Long-wavelength InGaAsP/InP multiquantum well distributed feedback and distributed Bragg reflector lasers grown by chemical beam epitaxy

Long-wavelength InGaAsP/InP multiquantum well distributed feedback and distributed Bragg reflector lasers grown by chemical beam epitaxy
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DOI:
10.1109/3.299459
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发表时间:
1994-06
影响因子:
2.5
通讯作者:
W. Tsang;Ming C. Wu;Young-Kai Chen;F. Choa;R. Logan;S. Chu;A. Sergent;P. Magill;K. Reichmann;C. Burrus
W. Tsang;Ming C. Wu;Young-Kai Chen;F. Choa;R. Logan;S. Chu;A. Sergent;P. Magill;K. Reichmann;C. Burrus
中科院分区:
工程技术3区
文献类型:
--
作者:
W. Tsang;Ming C. Wu;Young-Kai Chen;F. Choa;R. Logan;S. Chu;A. Sergent;P. Magill;K. Reichmann;C. Burrus

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利用化学束外延(CBE)成功制备了长波长InGaAsP低阈值电流指数耦合和增益耦合DFB激光器。对于指数耦合DFB激光器,埋地异质结构6 qw DFB激光器(250 /spl mu/m长,劈裂)工作功率为1.55 /spl mu/m,连续波阈值电流为10-15 mA,斜率效率高达0.35 mW/mA(两个方面)。侧模抑制比(SMSR)高达49 dB。激光器在相同的范围内工作,即使在高温(70/spl度/C检查)。对于增益耦合的DFB激光器,增益耦合是通过使用InGaAsP四元光栅或量子阱光栅来吸收DFB发射来实现的。特别是量子阱光栅的使用,极大地促进了光栅的可再生再生(无缺陷)和耦合系数的控制。连续波阈值电流仅在250-/spl mu/m时为10-15 mA, 250-/spl mu/m和500-/spl mu/m时为13-18 mA。坡度效率很高,/spl sim/0.4 mW/mA(两个方面)。在整个电流范围内,SMSR高达52 dB,保持在相同的DFB模式,SMSR保持在/spl sim/50 dB。线宽/倍频/功率产品为1.9-4.0,最小线宽为1.8-2.2 MHz。在2.5 Gb/s调制下,没有检测到啁啾。与指数耦合DFB激光器不同的是,当偏置高于阈值时,模式分割事件会缓慢减少,而当偏置接近阈值(/spl gsim/0.95 I/sub - th/)时,模式分割事件会急剧关闭。在230 km的放大光纤系统中,以1.7 Gb/s的速度使用这些激光器作为源,在10/sup -11/ BER的传输实验中测量到非常小的色散损失为1.0 dB。在这些增益耦合DFB激光器中没有观察到自脉动。这些增益耦合DFB激光器实现了4ghz的增益切换,光调制深度为100%,FWHM脉冲宽度为23 ps。峰值功率为/spl sim/72 mW,频宽为0.14 nm。我们还利用CBE技术制备了InGaAs/InGaAsP多量子阱DBR激光器。利用均匀的厚度增长和适当的弱光栅和长光栅设计,获得了创纪录的58.5 dB的高SMSR。>
We demonstrated the successful operation of long-wavelength InGaAsP low threshold-current index-coupled and gain-coupled DFB lasers grown by chemical beam epitaxy (CBE). For index-coupled DFB lasers, buried-heterostructure six-QW DFB lasers (250 /spl mu/m long and as-cleaved) operated at 1.55 /spl mu/m with CW threshold currents 10-15 mA and slope efficiencies up to 0.35 mW/mA (both facets). A side-mode suppression ratio (SMSR) as high as 49 dB was obtained. The lasers operated in the same range even at high temperatures (70/spl deg/C checked). For gain-coupled DFB lasers, gain-coupling is accomplished by using a InGaAsP quaternary grating or quantum-well grating that absorbs the DFB emission. The use of a quantum-well grating, in particular, greatly facilitates the reproducible regrowth (defect-free) over grating and the control of the coupling coefficient. CW threshold currents mere in the range of 10-15 mA for 250-/spl mu/m and 13-18 mA for 250-/spl mu/m and 500-/spl mu/m cavities, respectively. Slope efficiencies were high, /spl sim/0.4 mW/mA (both facets). SMSR was as high as 52 dB and remained in the same DFB mode with SMSR staying /spl sim/50 dB throughout the entire current range. Linewidth/spl times/power products of 1.9-4.0 mere measured with minimum linewidths of 1.8-2.2 MHz. No detectable chirp was measured under 2.5 Gb/s modulation. Unlike index-coupled DFB lasers in which mode partition events decrease slowly even when biased above threshold, these lasers have mode partition events shut off sharply as bias approaches threshold (/spl gsim/0.95 I/sub th/). A very small dispersion penalty of 1.0 dB was measured at 10/sup -11/ BER in transmission experiments using these lasers as sources at 1.7 Gb/s over an amplified fiber system of 230 km. No self-pulsation was observed in these gain-coupled DFB lasers. Gain-switching at 4 GHz with a 100% optical modulation depth and a FWHM pulse width of 23 ps was achieved with these gain-coupled DFB lasers. The peak power was /spl sim/72 mW and the FWHM bandwidth was 0.14 nm. We also fabricated InGaAs/InGaAsP multiquantum-well DBR lasers by CBE. Taking advantage of uniform thickness growth and proper design of weak and long gratings, a record high SMSR of 58.5 dB was obtained. >