Novel Type II superlattice design.

Schematic diagram of the M structure. The inserted AlSb layer forms a barrier for electrons in the conduction band and a double quantum well for holes in the valence band.

Type II InAs/GaSb superlattice was first introduced by the Nobel laureate L. Esaki in the 1970s and then proposed for infrared detection applications by Smith and Mailhiot in 1987. Since then, Type II Sb-based superlattice has evolved drastically with many variants for different purposes. We have developed a new superlattice design, called M-structure superlattice, which acquires the beneficial properties of the well established binary – binary antimonide based SL structures used in high performance infrared detectors. First, it conserves the Type – II misalignment of InAs and GaSb, which is capable of eliminating the electron-hole split – off band Auger transition by reducing the resonance between the energy gap and split-off band. Second, the AlSb layer has a large energy bandgap with the conduction band offset higher than that of GaSb and the valence band offset slightly higher than that of InAs. Due to this band offset, AlSb can be utilized as a blocking layer for both electrons in the conduction band and holes in the valence band. As a consequence, the insertion of the AlSb into the GaSb, forming the M – superlattice, will reduce the tunneling probability in long wavelength (LWIR) and very long wavelength (VLWIR) photodiodes because the effective mass of the carriers over the standard binary – binary SL is increased. In comparison with other ternary/quaternary superlattices, such as the WSL or the InAs/GaInSb superlattices, the M structure is easier to realize because it still keeps the simple form of a binary – only structure, which is less sensitive to the growth temperature and the III-V flux ratio. Finally, the growth of the M-structure is as simple as a standard binary – binary InAs/GaSb structure because there is a small mismatch in the lattice constant between AlSb (6.136 Å) and GaSb (6.097 Å) and the common antimony atom allows for a smooth interface between the two layers. The M-structure does not need as much care as the growth of AlSb on InAs in the WSL where the interface of AlSb and InAs have no common atom and AlSb grown on InAs is highly strained.

M-structure superlattice has been successfully integrated onto Type II InAs/GaSb superlattice photodiodes and demonstrated orders of magnitude of improvement for the electrical performance of LWIR and VLWIR detectors.

Material system with a large variation range of cut-off wavelength.

One of the benefits of Type II superlattice is the capability to tune the detection cut-off wavelength in a very wide range. By adjusting the thicknesses of constituent layers, the energy gap of the structure can be precisely controlled with excellent uniformity over a three inch wafer area. We have experimentally demonstrated Type-II InAs/GaSb superlattice photodiodes with cut-off wavelength varying from 3.5mm up to 32mm. The measured results fit nicely with the theoretical prediction using Empirical Tight Binding Model.

Spectral response of photodiodes with different InAs/GaSb superlattices in their active layer. The thickness of GaSb layer is 40 Å for all of the superlattices, while the thickness of the InAs layer is shown for each device. ETBM calculations agree with experimental data.

Relative responsivity for Type-II superlattice detectors with cutoff wavelength of 32 μm at T=9.2 K.

At the longest cut-off wavelength ( ~32 μm ), the detectors have a peak responsivity of 3 A/W and a detectivity of 4.25 x 1010 cm·Hz½/W at 15 μm under 40 mV reverse bias at 34 K.

Ultra Fast Uncooled Infrared Detectors

High-speed uncooled infrared (IR) detectors are highly demanded for many military and industrial applications such as: target detection systems, proximity fuzes, LIDARs, non-destructive testing and inspection techniques, monitoring of the chemical quality and process control, remote sensing, and free space communication. Commercially available uncooled IR imaging sensors use ferroelectric or microbolometer detectors which are inherently slow. Although photon detectors have gigahertz bandwidths, their high temperature detectivity is severely degraded due to several physical limitations. The existing infrared photon detectors can be categorized as interband, such as HgCdTe, and intersubband quantum well infrared detectors (QWIP). There are some fundamental limitations, namely fast Auger recombination rate in the interband detectors and high thermal generation rate in the intersubband detectors, which drastically decrease their performance and ability for high temperature operation.

At first, we developed the growth of high quality Type-II superlattices. In order to increase the operating temperature of detectors, we designed the superlattices for an effective suppression of Auger recombination, and confirmed it experimentally or the first time.

