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Negative response of HgCdTe photodiode induced by nanosecond laser pulse

机译:纳秒激光脉冲诱导的HGCDTE光电二极管的负响应

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Photodetectors' behavior and mechanism of transient response are still not understood very well, especially under high photon injection. Most of the researches on this topic were carried out with ultra-short laser pulse, whose pulse width ranged from femtosecond scale to picosecond scale. However, in many applications the durations of incident light are in nanosecond order and the light intensities are strong. To investigate the transient response characteristics and mechanisms of narrow-bandgap photovoltaic detectors under short laser irradiation, we performed an experiment on HgCdTe photodiodes. The n~+-on-p type HgCdTe photodiodes in the experiment were designed to work in spectrum from 1.0μm to 3.0μm, with conditions of zero bias and room temperature. They were exposed to in-band short laser pulses with dwell time of 20 nanosecond. When the intensity of incident laser beam rose to 0.1J/cm~2 order, the photodiodes' response characteristics turned to be bipolar from unipolar. A much longer negative response with duration of about 10μs to 100μs followed the positive light response. The amplitude of the negative response increased with the laser intensity, while the dwell time of positive response decreased with the laser intensity. Considering the response characteristics and the device structure, it is proposed that the negative response was caused by space charge effect at the electrodes. Under intense laser irradiation, a temperature gradient formed in the HgCdTe material. Due to the temperature gradient, the majority carriers diffused away from upper surface and left space charge at the electrodes. Then negative response voltage could be measured in the external circuit. With higher incident laser intensity, the degree of the space charge effect would become higher, and then the negative response would come earlier and show larger amplitude.
机译:光电探测器的行为和机制仍然没有很好地理解,特别是在高光子注射下。大多数关于该主题的研究是用超短的激光脉冲进行的,其脉冲宽度从飞秒缩放到PicoSecond级。然而,在许多应用中,入射光的持续时间是纳秒顺序,光强度强劲。为了研究短激光照射下窄带隙光伏探测器的瞬态响应特性和机制,我们对HGCDTE光电二极管进行了实验。实验中的N〜+ -P-P型HGCDTE光电二极管设计成在1.0μm至3.0μm的光谱中,条件为零偏置和室温。它们暴露于带内的短激光脉冲,停留时间为20纳秒。当入射激光束强度升至0.1J / cm〜2的顺序时,光电二极管的响应特性转向单极的双极性。持续时间长度为约10μs至100μs的更长的负响应,然后是正光响应。负响应的幅度随着激光强度而增加,而正反应的停留时间随着激光强度而降低。考虑到响应特性和器件结构,提出了负响应是由电极的空间电荷效应引起的。在激光照射下,在HGCDTE材料中形成的温度梯度。由于温度梯度,多个载体扩散远离上表面和电极的左空间电荷。然后可以在外部电路中测量负响应电压。具有较高的入射激光强度,空间电荷效应的程度会变得更高,然后否则响应将提前呈现较大幅度。

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