• Chinese Optics Letters
  • Vol. 16, Issue 6, 060201 (2018)
Yingyu Niu* and Rong Wang
Author Affiliations
  • School of Science, Dalian Jiaotong University, Dalian 116028, China
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    DOI: 10.3788/COL201816.060201 Cite this Article Set citation alerts
    Yingyu Niu, Rong Wang. Photoassociation reaction of OH molecules through reverse ladder transition[J]. Chinese Optics Letters, 2018, 16(6): 060201 Copy Citation Text show less
    Processes of the reverse ladder transition.
    Fig. 1. Processes of the reverse ladder transition.
    Process of PA for the target state |9,0〉 in two laser pulses. (a) The total electric field of two laser pulses. (b) The time-dependent population distributions for rovibrational states. (c) The population distributions of the intermediate and background states at the end of laser pulses.
    Fig. 2. Process of PA for the target state |9,0 in two laser pulses. (a) The total electric field of two laser pulses. (b) The time-dependent population distributions for rovibrational states. (c) The population distributions of the intermediate and background states at the end of laser pulses.
    Time-dependent population distributions versus the amplitude E1 of the first pulse for the target state |9,0〉.
    Fig. 3. Time-dependent population distributions versus the amplitude E1 of the first pulse for the target state |9,0.
    Time-dependent population distributions versus the amplitude E2 of the second pulse for the target state |9,0〉.
    Fig. 4. Time-dependent population distributions versus the amplitude E2 of the second pulse for the target state |9,0.
    Processes of PA for the target states |8,0〉 and |7,0〉 in two laser pulses. (a) The total electric field for the target state |8,0〉. The parameters of the second pulse are E2=168.69 MV/cm, τ2=1.35 ps, t2=0 ps, and ω2=6528.29 cm−1. (b) The total electric field for the target state |7,0〉. Parameters of the second pulse are E2=374.38 MV/cm, τ2=2.88 ps, t2=0 ps, and ω2=9056.01 cm−1. (c) and (d) The time-dependent population distributions for rovibrational states.
    Fig. 5. Processes of PA for the target states |8,0 and |7,0 in two laser pulses. (a) The total electric field for the target state |8,0. The parameters of the second pulse are E2=168.69MV/cm, τ2=1.35ps, t2=0ps, and ω2=6528.29cm1. (b) The total electric field for the target state |7,0. Parameters of the second pulse are E2=374.38MV/cm, τ2=2.88ps, t2=0ps, and ω2=9056.01cm1. (c) and (d) The time-dependent population distributions for rovibrational states.
    Process of PA for the target state |0,0〉 in four laser pulses. (a) The total electric field of four laser pulses. (b) The time-dependent population distributions for rovibrational states.
    Fig. 6. Process of PA for the target state |0,0 in four laser pulses. (a) The total electric field of four laser pulses. (b) The time-dependent population distributions for rovibrational states.
    Yingyu Niu, Rong Wang. Photoassociation reaction of OH molecules through reverse ladder transition[J]. Chinese Optics Letters, 2018, 16(6): 060201
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