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    • 2. 发明申请
    • AN INTEGRATED OPTICAL DEVICE
    • 一体化光学器件
    • WO1997049150A1
    • 1997-12-24
    • PCT/US1997009495
    • 1997-05-30
    • BELL COMMUNICATIONS RESEARCH, INC.
    • BELL COMMUNICATIONS RESEARCH, INC.AMERSFOORT, MartinZAH, Chung-En
    • H01S03/19
    • H01S5/026G02B6/12004G02B2006/12097G02B2006/12119G02B2006/12176H01S5/1028H01S5/22H01S5/4025
    • An opto-electronic integrated circuit including an active ridge waveguide (60), for example, a semiconductor laser diode, and a passive buried heterostructure semiconductor waveguide (64). The two types of waveguides are chosen for their respective tasks so as to minimize the lasing wavelength dependencies arising from fabricational variations and to simultaneously reduce the allowable bending radius, thus reducing the chip size. The two waveguides are coupled by a transition structure (62), including a laterally undefined slab waveguide. A fabricational method is described that self aligns the ridge and buried heterostructure waveguides so that the transition loss is negligible. The method can be integrated with fabrication of a window facet (118', 118'') between an end of the ridge waveguide and the chip edge, which prevents unintended back reflections from the chip edge.
    • 一种包括有源脊波导(60),例如半导体激光二极管和无源掩埋异质结构半导体波导(64)的光电集成电路。 为了各自的任务选择两种类型的波导,以便最小化由制造变化引起的激光波长依赖性并且同时减小允许的弯曲半径,从而减小芯片尺寸。 两个波导通过过渡结构(62)耦合,包括横向未定义的平板波导。 描述了自对准脊和掩埋异质结构波导的制造方法,使得过渡损耗可以忽略不计。 该方法可以与在脊形波导的端部和芯片边缘之间的窗口小面(118',118“)的制造集成,从而防止来自芯片边缘的意外反射。
    • 4. 发明申请
    • SEMICONDUCTOR OPTICAL AMPLIFYING MEDIA WITH REDUCED SELF-FOCUSING
    • 具有减少自聚焦的半导体光学放大介质
    • WO1997001204A1
    • 1997-01-09
    • PCT/US1996010747
    • 1996-06-19
    • SDL, INC.
    • SDL, INC.LANG, Robert, J.OSINSKI, Julian, S.WELCH, David, F.
    • H01S03/19
    • H01S5/10H01S5/0618H01S5/1057H01S5/20H01S5/50
    • A semiconductor light amplifying medium (11; 23) has reduced self-focusing and optical filamentation for providing higher power coherent outputs in broad-area laser and amplifier devices (Figs. 1 and 2). In one embodiment, a longitudinally inhomogeneous active region (13; 25) has alternating segments of first gain portions (15; 27) and second compensating portions (17; 29). The compensating portions have a negative self-focusing parameter [ DIFFERENTIAL n/ DIFFERENTIAL P] (Figs. 3 and 10) and may be light absorbing (negative gain) regions with negative antiguiding factor alpha (Figs. 4A-4C and 5) or light amplifying (positive gain) regions with positive antiguiding factor alpha (Figs. 6A-6B and 7A-7B). The alpha -parameter is defined as the ratio of refractive index change per change in gain, as a function of carrier density. In a second embodiment, the medium may have longitudinally varying peak filament period [Kpk] so that filaments beginning to form in one portion of the active region are subsequently dispersed in a succeeding portion, slowing filament growth. In addition to self-focusing compensation, media with a lower alpha -parameter are provided by increasing the barrier height in quantum well active regions (Figs. 8A-8B), straining (Fig. 9) or p-doping the active region, or a combination of these methods.
