Lee S C, Krishna S, Brueck S R J
Center for High Technology Materials and Department of Electrical and Computer Engineering, University of New Mexico, 1313 Goddard SE, Albuquerque, NM 87106, USA.
Opt Express. 2009 Dec 7;17(25):23160-8. doi: 10.1364/OE.17.023160.
Up to a thirty-fold detectivity enhancement is achieved for an InAs quantum dot infrared photodetector (QDIP) by the excitation of surface plasma waves (SPWs) using a metal photonic crystal (MPC) integrated on top of the detector absorption region. The MPC is a 100 nm-thick gold film perforated with a 3.6 microm period square array of circular holes. A bare QDIP shows a bias-tunable broadband response from approximately 6 to 10 microm associated with the quantum confined Stark (QCS) effect. On the other hand, an MPC-integrated QDIP exhibits a dominant peak at 11.3 microm with a approximately 1 microm full width at half maximum and the highly enhanced detectivity at the bias polarity optimized for long wavelength. This is very different from the photoresponse of the bare QDIP but fully consistent with the direct coupling of the QDs in the detector absorption region to the SPWs excited at the MPC/detector interface by incident photons. The SPW resonance wavelength, lambda, for the smallest coupling wavevector of the array in the MPC is close to 11.3 microm. The response also shows other SPW-coupled peaks: a significant peak at 8.1 microm (approximately lambda/radical2) and noticeable peaks at 5.8 microm (approximately lambda/2) and 5.4 microm (approximately lambda/ radical5) which correspond to higher-order coupling wavevectors. For the opposite bias, the MPC-integrated QDIP shows the highest response at 8.1 microm, providing a dramatic voltage tunability that is associated with QCS effect. SPWs propagate with TM (x, z) polarization along the MPC/detector interface. The enhanced detectivity is explained by these characteristics which increase both the effective absorption cross section with propagation and the interaction strength with TM polarization in the coupling to the QDs. Simulations show good qualitative agreement with the observed spectral behavior.
通过在探测器吸收区域顶部集成金属光子晶体(MPC)来激发表面等离子体波(SPW),砷化铟量子点红外探测器(QDIP)的探测率提高了30倍。该MPC是一层100纳米厚的金膜,上面有一个周期为3.6微米的圆形孔方形阵列。裸QDIP表现出与量子限制斯塔克(QCS)效应相关的约6至10微米的偏置可调宽带响应。另一方面,集成MPC的QDIP在11.3微米处呈现出一个主峰,半高宽约为1微米,并且在针对长波长优化的偏置极性下探测率大幅提高。这与裸QDIP的光响应有很大不同,但与探测器吸收区域中的量子点与入射光子在MPC/探测器界面激发的SPW的直接耦合完全一致。MPC中阵列最小耦合波矢的SPW共振波长λ接近11.3微米。该响应还显示出其他SPW耦合峰:8.1微米处有一个显著峰(约为λ/√2),5.8微米(约为λ/2)和5.4微米(约为λ/√5)处有明显峰,它们对应于高阶耦合波矢。对于相反的偏置,集成MPC的QDIP在8.1微米处显示出最高响应,提供了与QCS效应相关的显著电压可调性。SPW以TM(x,z)极化沿MPC/探测器界面传播。这些特性增加了传播时的有效吸收截面以及与TM极化在与量子点耦合时的相互作用强度,从而解释了探测率的提高。模拟结果与观察到的光谱行为在定性上吻合良好。