• Acta Physica Sinica
  • Vol. 69, Issue 8, 080301-1 (2020)
Xiang-Yan Li, Zhi-Hui Wang, Shao-Kang Li, Ya-Li Tian, Gang Li*, Peng-Fei Zhang, and Tian-Cai Zhang*
Author Affiliations
  • Collaborative Innovation Center of Extreme Optics, State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Opto-Electronics, Shanxi University, Taiyuan 030006, China
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    DOI: 10.7498/aps.69.20192001 Cite this Article
    Xiang-Yan Li, Zhi-Hui Wang, Shao-Kang Li, Ya-Li Tian, Gang Li, Peng-Fei Zhang, Tian-Cai Zhang. Measurement of magnetically insensitive state coherent time in blue dipole trap[J]. Acta Physica Sinica, 2020, 69(8): 080301-1 Copy Citation Text show less
    The relative DES (differential energy shift) between cesium hyperfine states and functional relationship with the magnetic field. The blue star indicates the magic magnetic field.
    Fig. 1. The relative DES (differential energy shift) between cesium hyperfine states and functional relationship with the magnetic field. The blue star indicates the magic magnetic field.
    The experimental setup for the trapping of a single cesium atom in the blue detuned dipole trap.
    Fig. 2. The experimental setup for the trapping of a single cesium atom in the blue detuned dipole trap.
    (a) Energy scheme for initialization of Zeeman state by optical pumping; (b) the preparation of qubit through two-photon Raman transition. is the intermediate state detuning from the excited state ; (c) two-photon Raman Rabi oscillations on the transition. The red solid line is fits to a Rabi sinc function; (d) two-photon Raman Rabi oscillations on the , F = 4, transition. The oscillation is a fit according to cosine function. Each point is the statistics over 100 shoots.
    Fig. 3. (a) Energy scheme for initialization of Zeeman state by optical pumping; (b) the preparation of qubit through two-photon Raman transition. is the intermediate state detuning from the excited state ; (c) two-photon Raman Rabi oscillations on the transition. The red solid line is fits to a Rabi sinc function; (d) two-photon Raman Rabi oscillations on the , F = 4, transition. The oscillation is a fit according to cosine function. Each point is the statistics over 100 shoots.
    The relative DES between states and , solid line is the functional fitting. Inset is the Raman spectrum measured at B = 1.233 Gauss, the relative offset of spectrum is –1.957(4) kHz.
    Fig. 4. The relative DES between states and , solid line is the functional fitting. Inset is the Raman spectrum measured at B = 1.233 Gauss, the relative offset of spectrum is –1.957(4) kHz.
    Experimental results for the coherence time measurements: (a) The Ramsey spectrum. The fitting by gives the coherence time of 11(1) ms; (b) the decay of the amplitude of spin echo signal. The exponential fitting (solid line) gives a coherence time of . Insert is the spin echo signal at evolution time of .
    Fig. 5. Experimental results for the coherence time measurements: (a) The Ramsey spectrum. The fitting by gives the coherence time of 11(1) ms; (b) the decay of the amplitude of spin echo signal. The exponential fitting (solid line) gives a coherence time of . Insert is the spin echo signal at evolution time of .
    Xiang-Yan Li, Zhi-Hui Wang, Shao-Kang Li, Ya-Li Tian, Gang Li, Peng-Fei Zhang, Tian-Cai Zhang. Measurement of magnetically insensitive state coherent time in blue dipole trap[J]. Acta Physica Sinica, 2020, 69(8): 080301-1
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