Spatially resolved characterization of HgCdTe materials and devices by scanning laser microscopy

Spatially resolved characterization of HgCdTe materials and p-n junction diodes using scanning laser microscopy is reviewed. Several techniques that yield spatial maps of electrical inhomogeneities in HgCdTe material and non-uniformities in various performance parameters of p-n junctions fabricated using these materials have been developed. Many of the techniques are non-destructive, or can be made such with minor changes in sample preparation, and are scalable to large full wafers. A high-resolution and non-destructive technique called 'laser beam induced current (LBIC)' has been developed for spatial mapping of electrically active regions in HgCdTe. When applied to unprocessed HgCdTe material, LBIC images represent spatial distributions of electrically active defects including inclusions, strain, damage, precipitates, stacking faults, twin boundaries, dislocation clusters, bandgap and doping variations. Device structures such as p-n junctions are special cases of electrically active regions, therefore the LBIC technique lends itself to a non-destructive study of p-n junction arrays without requiring any direct electrical contact to the individual elements of the array. The remote contacting, especially using pressure contacts, makes the application of the LBIC technique non-destructive, allowing testing at various stages of device processing to identify particular processing procedures that need optimization. LBIC has also been used to spatially map electrical non-uniformities at the HgCdTe surface near its interface with an insulating passivation layer. Besides LBIC imaging, scanning laser microscopy has been used for several other applications. For HgCdTe p-n junctions, applications include photoresponse mapping (uniformity, active area and diffusion length determination, contact bonding effects), spatially resolved light-induced degradation, and avalanche photodiode properties (ionization coefficients, localized breakdown). A key technique currently in development is the non-contact diode R0A determination based on trapping mode photoconductivity. Examples of scanning laser microscopy on HgCdTe materials are infrared transmission mapping (thickness and bandgap variations), photoluminescence mapping, and minority carrier lifetime mapping (distribution of recombination centres).

[1]  J. Bajaj,et al.  Laser beam induced current imaging of surface nonuniformity at the HgCdTe/ZnS interface , 1988 .

[2]  W. Tennant,et al.  Observation of charge‐separating defects in HgCdTe using remote contact electron beam induced current , 1988 .

[3]  Donald E. Cooper,et al.  Spectroscopic Techniques For The Analysis Of CdTe Substrates Used For The Growth Of HgCdTe , 1989, Defense, Security, and Sensing.

[4]  J. Bajaj,et al.  Remote contact LBIC imaging of defects in semiconductors , 1990 .

[5]  J. Bajaj,et al.  Minority carrier lifetime and diffusion length in HgTe/CdTe superlattices by molecular beam epitaxy , 1992 .

[6]  E. Molva,et al.  Donors and acceptors in tellurium compounds; The problem of doping and self-compensation , 1985 .

[8]  C. J. Miner,et al.  A spatially resolved spectrally resolved photoluminescence mapping system , 1990 .

[9]  J. Wallmark A New Semiconductor Photocell Using Lateral Photoeffect , 1957, Proceedings of the IRE.

[10]  E. Weiss,et al.  Degradation mechanisms of gamma irradiated LWIR HgCdTe photovoltaic detectors , 1990 .

[11]  J. Bajaj,et al.  Spatial origin of various PL lines in CdTe at 77 K , 1988 .

[12]  J. Bajaj,et al.  Variable-area diode data analysis of surface and bulk effects in MWIR HgCdTe/CdTe/sapphire photodetectors , 1993 .

[13]  S. Shin,et al.  Effect of the dislocation density on minority‐carrier lifetime in molecular beam epitaxial HgCdTe , 1991 .

[14]  A. Syllaios,et al.  Minority carrier lifetime in mercury cadmium telluride , 1993 .

[15]  L. O. Bubulac,et al.  Spatial mapping of electrically active defects in HgCdTe using laser beam‐induced current , 1987 .