• High Power Laser and Particle Beams
  • Vol. 33, Issue 11, 111007 (2021)
Adewale Akinyimika1、2、3, Yulei Wang1、2、*, Zhenxu Bai1、2, Yunfei Li1、2, and Zhiwei Lu1、2
Author Affiliations
  • 1Center for Advanced Laser Technology, Hebei University of Technology, Tianjin 300401, China
  • 2Hebei Key Laboratory of Advanced Laser Technology and Equipment, Hebei University of Technology, Tianjin 300401, China
  • 3Department of Physics, Federal University of Technology Akure, P. M. B 704 Akure, Nigeria
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    DOI: 10.11884/HPLPB202133.210313 Cite this Article
    Adewale Akinyimika, Yulei Wang, Zhenxu Bai, Yunfei Li, Zhiwei Lu. Phase conjugation lasers based on stimulated Brillouin scattering with high-power and high-energy[J]. High Power Laser and Particle Beams, 2021, 33(11): 111007 Copy Citation Text show less
    Nonlinear SBS energy level diagram; ωQ is the phonon frequency,ωS is the Stokes frequency, and ωL is the frequency of the incident electromagnetic wave[73]
    Fig. 1. Nonlinear SBS energy level diagram; ωQ is the phonon frequency,ωS is the Stokes frequency, and ωL is the frequency of the incident electromagnetic wave[73]
    Experimental set-up for measuring SBS medium properties (e.g., OBT)[48]
    Fig. 2. Experimental set-up for measuring SBS medium properties (e.g., OBT)[48]
    (a) SBS-PCM system with a rotating wedge[25] and (b) laser spot at focus plane[62]
    Fig. 3. (a) SBS-PCM system with a rotating wedge[25] and (b) laser spot at focus plane[62]
    (a) Experimental setup of the circulating two-cell structure[60], (b) two SBS cell structure (right) and single cell setup (left)[45]
    Fig. 4. (a) Experimental setup of the circulating two-cell structure[60], (b) two SBS cell structure (right) and single cell setup (left)[45]
    (a) Diagram of the unlocked case, (b) a concentric type produces weak density modulation and (c) backward focusing produces weak density modulation[82]
    Fig. 5. (a) Diagram of the unlocked case, (b) a concentric type produces weak density modulation and (c) backward focusing produces weak density modulation[82]
    A sample experimental setup for a prepulse system. PBS: polarizing beam splitter; HWP: half-wave plate; L1: planoconcave lens; L2 and L3: planoconvex lens; M: mirrors; W: wedge; SBS-PCM (FC75, 30 cm long) [64]
    Fig. 6. A sample experimental setup for a prepulse system. PBS: polarizing beam splitter; HWP: half-wave plate; L1: planoconcave lens; L2 and L3: planoconvex lens; M: mirrors; W: wedge; SBS-PCM (FC75, 30 cm long) [64]
    A typical experimental setup of a four-beam combination system using the RW-SSP. ISO: optical isolator; PZT: 45 degree mirror attached piezoelectric transducer; RW: rotating wedge device; QWP: quarter wave plate; EM: energy meter[40]
    Fig. 7. A typical experimental setup of a four-beam combination system using the RW-SSP. ISO: optical isolator; PZT: 45 degree mirror attached piezoelectric transducer; RW: rotating wedge device; QWP: quarter wave plate; EM: energy meter[40]
    Experimental setup for the measurement of the leak beam patterns and the depolarization ratio for the four possible optical schemes in a double-pass Nd:YAG rod amplifier with an SBS-PCM. W: wedged window; AMP: Nd:YAG rod amplifier; FR: Faraday rotator[59]
    Fig. 8. Experimental setup for the measurement of the leak beam patterns and the depolarization ratio for the four possible optical schemes in a double-pass Nd:YAG rod amplifier with an SBS-PCM. W: wedged window; AMP: Nd:YAG rod amplifier; FR: Faraday rotator[59]
    Reflected energy with rotating off-centered lens and normal lens[25]
    Fig. 9. Reflected energy with rotating off-centered lens and normal lens[25]
    Closed-type SBS-PCM used to measure reflectivity at varying repetition rates. RT: quartz rotator; SF: spatial filter[26]
    Fig. 10. Closed-type SBS-PCM used to measure reflectivity at varying repetition rates. RT: quartz rotator; SF: spatial filter[26]
    Fraction of the light pathway for testing SBS reflectivity[27]
    Fig. 11. Fraction of the light pathway for testing SBS reflectivity[27]
    max. reflectivity (%)input energy/mJfrequency/Hzoutput Pulse width/nsmediumyearreference
    9880020038.8FC-7702017[27]
    95.290017020FC-7702017[52]
    9416020010FC-7702018[26]
    936002009.3FC-7702020[46]
    921050014HT-2702019[61]
    9212050010FC-7702018[26]
    88220100008.5HT-702014[86]
    84.760010FC-722010[60]
    81.2501000HT-2702019[25]
    78.430010FC-722010[51]
    757.365050FC-752005[63]
    6948250008FC-752011[41]
    60130100028FC-752003[87]
    444515000FC-752016[38]
    Table 1. Some scientific achievements in SBS-PCM reflectivity
    Adewale Akinyimika, Yulei Wang, Zhenxu Bai, Yunfei Li, Zhiwei Lu. Phase conjugation lasers based on stimulated Brillouin scattering with high-power and high-energy[J]. High Power Laser and Particle Beams, 2021, 33(11): 111007
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