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    • 53. 发明公开
    • VORRICHTUNG ZUR ERZEUGUNG KURZER IMPULSE DURCH PASSIVE MODENKOPPLUNG
    • 装置于产生短IMPULSE被动模式耦合
    • EP1166403A1
    • 2002-01-02
    • EP00930991.5
    • 2000-03-24
    • Forschungsverbund Berlin e.V.
    • GLAS, PeterLEITNER, Martin
    • H01S3/098G02F1/35
    • H01S3/1112G02F1/3511G02F1/3526H01S3/0805H01S3/08059H01S3/1118
    • Conventional devices for producing very short laser pulses in which an optical medium as the laser source is arranged between two reflectors are provided with a reflector that is provided with semiconductor layers that absorb the incident laser beam depending on the intensity thereof. The aim of the invention is to provide such a device that is easy to produce and does not require a complicated adjustment. To this end, the optical non-linear reflector (2) consists of a refraction-controlled semiconductor layer (7) that has an intensity-depending refractive index and a highly refractive layer (8). A diaphragm (4) and a lens system that consists of at least two lenses (5, 6) is arranged in the beam path between the laser source (3) and the non-linear reflector (2). The distance (a) between the lens (6) and the refraction-controlled layer (7) of the non-linear refractor (2) is adjusted in such a manner that the resulting diameter (12) of the intensity distribution is larger for small intensities than the diameter of the diaphragm (4). The inventive device is easy to produce, can be integrated and easily adapted to different lasers. The inventive device can be used to compensate refractive effects since the refractive index increments for the refraction-controlled semiconductor layer (7) and the optical media (3, 5, 6) have opposite algebraic signs.
    • 55. 发明公开
    • MULTIWAVELENGTH ACTIVELY MODE-LOCKED EXTERNAL CAVITY SEMICONDUCTOR LASER
    • 多波长有源模式锁定外腔半导体激光器
    • EP1121734A1
    • 2001-08-08
    • EP99969540.6
    • 1999-09-20
    • Sarnoff Corporation
    • ABELES, Joseph, Hy
    • H01S3/098
    • H01S5/0657G02B6/4206G02B6/4215G02B6/4245G02B6/4248G02B6/4251G02B6/4271G02B6/4285H01S5/0222H01S5/02284H01S5/141H01S5/142H01S5/146H01S5/4062H01S5/4068H01S5/4087H01S5/50Y10T74/18656
    • A multiwavelength mode-locked MWML angled-stripe SOA laser that emits multiple discrete groups of wavelengths simultaneously in a short time interval, where each group is located at a wavelength suitable to wavelength division multiplexed optical transmission. Feedback (60, 70) and/or feedthrough optics (90) are combined with an angled-stripe SOA to provide different laser embodiments. The actively mode locked MWML laser emits individual spectral components at a plurality of wavelengths simultaneously. The optics are coupled to one or more angled-stripe SOA ports in reflective or optical ring resonator configurations to provide simultaneous feedback at the plurality of wavelengths and to provide substantially identical round-trip travel times and net gains within the lasing cavity for pulses at each of the plurality of wavelengths. A MWML laser so formed is particularly useful as a multiwavelength source for optical signal processing and transmission systems and can be placed in a hermetically sealed package.
    • 一种多波长锁模MWML成角度SOA SOA激光器,可在短时间间隔内同时发射多个离散波长组,其中每个组位于适合于波分复用光传输的波长。 反馈(60,70)和/或馈通光学器件(90)与成角度的SOA结合以提供不同的激光器实施例。 主动模式锁定的MWML激光器同时发射多个波长的单个光谱分量。 光学器件耦合到反射式或光学环形谐振器配置中的一个或多个成角度的SOA端口,以在多个波长处提供同时反馈,并且在激光谐振腔内为每个脉冲提供基本相同的往返传播时间和净增益 在多个波长中。 这样形成的MWML激光器作为用于光信号处理和传输系统的多波长源特别有用,并且可以放置在密封封装中。
    • 56. 发明公开
    • Laser oscillator with transverse mode control
    • 激光振荡器
    • EP1119084A1
    • 2001-07-25
    • EP00306862.4
    • 2000-08-10
    • Intralase Corporation
    • Horvath, Christopher
    • H01S3/098H01S3/106
    • H01S3/08H01S3/08045H01S3/0805H01S3/081H01S3/106H01S3/1118
    • An oscillator (10) for isolating a transverse electro-magnetic (TEM) zero-zero mode pulsed laser beam includes a laser pumping diode (12) that is mounted on a base to induce a multi-mode laser beam (26) from a lasing medium (24). As initially induced, the multi-mode laser beam (26) is directed along a path and is characterized by a beating signal which has a frequency that is based on amplitude variations of laser pulses in the multi-mode laser beam (26). Electronics (42) detect this beating signal and generates a responsive error signal. With closed loop control, the error signal is used to advance a straightedge (50) toward the path of the multi-mode laser beam (26) to remove transverse modes from the multi-mode laser beam (26) with the straightedge (50). This advancement continues until the error signal is a null and the zero-zero mode pulsed laser beam is thereby isolated.
    • 用于隔离横向电磁(TEM)零 - 零模式脉冲激光束的振荡器(10)包括激光泵浦二极管(12),其安装在基座上以从激光器引导多模激光束(26) 中等(24)。 如最初感应的那样,多模激光束(26)沿着路径被引导,并且其特征在于具有基于多模激光束(26)中的激光脉冲的幅度变化的频率的跳动信号。 电子(42)检测该跳动信号并产生响应误差信号。 通过闭环控制,使用误差信号使直尺(50)朝向多模激光束(26)的路径前进,以从多模激光束(26)中移除横模,并具有直线(50) 。 这一进展继续进行,直到误差信号为零,从而分离零零模式的脉冲激光束。
    • 57. 发明公开
    • Saturable Bragg reflectors and their use in mode-locked lasers
    • 在Modengekoppelten Lasern的SättigbareBragg-Reflektoren und ihre Verwendung
    • EP1071179A2
    • 2001-01-24
    • EP00305863.3
    • 2000-07-11
    • LUCENT TECHNOLOGIES INC.
    • Cunningham, John E.Knox, Wayne H.
    • H01S3/098G02F1/35
    • H01S3/1118G02F1/3523
    • A saturable Bragg reflector for use in mode locking a laser comprises a stack alternately of layers of a high index of refraction and layers of a low index of refraction. The layers of high index all have optical thicknesses of about one quarter the operating wavelength of the laser. The layers of low index, except for the pair of uppermost layers, have optical thicknesses of a quarter the operating wavelength but that pair have a thickness of about one eighth of a wavelength. A quantum well is located near the center of the layer of high index between the pair of one eighth wavelength. Such a reflector is used as one end of a resonant cavity that houses a gain medium.
    • 用于模式锁定激光器的饱和布拉格反射器包括交替折射率高的折射率层和低折射率层的堆叠。 高折射率层都具有约1/4激光器工作波长的光学厚度。 除了一对最上层之外,低折射率层具有四分之一工作波长的光学厚度,但是该对具有约八分之一波长的厚度。 量子阱位于一对八分之一波长之间的高折射率层的中心附近。 这种反射器用作容纳增益介质的谐振腔的一端。