Dark Current Transport and Avalanche Mechanism in HgCdTe Electron-Avalanche Photodiodes

HgCdTe electron avalanche photodiodes (e-APDs) have been widely used for low-flux and high-speed application. To better understand the dark current transport and electron-avalanche mechanism of the devices and optimize the structures, we performed accurate numerical simulations of the current-voltage characteristics and multiplication factor in planar homojunction (p-i-n) HgCdTe APDs. Based on the Okuto-Crowell avalanche model, an efficient physical model has been obtained by concerning the major generation-recombination processes, such as trap-assisted tunneling and band-to-band tunneling (BBT) recombination. Simulated current-voltage characteristics were in good agreement with available data in the literature, which demonstrates the validity of the proposed model. The origins of dark current in high reverse voltages are jointly dominated by BBT and the avalanche mechanism. It is proved to be effective for reducing BBT by improving the uniformity of the electric field distribution across the junction. The electric performance of p-i-n e-APD can be improved by optimizing the APD structure, such as eliminating the sharp corners of junctions, light doping, and the appropriate thickness in multiplication region. Our works provide a good deal of insight into the fundamental carrier transport processes involved in HgCdTe e-APDs.

[1]  J. Rothman,et al.  High performance characteristics in pin MW HgCdTe e-APDs , 2007, SPIE Defense + Commercial Sensing.

[2]  C. Grein,et al.  Avalanche Mechanism in p+-n−-n+ and p+-n Mid-Wavelength Infrared Hg1−xCdxTe Diodes on Si Substrates , 2008 .

[3]  V. Gopal,et al.  Modelling of illuminated current–voltage characteristics to evaluate leakage currents in long wavelength infrared mercury cadmium telluride photovoltaic detectors , 2014 .

[4]  M. Kinch,et al.  The HgCdTe electron avalanche photodiode , 2006, 2006 Digest of the LEOS Summer Topical Meetings.

[5]  Gérard Destefanis,et al.  Gain and Dark Current Characteristics of Planar HgCdTe Avalanche Photo Diodes , 2007 .

[6]  Modeling of Dark Current in HgCdTe Infrared Detectors , 2013, Journal of Electronic Materials.

[7]  Xiaoshuang Chen,et al.  Polarity inversion and coupling of laser beam induced current in As-doped long-wavelength HgCdTe infrared detector pixel arrays: Experiment and simulation , 2012 .

[8]  Donald N. B. Hall,et al.  HgCdTe APD-based linear-mode photon counting components and ladar receivers , 2011, Defense + Commercial Sensing.

[9]  Weida Hu,et al.  128 × 128 long-wavelength/mid-wavelength two-color HgCdTe infrared focal plane array detector with ultralow spectral cross talk. , 2014, Optics letters.

[10]  W. Lu,et al.  Improved performance of HgCdTe infrared detector focal plane arrays by modulating light field based on photonic crystal structure , 2014 .

[11]  Xiaoli Ji,et al.  Deep-level traps induced dark currents in extended wavelength InxGa1−xAs/InP photodetector , 2013 .

[12]  S. Sivananthan,et al.  A model for dark current and multiplication in HgCdTe avalanche photodiodes , 2000 .

[13]  T. Jiang,et al.  Novel signal inversion of laser beam induced current for femtosecond-laser-drilling-induced junction on vacancy-doped p-type HgCdTe , 2014 .

[14]  J. Rothman,et al.  HgCdTe APD- Focal Plane Array development at DEFIR for low flux and photon-counting applications. , 2009 .

[15]  W. Pusz,et al.  Modeling of HOT (111) HgCdTe MWIR detector for fast response operation , 2014 .

[16]  L. He,et al.  Photon trapping photodiode design in HgCdTe mid-wavelength infrared focal plane array detectors , 2014 .

[17]  V. Srivastav,et al.  HgCdTe avalanche photodiodes: A review , 2011 .

[18]  Weida Hu,et al.  Dependence of Ion-Implant-Induced LBIC Novel Characteristic on Excitation Intensity for Long-Wavelength HgCdTe-Based Photovoltaic Infrared Detector Pixel Arrays , 2013, IEEE Journal of Selected Topics in Quantum Electronics.

[19]  J. Rothman,et al.  Electrical modeling of InSb PiN photodiode for avalanche operation , 2013 .

[20]  Jean-Paul Chamonal,et al.  Impulse Response Time Measurements in Hg0.7Cd0.3Te MWIR Avalanche Photodiodes , 2008 .

[21]  Y. Reibel,et al.  Performance of Mid-Wave Infrared HgCdTe e-Avalanche Photodiodes , 2012, Journal of Electronic Materials.

[22]  Enrico Bellotti,et al.  Numerical simulation of crosstalk in reduced pitch HgCdTe photon-trapping structure pixel arrays. , 2013, Optics express.

[23]  P. Norton HgCdTe Infrared Detectors , 2002 .

[24]  Piotr Martyniuk,et al.  Modelling of MWIR HgCdTe complementary barrier HOT detector , 2013 .

[25]  Jinxue Wang,et al.  Advances in HgCdTe APDs and LADAR receivers , 2010, Defense + Commercial Sensing.

[26]  Silviu Velicu,et al.  Hg1-x CdxTe mid-wavelength infrared (MWIR) avalanche photodiode (APD) grown on Si substrate , 2007, SPIE Organic Photonics + Electronics.

[27]  H. Kocer,et al.  Numerical analysis of long wavelength infrared HgCdTe photodiodes , 2012 .

[28]  Weida Hu,et al.  Laser beam induced current microscopy and photocurrent mapping for junction characterization of infrared photodetectors , 2015 .

[29]  A. Kerlain,et al.  Short-Wave Infrared HgCdTe Avalanche Photodiodes , 2012, Journal of Electronic Materials.

[30]  Jarek Antoszewski,et al.  Performance Modeling of Bandgap Engineered HgCdTe-Based nBn Infrared Detectors , 2014, IEEE Transactions on Electron Devices.

[31]  Bo Zhang,et al.  Temperature-sensitive junction transformations for mid-wavelength HgCdTe photovoltaic infrared detector arrays by laser beam induced current microscope , 2014 .

[32]  Jean-Paul Chamonal,et al.  Study of the Transit-Time Limitations of the Impulse Response in Mid-Wave Infrared HgCdTe Avalanche Photodiodes , 2009 .

[33]  John Marciniec,et al.  Characterization of HgCdTe MWIR Back-Illuminated Electron-Initiated Avalanche Photodiodes , 2008 .