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    • 71. 发明授权
    • THz wave generation device
    • 太赫兹波发生装置
    • US07764422B2
    • 2010-07-27
    • US11992801
    • 2006-09-27
    • Junichiro Ichikawa
    • Junichiro Ichikawa
    • G02F1/355H01S3/11H01S3/16
    • G02F1/3534G02F2202/02G02F2203/13H01S1/02H01S3/0078H01S3/06754H01S3/1608H01S3/30
    • In a THz wave generator for generating a THz wave from a THz wave generating element by inputting a plurality of laser beams having different wavelengths to the THz wave generating element, all of the plurality of laser beams are formed into a pulse beam by the pulse generator and the pulse beam is amplified by a single optical amplifier E to which the laser beams are inputted with polarization planes of the laser beams being controlled, and then the pulse beam is inputted to the THz wave generating element F. Preferably, the plurality of laser beams having different wavelengths are generated by inputting single wavelength beam to a multi wavelength generator from single mode laser light source and by inputting light waves having a plurality of wavelengths generated from the multi wavelength generator to wavelength selecting means.
    • 在用于通过将具有不同波长的多个激光束输入到太赫兹波发生元件从太赫兹波发生元件产生太赫兹波的太赫兹波发生器中,所有多个激光束都被脉冲发生器形成为脉冲波束 并且脉冲束被激光束输入的单个光学放大器E放大,激光束的偏振面被控制,然后脉冲光束被输入到太赫兹波发生元件F.优选地,多个激光 通过从单模激光光源将单波长光束输入到多波长发生器并通过将具有从多波长发生器产生的多个波长的光波输入到波长选择装置来产生具有不同波长的光束。
    • 73. 发明授权
    • Light intensity attenuator and attenuating method
    • 光强衰减器和衰减方法
    • US6134372A
    • 2000-10-17
    • US319068
    • 1999-06-01
    • Junichiro IchikawaHirotoshi NagataKaoru HigumaJunichiro MinowaTakaaki OgataYasuhisa Taneda
    • Junichiro IchikawaHirotoshi NagataKaoru HigumaJunichiro MinowaTakaaki OgataYasuhisa Taneda
    • G02F1/01G02F1/35G02F1/365G02F1/37G02F1/377G02B6/122
    • G02F1/3511G02F1/365G02F1/0147G02F1/377G02F2001/374
    • A light intensity attenuator and attenuating method is provided, by which a pulse-shaped optical surge can be attenuated and an optical signal component using desired light intensity can be output by using a simpler structural arrangement, and without using many optical components and circuits. In this method, an optical signal including a pulse-shaped optical surge component is received, and the optical signal is again output after the light intensity of the surge component is attenuated by a desired amount. Typically, (i) at least one of a substrate and an optical waveguide formed on the substrate is made of a material producing a nonlinear optical effect, and the refractive index of the optical waveguide with respect to the optical signal is smaller than the refractive index of the substrate with respect to a higher harmonic of the optical signal, thereby wavelength-converting a part of the input optical signal by the nonlinear optical effect into a light portion having a wavelength shorter than that of the optical signal, and scattering this converted portion, and (ii) a part of the optical signal is scattered by using a polar-molecule liquid including polar molecules.
    • PCT No.PCT / JP98 / 04346 Sec。 371日期1999年6月1日 102(e)1999年6月1日PCT PCT 1998年9月20日PCT公布。 公开号WO99 /​​ 17472 日期1999年4月8日提供了一种光强度衰减器和衰减方法,通过该光强度衰减器和衰减方法可以衰减脉冲形波浪,并且可以通过使用更简单的结构布置输出使用期望光强的光信号分量,并且不使用许多光 组件和电路。 在该方法中,接收包括脉冲状波浪分量的光信号,并且在浪涌元件的光强度衰减期望量之后再次输出光信号。 通常,(i)形成在基板上的基板和光波导中的至少一个由产生非线性光学效应的材料制成,光波导相对于光信号的折射率小于折射率 相对于光信号的高次谐波而使输入光信号的一部分通过非线性光学效应波长转换为波长短于光信号的波长的光部分,并将该转换部分散射 ,和(ii)通过使用包含极性分子的极性分子液体来散射光信号的一部分。