• Advanced Photonics
  • Vol. 5, Issue 2, 026006 (2023)
Yingxuan Chen1, Qiqi Zhu1, Xutong Wang1, Yanbo Lou1、*, Shengshuai Liu1、*, and Jietai Jing1、2、3、*
Author Affiliations
  • 1East China Normal University, State Key Laboratory of Precision Spectroscopy, Joint Institute of Advanced Science and Technology, School of Physics and Electronic Science, Shanghai, China
  • 2CAS Center for Excellence in Ultra-intense Laser Science, Shanghai, China
  • 3Shanxi University, Collaborative Innovation Center of Extreme Optics, Taiyuan, China
  • show less
    DOI: 10.1117/1.AP.5.2.026006 Cite this Article Set citation alerts
    Yingxuan Chen, Qiqi Zhu, Xutong Wang, Yanbo Lou, Shengshuai Liu, Jietai Jing. Deterministic all-optical quantum state sharing[J]. Advanced Photonics, 2023, 5(2): 026006 Copy Citation Text show less
    The detailed experimental setup of the deterministic AOQSS protocol. (a) The detailed experimental scheme. (b) {1,2} reconstruction structure. (c) {1,3} reconstruction structure. (d) {2,3} reconstruction structure. HWP, half-wave plate; GL, Glan–laser polarizer; GT, Glan–Thompson polarizer; a^in, the annihilation operator associated with the secret coherent state; a^1, a^2, and a^3, the annihilation operators associated with three shares held by player1, player2, and player3, respectively. (e) Energy level diagram of the double-Λ scheme in the D1 line of Rb85. Δ, one-photon detuning; δ, two-photon detuning.
    Fig. 1. The detailed experimental setup of the deterministic AOQSS protocol. (a) The detailed experimental scheme. (b) {1,2} reconstruction structure. (c) {1,3} reconstruction structure. (d) {2,3} reconstruction structure. HWP, half-wave plate; GL, Glan–laser polarizer; GT, Glan–Thompson polarizer; a^in, the annihilation operator associated with the secret coherent state; a^1, a^2, and a^3, the annihilation operators associated with three shares held by player1, player2, and player3, respectively. (e) Energy level diagram of the double-Λ scheme in the D1 line of Rb85. Δ, one-photon detuning; δ, two-photon detuning.
    The typical noise power results for {1,2} reconstruction structure. (a) and (b) The amplitude and phase quadrature variances with classical modulations for the input secret state (blue dashed traces) and the output state (orange solid traces), respectively. (c) and (d) The amplitude and phase quadrature variances without classical modulations for the input secret state (blue traces) and the output state (orange traces) at 1.5 MHz, respectively. The vertical scale is normalized to the quadrature variances of the input secret state.
    Fig. 2. The typical noise power results for {1,2} reconstruction structure. (a) and (b) The amplitude and phase quadrature variances with classical modulations for the input secret state (blue dashed traces) and the output state (orange solid traces), respectively. (c) and (d) The amplitude and phase quadrature variances without classical modulations for the input secret state (blue traces) and the output state (orange traces) at 1.5 MHz, respectively. The vertical scale is normalized to the quadrature variances of the input secret state.
    The typical noise power results for {1,3} reconstruction structure and the corresponding adversary structure {2}. (a) and (b) The amplitude and phase quadrature variances with classical modulations for the input secret state (blue dashed traces) and the output state (orange solid traces) of the classical {1,3} structure, respectively. (c) and (d) The amplitude and phase quadrature variances without the classical modulations for the input secret state (blue traces), the output state of {1,3} structure (green traces), and the corresponding classical {1,3} structure (orange traces), respectively. The center frequency of SA is set to 1.5 MHz. (e) and (f) The amplitude and phase quadrature variances of {2} structure, respectively. The input secret state and the output state with (without) classical modulations are shown as the blue (black) traces and the orange (red) traces, respectively. The vertical scale is normalized to the quadrature variances of the input secret state.
    Fig. 3. The typical noise power results for {1,3} reconstruction structure and the corresponding adversary structure {2}. (a) and (b) The amplitude and phase quadrature variances with classical modulations for the input secret state (blue dashed traces) and the output state (orange solid traces) of the classical {1,3} structure, respectively. (c) and (d) The amplitude and phase quadrature variances without the classical modulations for the input secret state (blue traces), the output state of {1,3} structure (green traces), and the corresponding classical {1,3} structure (orange traces), respectively. The center frequency of SA is set to 1.5 MHz. (e) and (f) The amplitude and phase quadrature variances of {2} structure, respectively. The input secret state and the output state with (without) classical modulations are shown as the blue (black) traces and the orange (red) traces, respectively. The vertical scale is normalized to the quadrature variances of the input secret state.
    The experimental fidelities versus the sideband frequency. The fidelities of deterministic AOQSS with a {1,3} reconstruction structure and corresponding experimental classical limit are shown as the blue trace and the orange trace, respectively. The error bars are obtained from the standard deviations of multiple repeated measurements.
    Fig. 4. The experimental fidelities versus the sideband frequency. The fidelities of deterministic AOQSS with a {1,3} reconstruction structure and corresponding experimental classical limit are shown as the blue trace and the orange trace, respectively. The error bars are obtained from the standard deviations of multiple repeated measurements.
    Yingxuan Chen, Qiqi Zhu, Xutong Wang, Yanbo Lou, Shengshuai Liu, Jietai Jing. Deterministic all-optical quantum state sharing[J]. Advanced Photonics, 2023, 5(2): 026006
    Download Citation