Excess low frequency noise/I-V studies in p-on-n MBE LWIR Hg1-xCdxTe detectors

Excess low frequency noise is investigated for the first time in infrared MBE grown LWIR Hg1-xCdxTe double layer planar heterostructure (DLPH) detectors grown on lattice matched substrates. LWIR detectors having R(o)A(opt) values at 40K in the 10(1)-10(7) Omega-cm(2) range have been characterized as a function of temperature between 120 and 20K. Detectors with R(o)A(opt) greater than or equal to 10(3) Omega-cm(2) at 40K have theoretical diffusion limited performance down to 78K and detectors with R(o)A(opt) greater than or equal to 10(5) Omega-cm(2) at 40K are within a factor of two of theoretical diffusion limited performance for T > 65K. Activation energies extracted from noise (V-d = -100 mV) and dark current (V-d = -100 mV) vs temperature measurements were detector dependent. The activation energy for detectors with R(o)A(opt) approximate to 10(6) Omega-cm(2) at 40K is similar to 0.90*E-g to 0.99*E-g. The noise measured between 78 and 105K in the intermediate performance (R(o)A(opt) similar to 10(3)-10(4) Omega-cm(2) at 40K) detectors are higher than the noise measured in the higher performance (R(o)A(opt) similar to 10(5)-10(7) Omega-cm(2)) detectors. In addition, the excess low frequency noise and the dark current at -100 mV in the intermediate and poor (R(o)A(opt) similar to 10(1) Omega-cm(2)) performance detectors are temperature independent. For each detector measured, the activation energy extracted from noise (V-d = -100 mV) vs temperature measurements is equal to the activation energy extracted from the total dark current (V-d = -100 mV) vs temperature measurements. For different dark current mechanisms, the excess low frequency noise varies with temperature and also with area within statistical accuracy in the same manner as the total dark current through the detector. At 78K, the Tobin(14) expression holds in the general sense for equal area detectors dominated by different current mechanisms and also for detectors with a wide range of implant dimensions (A(imp) = 3.85 x 10(-7) cm(2) to A(imp) = 6.25 x 10(-4)cm(2)). Following measurements, the detectors were stripped of the passivation and overlaying metal layers and dressed by a defect etch to reveal defects in each detector. A correlation among noise, leakage current and defect type has been determined for each detector.