• Laser & Optoelectronics Progress
  • Vol. 57, Issue 7, 071609 (2020)
Bing Liu, Xuping Wang*, Yuguo Yang, Yanyan Hu, Huajian Yu, and Fengnian Wu
Author Affiliations
  • Advanced Materials Institute, Qilu University of Technology (Shandong Academy of Sciences), Jinan, Shandong 250014, China
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    DOI: 10.3788/LOP57.071609 Cite this Article Set citation alerts
    Bing Liu, Xuping Wang, Yuguo Yang, Yanyan Hu, Huajian Yu, Fengnian Wu. Principles, Devices, and Applications of Beam Deflection Based on Quadratic Electro-Optic Effect of Potassium Tantalate Niobate[J]. Laser & Optoelectronics Progress, 2020, 57(7): 071609 Copy Citation Text show less
    Space-charge-controlled electro-optic deflection[52]
    Fig. 1. Space-charge-controlled electro-optic deflection[52]
    Voltage profile of new electro-optic deflection model[30]
    Fig. 2. Voltage profile of new electro-optic deflection model[30]
    Deflection angle as a function of applied voltage at 100 kHz[30]
    Fig. 3. Deflection angle as a function of applied voltage at 100 kHz[30]
    Schematic of electro-optic deflection based on KTN composition gradient[45]
    Fig. 4. Schematic of electro-optic deflection based on KTN composition gradient[45]
    Variation in electro-optic deflection angle with applied voltage based on KTN composition gradient[45]
    Fig. 5. Variation in electro-optic deflection angle with applied voltage based on KTN composition gradient[45]
    Diagram of temperature gradient of KTN[37]
    Fig. 6. Diagram of temperature gradient of KTN[37]
    Temperature gradient induced electro-optic deflection angle varies with applied voltage[63]
    Fig. 7. Temperature gradient induced electro-optic deflection angle varies with applied voltage[63]
    KTN electro-optic deflector with multiple reflection structure. (a) Reflection for twice[65] (b) reflection for six times[66]
    Fig. 8. KTN electro-optic deflector with multiple reflection structure. (a) Reflection for twice[65] (b) reflection for six times[66]
    Quadratic electro-optic coefficient as a function of temperature at different cooling rates[34]
    Fig. 9. Quadratic electro-optic coefficient as a function of temperature at different cooling rates[34]
    Response time of electro-optic rotation of KTN crystal at different temperature[38]
    Fig. 10. Response time of electro-optic rotation of KTN crystal at different temperature[38]
    Number of resolvable points for electro-optic deflector[65]
    Fig. 11. Number of resolvable points for electro-optic deflector[65]
    Tracing result of deflected beam of KTN[73]. (a) Beam distortion; (b) beam shaping
    Fig. 12. Tracing result of deflected beam of KTN[73]. (a) Beam distortion; (b) beam shaping
    Power consumption versus frequency[77]
    Fig. 13. Power consumption versus frequency[77]
    Schematic diagram of KTN deflector[66]
    Fig. 14. Schematic diagram of KTN deflector[66]
    Space charge density distributions in KTN with applied voltage[79]. (a) With different voltages; (b) with different permittivities
    Fig. 15. Space charge density distributions in KTN with applied voltage[79]. (a) With different voltages; (b) with different permittivities
    Electron penetration depth as a function of time[82]
    Fig. 16. Electron penetration depth as a function of time[82]
    Size of PNRs versus temperature[69]
    Fig. 17. Size of PNRs versus temperature[69]
    D-E curves of KTN crystal with platinum electrode[88]
    Fig. 18. D-E curves of KTN crystal with platinum electrode[88]
    Deflection angle caused by field-induced phase transition varies with applied voltage[90]
    Fig. 19. Deflection angle caused by field-induced phase transition varies with applied voltage[90]
    Deflection angle at different positions in x direction with 2000 V applied voltage[39]
    Fig. 20. Deflection angle at different positions in x direction with 2000 V applied voltage[39]
    Illustration of KTN varifocal lens[95].(a)Apparatus; (b)optical path length at different positions in x direction
    Fig. 21. Illustration of KTN varifocal lens[95].(a)Apparatus; (b)optical path length at different positions in x direction
    Schematic of experimental setup for 1×5 optical switch[104]
    Fig. 22. Schematic of experimental setup for 1×5 optical switch[104]
    Electric-field-induced superlattice optical switching effect in Cu-doped KTN crystals[106]. (a) Diffraction spot induced by spontaneously formed superlattices; (b)(c) optical switching states of diffraction spot with 1 Hz square-wave voltage
    Fig. 23. Electric-field-induced superlattice optical switching effect in Cu-doped KTN crystals[106]. (a) Diffraction spot induced by spontaneously formed superlattices; (b)(c) optical switching states of diffraction spot with 1 Hz square-wave voltage
    Setup of swept light source with KTN electro-optic deflector[33]
    Fig. 24. Setup of swept light source with KTN electro-optic deflector[33]
    3D OCT image of strawberry surface[109]
    Fig. 25. 3D OCT image of strawberry surface[109]
    Schematic of spectrometer using KTN optical beam deflector[110]
    Fig. 26. Schematic of spectrometer using KTN optical beam deflector[110]
    Spatial overlap modulation nonlinear optical microscopy[112]
    Fig. 27. Spatial overlap modulation nonlinear optical microscopy[112]
    Illustration of time division multiplexed beam combining technique[113]
    Fig. 28. Illustration of time division multiplexed beam combining technique[113]
    SampleDamage threshold /(MW·cm-2)Ratio of damage threshold of sample todamage threshold of LiNbO3
    Colorless LGS950.009.5000
    DKDP3260.0032.6000
    LiNbO3100.001.0000
    KTN0.260.0026
    Table 1. Damage thresholds of several optical crystals
    Bing Liu, Xuping Wang, Yuguo Yang, Yanyan Hu, Huajian Yu, Fengnian Wu. Principles, Devices, and Applications of Beam Deflection Based on Quadratic Electro-Optic Effect of Potassium Tantalate Niobate[J]. Laser & Optoelectronics Progress, 2020, 57(7): 071609
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