• Photonics Research
  • Vol. 8, Issue 11, 1697 (2020)
Xiaotian Feng1, Zhifei Yu1, Bing Chen2, Shuying Chen1, Yuan Wu1, Donghui Fan1, Chun-Hua Yuan1、5、*, L. Q. Chen1、6、*, Z. Y. Ou3, and Weiping Zhang4
Author Affiliations
  • 1State Key Laboratory of Precision Spectroscopy, Quantum Institute for Light and Atoms, Department of Physics, East China Normal University, Shanghai 200062, China
  • 2School of Electronic Science and Applied Physics, Hefei University of Technology, Hefei 230009, China
  • 3Department of Physics, Indiana University-Purdue University Indianapolis, Indianapolis, Indiana 46202, USA
  • 4School of Physics and Astronomy, and Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai 200240, China
  • 5e-mail: chyuan@phy.ecnu.edu.cn
  • 6e-mail: lqchen@phy.ecnu.edu.cn
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    DOI: 10.1364/PRJ.400708 Cite this Article Set citation alerts
    Xiaotian Feng, Zhifei Yu, Bing Chen, Shuying Chen, Yuan Wu, Donghui Fan, Chun-Hua Yuan, L. Q. Chen, Z. Y. Ou, Weiping Zhang. Reducing the mode-mismatch noises in atom–light interactions via optimization of the temporal waveform[J]. Photonics Research, 2020, 8(11): 1697 Copy Citation Text show less
    (a) Schematic of the experimental setup. PBS, polarized beam splitter; HWP, half-wave plate; EOM, electro-optic modulator; AOM, acousto-optic modulator; PD, photodetector; AWG, arbitrary wave generator; DPO, digital phosphor oscilloscope. (b) Energy levels of the Rb87 atom and the frequencies of the lasers: |g,m⟩, hyperfine levels |52S1/2,F=1,F=2⟩; |e1,e2⟩, hyperfine levels |52P1/2,F=2⟩ and |52P3/2⟩; W, the Raman pump field; a^in, the initial input Stokes seed; a^out, the output Stokes field via SRS; OP, the optical pumping; S^, the atomic spin wave; R, the read field; b^out, the output anti-Stokes field by the reading process.
    Fig. 1. (a) Schematic of the experimental setup. PBS, polarized beam splitter; HWP, half-wave plate; EOM, electro-optic modulator; AOM, acousto-optic modulator; PD, photodetector; AWG, arbitrary wave generator; DPO, digital phosphor oscilloscope. (b) Energy levels of the Rb87 atom and the frequencies of the lasers: |g,m, hyperfine levels |52S1/2,F=1,F=2; |e1,e2, hyperfine levels |52P1/2,F=2 and |52P3/2; W, the Raman pump field; a^in, the initial input Stokes seed; a^out, the output Stokes field via SRS; OP, the optical pumping; S^, the atomic spin wave; R, the read field; b^out, the output anti-Stokes field by the reading process.
    Iteration diagram. a^in,a^in(1),…,a^in(i) are normalized initially input Stokes seeds; a^out,a^out(1),…,a^out(i) are output signals by SRS, corresponding to the ith iteration.
    Fig. 2. Iteration diagram. a^in,a^in(1),,a^in(i) are normalized initially input Stokes seeds; a^out,a^out(1),,a^out(i) are output signals by SRS, corresponding to the ith iteration.
    (a) and (b) a^in is the initially input seed waveform and a^out(0) is the corresponding output signal of SRS. a^out(1) is the output signal of SRS in the first round, a^out(1) is stable waveform after several iteration rounds. (c) Pink circles and green solid triangles are a^out(f) corresponding to different a^in in (a) and (b), respectively.
    Fig. 3. (a) and (b) a^in is the initially input seed waveform and a^out(0) is the corresponding output signal of SRS. a^out(1) is the output signal of SRS in the first round, a^out(1) is stable waveform after several iteration rounds. (c) Pink circles and green solid triangles are a^out(f) corresponding to different a^in in (a) and (b), respectively.
    (a) and (b) The different energy fluctuations ΔEa^out(0) of a^out(0) and ΔEa^out(f) of a^out(f) during many measurement times. (c) E¯a^out is the average energy of the output Stokes field. Black square and red triangle curves are respective Var(E) for Ea^out(0) and Ea^out(f) both with 100 ns long square-W pulse.
    Fig. 4. (a) and (b) The different energy fluctuations ΔEa^out(0) of a^out(0) and ΔEa^out(f) of a^out(f) during many measurement times. (c) E¯a^out is the average energy of the output Stokes field. Black square and red triangle curves are respective Var(E) for Ea^out(0) and Ea^out(f) both with 100 ns long square-W pulse.
    Black square and red triangle curves are respective Var(EDiff) for a^out(0) and a^out(f) both with the square-W and square-R pulse acquired in the experiment.
    Fig. 5. Black square and red triangle curves are respective Var(EDiff) for a^out(0) and a^out(f) both with the square-W and square-R pulse acquired in the experiment.
    Xiaotian Feng, Zhifei Yu, Bing Chen, Shuying Chen, Yuan Wu, Donghui Fan, Chun-Hua Yuan, L. Q. Chen, Z. Y. Ou, Weiping Zhang. Reducing the mode-mismatch noises in atom–light interactions via optimization of the temporal waveform[J]. Photonics Research, 2020, 8(11): 1697
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