• Chinese Optics Letters
  • Vol. 21, Issue 9, 092701 (2023)
Weihang Zhang1、2, Yinghao Ye1、2、3, Lei Zeng1、2, Enze Li1、2, Jingyuan Peng1、2, Dongsheng Ding1、2、*, and Baosen Shi1、2、**
Author Affiliations
  • 1CAS Key Laboratory of Quantum Information, University of Science and Technology of China, Hefei 230026, China
  • 2CAS Center for Excellence in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei 230026, China
  • 3Institute for Quantum Control and Quantum Information and School of Physics and Materials Engineering, Hefei Normal University, Hefei 230601, China
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    DOI: 10.3788/COL202321.092701 Cite this Article Set citation alerts
    Weihang Zhang, Yinghao Ye, Lei Zeng, Enze Li, Jingyuan Peng, Dongsheng Ding, Baosen Shi. High-dimensional frequency conversion in a hot atomic system[J]. Chinese Optics Letters, 2023, 21(9): 092701 Copy Citation Text show less
    (a) Energy diagram of the diamond configuration. (b) The schematic diagram of the experimental setup. SLM 1 and SLM 2, spatial light modulator; PBS, polarizing beam splitter; DM, long-pass dichroic mirror; SF, short-pass filter; BF, band-pass filter; BT, beam traps; SMF 1 and SMF 2, single-mode fiber; M, mirror. The focal lengths of lenses L1, L2, L3, L4, L5, and L6 are 75, 150, 150, 150, 150, and 75 mm, respectively.
    Fig. 1. (a) Energy diagram of the diamond configuration. (b) The schematic diagram of the experimental setup. SLM 1 and SLM 2, spatial light modulator; PBS, polarizing beam splitter; DM, long-pass dichroic mirror; SF, short-pass filter; BF, band-pass filter; BT, beam traps; SMF 1 and SMF 2, single-mode fiber; M, mirror. The focal lengths of lenses L1, L2, L3, L4, L5, and L6 are 75, 150, 150, 150, 150, and 75 mm, respectively.
    (a) Intensity profiles of the input POV beams (red) and the converted POV beams (blue). (b),(c) The distribution of conversion efficiency η (unit is ‰) with different values of l in the case of kr = 6.13 mm−1 and kr = 24.51 mm−1. The η is estimated from the power and wavelength of lights before and after frequency conversion.
    Fig. 2. (a) Intensity profiles of the input POV beams (red) and the converted POV beams (blue). (b),(c) The distribution of conversion efficiency η (unit is ‰) with different values of l in the case of kr = 6.13 mm−1 and kr = 24.51 mm−1. The η is estimated from the power and wavelength of lights before and after frequency conversion.
    (a) Cross-talk matrix between the input and the converted beams formed by the POV states in subspace {|−6〉,…,|6〉}. (b) The theoretical, input, and converted beam intensity profiles of four 2D states. (c) The real and imaginary parts of the reconstructed density matrix for the four 2D states.
    Fig. 3. (a) Cross-talk matrix between the input and the converted beams formed by the POV states in subspace {|−6〉,…,|6〉}. (b) The theoretical, input, and converted beam intensity profiles of four 2D states. (c) The real and imaginary parts of the reconstructed density matrix for the four 2D states.
    (a) The theoretical, input, and converted beam intensity profiles of the 3D, 5D, and 7D states. (b) The real and imaginary parts of the reconstructed density matrix for the 3D, 5D, and 7D states. (c) The distribution of conversion efficiency η with different states |Ψ〉, where |2D1〉 = (|0〉 + |6〉)/2, |2D2〉 = (|1〉 + |−5〉)/2, |2D3〉 = (|2〉 + |4〉)/2, |2D4〉 = (|−3〉 + |−6〉)/2, |3D〉 = (|−1〉+|3〉 + |−6〉)/3, |5D〉 = (|0〉 + |1〉 + |−3〉 + |−5〉 + |6〉)/5, and |7D〉 = (|0〉 + |−1〉 + |2〉 + |3〉 + |−4〉 + |5〉 + |−6〉)/7.
    Fig. 4. (a) The theoretical, input, and converted beam intensity profiles of the 3D, 5D, and 7D states. (b) The real and imaginary parts of the reconstructed density matrix for the 3D, 5D, and 7D states. (c) The distribution of conversion efficiency η with different states |Ψ〉, where |2D1〉 = (|0〉 + |6〉)/2, |2D2〉 = (|1〉 + |−5〉)/2, |2D3〉 = (|2〉 + |4〉)/2, |2D4〉 = (|−3〉 + |−6〉)/2, |3D〉 = (|−1〉+|3〉 + |−6〉)/3, |5D〉 = (|0〉 + |1〉 + |−3〉 + |−5〉 + |6〉)/5, and |7D〉 = (|0〉 + |−1〉 + |2〉 + |3〉 + |−4〉 + |5〉 + |−6〉)/7.
    Weihang Zhang, Yinghao Ye, Lei Zeng, Enze Li, Jingyuan Peng, Dongsheng Ding, Baosen Shi. High-dimensional frequency conversion in a hot atomic system[J]. Chinese Optics Letters, 2023, 21(9): 092701
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