Electrical and Optical Output Characteristics of InP/InGaAsP pnpn Structures Grown via LPE

W. Buchwald, Jian H. Zhao, Long D. Zhu
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Abstract

Gated p(1nP)-n(InP)-p(1nGaAsF’)-n(1nP) struchires have been fabricated via LPE. These devices are shown to have gate controlled, thyristor like, DC switching characteristics as well as gate controlled optical output at 940nm and 1280nm. The switching characteristics of these devices are also reported. Introduction The fabrication of PNPN devices from III-V compounds has recently received much interest due to the possibility of using these devices not only as optoelectronic power control elements [14], but also for applications such as dynamic memories [ 5 ] , two and three terminal optoelectronic switches [6,7]. optical amplifiers [SI and negative differentialresistancelasers,(NDRLaser) 191. Todate,researchinthis typeofsmcturehasbeencenteredontheGaAs/ AlGaAs matenal system, however, due to interest in optoelectronic devices operating at 1.3 and 1 . 5 5 ~ , the I@/ InGaAsP system is also receiving interest r8.101. At present, with respect to the InPDnGaAsP system, only two terminal devices have been successfully fabricated. This work presents the successful fabrication of an InPflnGaAsP based, three terminal pnpn optothynstor. The device presented here combines a double heterosmcture (DH) laser structure with a conventional thyristor into a single device. Negative differential resistance switching, with a maximum gate controlled breakover voltage of approximately 8V, is reported. An increase in the spontaneous emission of light at both 1.3 and 0 . 9 3 ~ is observed upon device switching from the high impedance OFF state to the low impedance ON state, suggesting the possibility of laser output when the device is fabricated into a suitable laser cavity. Measmments of the dynamic switching reveal device tum-on to be composed of a delay time followed by a more rapid (20011s) switching to the low impedance state. The switching delay time was also found to decrease with an increase in the gate trigger current. An anmalous feature of decrease in optical output as a function of device switching at high gate current is also reported. Device Fabrication Figure 1 shows the device smctme used for this work. The substrate was doped with Sn while the liquid phaseepitaxy (LPE) layernandp-typedopantswereTeandZnrespectively. TheInGaAsPlayerwas grown to produce spontaneous emission of light at a wavelength of 13OOnm. SIMS measurements were used to calibrate the layer t 500pm* I--54OplTl-i 9 o o p m F 920pm Cathode 58Ovmn InP 3.0pm 3.0x1017cm-3
LPE生长的InP/InGaAsP pnpn结构的光电输出特性
通过LPE制备了门控p(1nP)-n(InP)-p(1nGaAsF ')-n(1nP)结构。这些器件显示出具有门控、晶闸管式直流开关特性以及在940nm和1280nm的门控光输出。本文还报道了这些器件的开关特性。由III-V化合物制备PNPN器件最近受到了广泛关注,因为这些器件不仅可以用作光电功率控制元件[14],还可以用于动态存储器[5]、二端和三端光电开关[6,7]等应用。光学放大器[SI和负微分电阻弹性器],(NDRLaser), 2011。然而,由于对工作在1.3和1的光电器件的兴趣,目前对这种类型结构的研究已经集中在gaas / AlGaAs材料系统上。5 . 5 ~ 5, I@/ InGaAsP系统也收到利息8.101。目前,对于InPDnGaAsP系统,仅成功制作了两个终端器件。本文成功地制作了一种基于InPflnGaAsP的三端pnpn光晶闸管。该器件将双异质结构(DH)激光结构与传统晶闸管结合为一个器件。负差分电阻开关,最大门控开关电压约8V,报道。在1.3和0时自发光发射增加。当器件从高阻抗OFF状态切换到低阻抗ON状态时,观察到9 3 ~,表明当器件被制造到合适的激光腔中时,有可能输出激光。动态开关的测量表明,器件的导通是由一个延迟时间组成的,随后是一个更快速的(20011秒)切换到低阻抗状态。开关延迟时间也随着栅极触发电流的增大而减小。本文还报道了在高栅极电流下器件切换时光输出减少的反常特征。图1显示了用于此工作的设备smctme。衬底掺杂锡,液相外延(LPE)层和p型掺杂分别掺杂锡和锌。该ingaasplayer生长产生自发发射光的波长为13oom。使用SIMS测量来校准层至500pm* I- 54OplTl-i 9至920pm阴极58Ovmn InP 3.0pm 3 × 1017cm-3
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