InGaAs/InP P-I (MQW)-N表面法向电吸收调制器在气源MBE生长的1.55/spl mu/m应用中表现出优于8:1的对比度

R. N. Pathak, K. Goossen, J. E. Cunningham, W. Jan
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引用次数: 2

摘要

传统的双向光纤系统采用两个激光器、两根光纤和两个探测器,由于元件成本高,不适合光纤在家庭通信中的应用。最近,一种用于中程应用的系统已经被证明,该系统成功地使用了表面法向p-i (MQW)-n调制器将下游光转换为来自用户终端的上游数据[1]。在这种系统中使用这些设备的要求是它们的对比度为10:1。在860nm的器件中已经实现了这样的对比度,但是在13001550nm的表面法向器件中已经报道了更低的对比度,对应于光纤的低损耗-低色散窗口,用于长距离通信应用。据我们所知,在该波长范围内,表面法向器件的最高对比度为2.6:1 (4.1 dB),其中包含150周期InGaAs-InP MQW[2]的器件的反向偏置为40 V,而非对称法布里佩罗(ASFP)调制器的对比度为3 dB,尽管驱动电压较低为5 V[3]。对比度较低的原因是该材料体系的吸收系数较低(仅为AIGaAs-GaAs材料体系的40%左右)。该器件结构采用气源MBE在n型Inp (Sn掺杂)晶圆上生长,以ASH3和PH3为V族源气体,生长温度为500℃。该结构由1.5 pm的n型Inp包覆层(Si掺杂至3 × 1018 cm-3)和由200,10 nm &.53%组成的本质区组成。47As阱晶格与8nm的InP势垒匹配,然后是1 pm厚的p型InP包覆层(Be掺杂到3 × lo** cm-3)。后生长处理包括台面蚀刻和p和n型接触金属化。然后在晶圆背面涂上Si0抗反射涂层。由于InP衬底在感兴趣的波长处是透明的,因此没有衬底变薄。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
InGaAs/InP P-I (MQW)-N Surface Normal Electroabsorption Modulators Exhibiting Better Than 8:1 Contrast Ratio For 1.55/spl mu/m Applications Grown By Gas Source MBE
Traditional bi-directional optical fiber systems utilizing two lasers, two fibers and two detectors are unattractive for fiber to the home communication applications due to the high component cost. A system for medium range applications has recently been demonstrated in which a surface normal p-i (MQW)-n modulator was successllly used to convert downstream light into upstream data fiom the subscriber terminal [l]. A requirement for these devices to be used in such a system is that they exhibit a contrast ratio on the order of 10: 1. Such contrast ratios have been achieved in devices operating at 860 nm but much lower contrast ratios have been reported for surface normal devices operating at 13001550 nm, corresponding to the low loss-low dispersion window of optical fibers, for long haul communication applications. The highest contrast ratio reported for surface normal devices in this wavelength regime to the best of our knowledge is 2.6: 1 (4.1 dB) at an applied reverse bias of 40 V for a device incorporating a 150 period InGaAs-InP MQW [2] and 3 dB for an Asymmetric Fabry Perot (ASFP) modulator albeit at a low drive voltage of 5 V [3]. The reason for the low contrast ratios is the low value of the absorption coefficient exhibited by this material system (only about 40% of that exhibited by the AIGaAs-GaAs material system). The device structure was grown on top of an n type Inp (Sn doped) wafer by Gas Source MBE using ASH3 and PH3 as the Group V source gases at a growth temperature of 500 C. The structure consisted of a 1.5 pm n-type InP clad layer (Si doped to 3 x 1018 cm-3) followed by an intrinsic region composed of 200, 10 nm &.53%.47As wells lattice matched to 8 nm InP barriers, followed by a 1 pm thick p-type InP clad layer (Be doped to 3 x lo** cm-3). Post growth processing consisted of a mesa etch and p and n type contact metallizations. An Si0 anti reflection coating was then applied to the backside of the wafer. Since the InP substrate is transparent at the wavelength of interest no substrate thinning was performed.
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