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首页> 外文期刊>Journal of Lightwave Technology >Bandwidth enhancement for p-end-illuminated InP/InGaAs/InP p-i-n photodiodes by utilizing symmetrical doping profiles
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Bandwidth enhancement for p-end-illuminated InP/InGaAs/InP p-i-n photodiodes by utilizing symmetrical doping profiles

机译:通过使用对称掺杂分布来增强p端照明的InP / InGaAs / InP p-i-n光电二极管的带宽

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This paper shows that the bandwidth of a p-end-illuminated planar InP-InGaAs-InP heterojunction p-i-n photodiode can be promoted by using a rather symmetrical doping profile that is produced through diffusion depth control. Caused by extra-depleted InP region in the end of p-InP, the device with symmetrical doping profile has additional series capacitance and thus has a smaller total capacitance than conventional asymmetrical doping profile. Such devices with 0.3 /spl mu/m depleted InP cap region, together with 1 /spl mu/m depleted InGaAs absorption region and 0.3 /spl mu/m depleted InP buffer region, having the capacitance as small as those devices with 1.6 /spl mu/m depletion region, while have the carrier transit time as short as those devices with 1.3 /spl mu/m depletion region. Under appropriate bias condition, which is required for getting rid of the heterointerface effects, the symmetrical device as stated with 40 /spl mu/m junction diameter can have a 3 dB bandwidth exceeding 17 GHz without inductance optimization. For device with conventional asymmetrical doping profile, that is, the p-n junction locating at /spl sim/0.1 /spl mu/m deep in the InGaAs layer, only a bandwidth of about 15 GHz can be obtained. Due to the same thickness of InGaAs absorption layer, both devices have similar responsivity of /spl sim/0.8 A/W at -5 V at 1.3 /spl mu/m wavelength. However, the heterointerface exposed in the depletion region results in several detrimental effects in symmetrical devices, such as interface-generation current, which leads to slightly increased dark current, and barrier/traps for hole transport, which lead to inferior photoresponse at low biases.
机译:本文表明,通过使用通过扩散深度控制产生的相当对称的掺杂轮廓,可以提高p端照明的平面InP-InGaAs-InP异质结p-i-n光电二极管的带宽。由p-InP末端的InP区域过度耗尽导致,具有对称掺杂分布的器件具有额外的串联电容,因此总电容比传统的非对称掺杂分布小。具有0.3 / spl mu / m耗尽的InP帽区,具有1 / spl mu / m耗尽的InGaAs吸收区和0.3 / spl mu / m耗尽的InP缓冲区的器件,其电容与具有1.6 / spl mu / m的InP缓冲区的电容一样小。 μ/ m耗尽区,而载流子传输时间短于1.3 / splμ/ m耗尽区的器件。在消除异质界面效应所需的适当偏置条件下,具有40 / splμ/ m结直径的对称器件在没有电感优化的情况下可以具有超过17 GHz的3 dB带宽。对于具有常规非对称掺杂分布的器件,即,位于InGaAs层深/ spl sim / 0.1 / spl mu / m的p-n结,只能获得大约15 GHz的带宽。由于InGaAs吸收层的厚度相同,两个器件在1.3 V / splμm/ m波长下在-5 V时具有相似的/ spl sim / 0.8 A / W响应度。然而,暴露在耗尽区中的异质界面会在对称器件中产生多种不利影响,例如界面产生电流,会导致暗电流略有增加;空穴传输的势垒/陷阱会导致低偏压下的光响应变差。

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