherent states (insets: corresponding edge distribution of quadrature amplitude and quadrature phase components of Wigner function) [31]
    Fig. 1. Wigner functions of quantum states. (a) Vacuum state; (b) coherent state; (c)(d) amplitude quadrature and phase quadrature squeezed vacuum states; (e)(f) amplitude quadrature and phase quadrature squeezed coherent states (insets: corresponding edge distribution of quadrature amplitude and quadrature phase components of Wigner function) [31]
    Wavefunctions of two-mode states in the position (left) and momentum (right) bases. (a) Two-mode vacuum state is uncorrelated in both bases; (b) two-mode squeezed state with amplitude quadrature correlated, and phase quadrature observables anticorrelated; (c) two-mode squeezed state with amplitude quadrature anticorrelated, and phase quadrature correlated [31]
    Fig. 2. Wavefunctions of two-mode states in the position (left) and momentum (right) bases. (a) Two-mode vacuum state is uncorrelated in both bases; (b) two-mode squeezed state with amplitude quadrature correlated, and phase quadrature observables anticorrelated; (c) two-mode squeezed state with amplitude quadrature anticorrelated, and phase quadrature correlated [31]
    Optical parametric amplifier. (a) Degenerate optical parametric amplifier; (b) polarization non-degenerate optical parametric amplifier
    Fig. 3. Optical parametric amplifier. (a) Degenerate optical parametric amplifier; (b) polarization non-degenerate optical parametric amplifier
    Four-wave mixing process in atomic ensemble. (a) Single-mode squeezed state generated from degenerate case; (b) two-mode squeezed state generated from non-degenerate case [34]
    Fig. 4. Four-wave mixing process in atomic ensemble. (a) Single-mode squeezed state generated from degenerate case; (b) two-mode squeezed state generated from non-degenerate case [34]
    Principle of balanced homodyne detection [31]
    Fig. 5. Principle of balanced homodyne detection [31]
    Principle and schematic of the test principle for error-tradeoff relation by using a EPR entangled state[54]
    Fig. 6. Principle and schematic of the test principle for error-tradeoff relation by using a EPR entangled state[54]
    Schematic of connecting two local quantum networks by quantum entanglement swapping [25]
    Fig. 7. Schematic of connecting two local quantum networks by quantum entanglement swapping [25]
    Schematic of the gate sequence based on continuous-variable cluster state [10]
    Fig. 8. Schematic of the gate sequence based on continuous-variable cluster state [10]
    Schematic of using amplitude-squeezed state of light to enhance the sensitivity of LIGO. (a) Schematic of experimental setup; (b) Wigner function projections of coherent state and squeezed coherent state in phase space; (c) photocurrents of coherent state and squeezed coherent state [31]
    Fig. 9. Schematic of using amplitude-squeezed state of light to enhance the sensitivity of LIGO. (a) Schematic of experimental setup; (b) Wigner function projections of coherent state and squeezed coherent state in phase space; (c) photocurrents of coherent state and squeezed coherent state [31]
    Schematic of quantum-enhanced stimulated Raman scattering microscopy. (a) Schematic of experimental setup; (b) vibration spectra of different molecules [93]
    Fig. 10. Schematic of quantum-enhanced stimulated Raman scattering microscopy. (a) Schematic of experimental setup; (b) vibration spectra of different molecules [93]
    Zhongzhong Qin, Meihong Wang, Rong Ma, Xiaolong Su. Progress of the Squeezed States of Light and Their Application[J]. Laser & Optoelectronics Progress, 2022, 59(11): 1100001
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