• Acta Physica Sinica
  • Vol. 69, Issue 14, 140601-1 (2020)
Yong Guan1、2、3, Dan-Dan Liu1、2、3, Xin-Liang Wang1、2、3, Hui Zhang1、2、3, Jun-Ru Shi1、2、3, Yang Bai1、2、3, Jun Ruan1、2、*, and Shou-Gang Zhang1、2
Author Affiliations
  • 1National Time Service Center, Chinese Academy of Sciences, Xi’an 710600, China
  • 2Key Laboratory of Time and Frequency Primary Standards, National Time Service Center, Chinese Academy of Sciences, Xi’an 710600, China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.7498/aps.69.20191800 Cite this Article
    Yong Guan, Dan-Dan Liu, Xin-Liang Wang, Hui Zhang, Jun-Ru Shi, Yang Bai, Jun Ruan, Shou-Gang Zhang. Investigation of cold atom collision frequency shift measured by rapid adiabatic passage in cesium fountain clock[J]. Acta Physica Sinica, 2020, 69(14): 140601-1 Copy Citation Text show less
    Map of coordinate transformation
    Fig. 1. Map of coordinate transformation
    Scheme of microwave circuit generating RAP pulses.
    Fig. 2. Scheme of microwave circuit generating RAP pulses.
    Transition probability as a function of b0 and δ0 with 8 ms pulse starts 4 ms after atoms entering the cavity: (a) δ0 = 5 kHz, with different b0; (b) b0 = 10 kHz, with different δ0.
    Fig. 3. Transition probability as a function of b0 and δ0 with 8 ms pulse starts 4 ms after atoms entering the cavity: (a) δ0 = 5 kHz, with different b0; (b) b0 = 10 kHz, with different δ0.
    Time evolution of deviation excitation.
    Fig. 4. Time evolution of deviation excitation.
    Transition probability as a function of time parameters, δ0 = 5 kHz, b0 = 10 kHz, atoms enter selection cavity at time 0: (a) Pulse duration remaining symmetric about the central point of cavity; (b) start point of pulse with a fixed duration of 8 ms.
    Fig. 5. Transition probability as a function of time parameters, δ0 = 5 kHz, b0 = 10 kHz, atoms enter selection cavity at time 0: (a) Pulse duration remaining symmetric about the central point of cavity; (b) start point of pulse with a fixed duration of 8 ms.
    Transition probabilty as a function of center frequency detuning.
    Fig. 6. Transition probabilty as a function of center frequency detuning.
    Transition probability as a function of b0 for a 5 kHz δ0 pulse start at 5 different points and end at 10 ms after entering cavity: (a) b0 as the abscissa; (b) b0T as the abscissa.
    Fig. 7. Transition probability as a function of b0 for a 5 kHz δ0 pulse start at 5 different points and end at 10 ms after entering cavity: (a) b0 as the abscissa; (b) b0T as the abscissa.
    Transition probability as a function of (a) b0 for five different δ0, (b) pulse duration with δ0 = 5 kHz, and b0 = 10 kHz.
    Fig. 8. Transition probability as a function of (a) b0 for five different δ0, (b) pulse duration with δ0 = 5 kHz, and b0 = 10 kHz.
    (a) Transition probability as a function of b0 for 100, 0, –100 Hz center frequency detuning; (b) transition probability as a function of center frequency detuning for δ0 = 5 kHz and b0 = 10 kHz.
    Fig. 9. (a) Transition probability as a function of b0 for 100, 0, –100 Hz center frequency detuning; (b) transition probability as a function of center frequency detuning for δ0 = 5 kHz and b0 = 10 kHz.
    Stability of atoms number ratio.
    Fig. 10. Stability of atoms number ratio.
    Transition probability as a function of magnetic field
    Fig. 11. Transition probability as a function of magnetic field
    Yong Guan, Dan-Dan Liu, Xin-Liang Wang, Hui Zhang, Jun-Ru Shi, Yang Bai, Jun Ruan, Shou-Gang Zhang. Investigation of cold atom collision frequency shift measured by rapid adiabatic passage in cesium fountain clock[J]. Acta Physica Sinica, 2020, 69(14): 140601-1
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