Vertical cavity surface emitting lasers with 14GHz bandwidth

P. Brusenbach, T. Uchida, C. Parsons, M. Kim, W. Quinn, S. Swirhun
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引用次数: 1

Abstract

The possibility of high speed operation is one of the most attractive features of vertical cavity surface emitting lasers (VCSELs). This arises from the small size and high photon density of the cavity. However, while relaxation oscillations at frequencies as high as 70 GHz [l] have been reported, the highest measured modulation bandwidth is in the 5-8 GHz range [2]. The low bandwidth is attributed to large parasitics of the VCSEL and specifically to the high resistance of the p-type mirror. We have investigated small diameter VCSELs and have observed a maximum bandwidth of 14 GHz. In this study, gain-guided VCSELs from two wafers were used, nominally lasing at either 780 nm or 960 nm. The epitaxial structure consisted of a bottom Si-doped mirror, a cavity region, and a top C-doped mirror. The mirrors consisted of quarterwavelength layers of AIAs/A10.3Ga0.7As or AIAs/GaAs for the 780 nm and 960 nm lasers, respectively. The active region of the 780 nm VCSEL was bulk A10,15Ga0.85As while the active region of the 960 nm wafer had three GaAs/ln0,2Ga0.gAs quantum wells. The structures were grown by MBE on 3” diameter n-type GaAs substrates and fabricated by completely planar technology. Threshold currents were 4-6 mA for laser diameters of 6-10 pm and the cw peak powers exceeded 0.4 mW. Modulation experiments showed a very high frequency-square root of power coefficient D=10 GHz/mW1/2. The maximum bandwidth of 13.7 GHz was reached at 20OC (and 14.7 GHz at 7OC) at a current of 8 mA for the 780 nm laser with a cavity diameter of 6 pm. The cavity region of these lasers received both a broad area proton implant as well as a second deep implant centered at the active region to better define the cavity diameter. The 960 nm lasers received only the first broad area implant and their measured response of 10 GHz indicates the importance of minimizing lateral carrier diffusion. Fitting of the response curves yields a damping rate r of more than 10 GHz, indicating an intrinsic response fmax greater than 50 GHz. The S-parameter data can be fitted to high accuracy with a realistic equivalent circuit.
14GHz带宽垂直腔面发射激光器
高速运行的可能性是垂直腔面发射激光器(VCSELs)最吸引人的特点之一。这是由腔的小尺寸和高光子密度引起的。然而,虽然已经报道了频率高达70 GHz的弛豫振荡[1],但测量到的最高调制带宽在5-8 GHz范围内[2]。低带宽归因于VCSEL的大寄生,特别是p型反射镜的高电阻。我们已经研究了小直径的vcsel,并观察到最大带宽为14 GHz。在这项研究中,使用了来自两个晶圆的增益引导vcsel,名义上激光波长为780 nm或960 nm。外延结构由底部掺硅反射镜、空腔区和顶部掺c反射镜组成。反射镜由四分之一波长层的AIAs/ a10.3 ga0.7和AIAs/GaAs组成,分别用于780 nm和960 nm激光器。780 nm VCSEL的活性区为a10,15ga0.85 as,而960 nm晶圆的活性区为三个GaAs/ ln0,2ga0。气体量子井。采用MBE法在直径为3”的n型GaAs衬底上生长,并采用全平面工艺制备。激光直径为6 ~ 10 pm时,阈值电流为4 ~ 6 mA,连续波峰值功率超过0.4 mW。调制实验表明,频率非常高,功率系数D的平方根=10 GHz/ mw /2。780nm、腔径为6pm的激光器在8 mA电流下,在20℃时达到最大带宽13.7 GHz(7℃时达到最大带宽14.7 GHz)。这些激光器的腔区既接受了广域质子植入,也接受了以活性区域为中心的第二次深度植入,以更好地确定腔直径。960 nm激光器仅接受了第一次大面积植入,其测量响应为10 GHz,这表明最小化横向载流子扩散的重要性。响应曲线的拟合得到阻尼率r大于10 GHz,表明本征响应fmax大于50 GHz。通过实际的等效电路,可以对s参数数据进行高精度拟合。
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