    • 半导体光放大介质(11; 23)具有减少的自聚焦和光纤丝化,用于在广域激光和放大器装置中提供更高功率的相干输出(图1和图2)。 在一个实施例中,纵向非均匀有源区(13; 25)具有第一增益部分(15; 27)和第二补偿部分(17; 29)的交替段。 补偿部分具有负的自聚焦参数[差分n /差分P](图3和图10),并且可以是具有负抗原因子α(图4A-4C和5)或光的吸光(负增益)区域 具有正抗原因子α的放大(正增益)区域(图6A-6B和7A-7B)。 α参数定义为每增益变化的折射率变化率,作为载流子密度的函数。 在第二个实施方案中,介质可以具有纵向变化的峰长丝周期[Kpk],使得开始在有源区域的一部分中形成的长丝随后分散在随后的部分中,从而减慢长丝生长。 除了自聚焦补偿之外,通过增加量子阱活性区域(图8A-8B)中的势垒高度,应变(图9)或p掺杂有源区域来提供具有较低α参数的介质,或 这些方法的组合。
    • 10. 发明申请
    • SEMICONDUCTOR DIODE LASER, IN PARTICULAR A LASER AMPLIFIER, AND METHOD OF MANUFACTURING THIS LASER
    • 半导体二极管激光器,特别是激光放大器及其制造方法
    • WO1997017750A1
    • 1997-05-15
    • PCT/IB1996001152
    • 1996-10-25
    • PHILIPS ELECTRONICS N.V.PHILIPS NORDEN AB
    • PHILIPS ELECTRONICS N.V.PHILIPS NORDEN ABTIEMEIJER, Lukas, FrederikBINSMA, Johannes, Jordanus, MariaTHIJS, Petrus, Johannes, Adrianus
    • H01S03/19
    • H01S5/10H01S5/1064H01S5/1085H01S5/50
    • The invention relates to a III-V laser (amplifier) with an active region (4A) which encloses a small angle with the end faces (50, 51), is separated therefrom by a preferably current-blocking cladding layer (5) and has a tapering end (40) of which a first side face (42) coincides with a side face (42) of the remainder of the strip-shaped active region (4A), while a second side face (43) thereof encloses an acute angle with the perpendicular to the end faces (50, 51). Such a laser has an amplification ripple, which is undesirable. In a laser according to the invention, the second side face (43) of the tapering portion (40) encloses an angle with the perpendicular to the end face (50, 51) which lies between 0 and 30 DEG , preferably between 0 and 10 DEG , and which is preferably approximately 0 DEG . The laser according to the invention has a particularly low reflection, as a result of which said amplification ripple is absent or at least very small. No differences in growing processes against said side faces occur since both the first and the second side faces (42, 43) of the active region (4A) are mutually substantially parallel. Accordingly, the laser is preferably of the buried hetero type. In that case, the growth around the active region (4A) is very homogeneous, which benefits the yield and quality of the lasers. The laser is preferably constructed as an amplifier, for which purpose the end faces (50, 51) are provided with an anti-reflection layer. The invention, finally, also relates to a method by which the desired laser is obtained in a simple manner.
    • 本发明涉及具有与端面(50,51)成小角度的有源区域(4A)的III-V激光器(放大器),其通过优选的阻流覆层(5)与其隔开,并具有 一个锥形端部(40),其第一侧面(42)与条状有源区域(4A)的其余部分的侧面(42)重合,而其第二侧面(43)包围锐角 垂直于端面(50,51)。 这种激光器具有放大纹波,这是不期望的。 在根据本发明的激光器中,锥形部分(40)的第二侧面(43)与垂直于端面(50,51)的角度包围在0和30度之间,优选在0和10之间 DEG,优选为约0℃。 根据本发明的激光器具有特别低的反射,其结果是所述放大纹波不存在或至少非常小。 由于活性区域(4A)的第一和第二侧面(42,43)彼此基本平行,因此不会发生生长过程与所述侧面的差异。 因此,激光器优选为埋入异种型。 在这种情况下,活性区域(4A)周围的生长是非常均匀的,这有利于激光器的产量和质量。 激光器优选地构造为放大器,为此目的,端面(50,51)设置有抗反射层。 本发明最终还涉及以简单的方式获得所需激光的方法。