The progress of cooled and un-cooled Type-II detectors at CQD.

Using such designs, we demonstrated the first uncooled infrared detectors from Type-II superlattices. The measured detectivity is more than 1x108 cm x Hz½/W at 10.6 μm at room temperature which is higher than the commercially available uncooled photon detectors at similar wavelength. The measured carrier lifetime was about 27 nsec which is an order of magnitude longer than the bulk material due to the suppression of the Auger recombination. To use such devices in focal plane arrays (FPA) for imaging applications, we also developed Type-II photodiodes operating at zero bias.

Comparison with the state of the art and with the theoretical Auger limited detectivity.

Furthermore, we realized the first uncooled Type-II photodiode at λ=8 μm with a zero bias detectivity of 1 x 108 cm·Hz½/W. Recently we demonstrated uncooled photodiodes with 5 μm cutoff that have a zero bias detectivity above 1 x 109 cm·Hz½/W and a device quantum efficiency exceeding 30 %. These results indicate that Type II superlattice is an excellent candidate for uncooled applications.

High performance Superlattice Photodiodes

Very high performance long-wavelength infrared (LWIR or 8~12 μm) and very-long-wavelength infrared (VLWIR, l > 12 μm) detectors and imaging arrays are in high demand for strategic missile defense, pollution monitoring, and space-based astronomy. Material uniformity complexities and strong leakage currents limit the viability of state-of-the-art HgCdTe detectors in this wavelength regime. For this reason, type-II superlattices are being pursued as an alternative third generation focal plane array technology.

Intensive research in the LWIR and VLWIR has lifted the performance of Type II superlattice photodiodes to a comparable level to the state-of-the-art HgCdTe technology. High quality material has been obtained, allowing for the very thick device structure without any degradation of the crystallinity. As a results, the absorption length of the photodiodes could be extended, the devices exhibit a quantum efficiency more than 50% for front side, single path configuration, and more than 75% for back side multiple path configurations.

Optical responsivity, Quantum efficiency and specific detectivity as a function of device thicknesses. Thicker device allows for higher optical performance.

In attempt to reduce the electrical noise due to the dark current, we developed a new device architecture, where the M-structure superlattice was used as a barrier in between the p and n- regions of the diode. The M-barrier has been shown to efficiently suppress both the tunneling and the diffusion current of the device, leading to an order of magnitude decrease of the dark current.

New device architecture with M-structure superlattice for the suppression of dark current.

A combination of optimization schemes for the optical and electrical performance enables LWIR devices to be BLIP limited at 110K with a 2p field of view facing a 300K background. The same study can be applied for

Measurement of BLIP temperature using the delineation of dark current between cold shielded/ no cold shield configurations, and using specific detectivity measurement.

World's First High PerformanceType-II Superlattice Focal Plane Array

Building on our extensive experience on this material, we have recently demonstrated the world's first uncooled Type-II mid-wave infrared focal plane array operating with a 5 μm cutoff wavelength. This uncooled camera array operates with 25 % quantum efficiency, a detectivity of 8 x 108 cm·Hz½/W, and a NEΔT of 50 K.

MWIR Type-II InAs/GaSb superlattice FPA imaging obtained at 77 K, left. Uncooled infrared imaging of a hot soldering iron based on MWIR Type-II InAs/GaSb superlattices, right.

These superlattice FPAs provide high quality imaging of warm subjects, such as human beings, up to a temperature of about 160 K, significantly higher than the conventional operating temperature of 77 K. It can also provide fast uncooled imaging at room temperature for a hot soldering iron with demonstrated frame rate of 110 Hz and potentially up to 600 Hz.

Silicon dioxide surface passivation greatly reduces the surface leakage in VLWIR type-II photodiodes, making focal plane arrays in this wavelength regime a possibility.

One obstacle to the technological success of type-II infrared focal plane imaging arrays is solving the ever-present problem of surface passivation. The small dimensions of focal plane array pixels enhance the amount of leakage current caused by surface effects. With a proper electrically passivating layer, surface states can be reduced and leakage current decreased, greatly improving the overall device detectivity and performance. At CQD we have demonstrated successful silicon dioxide passivation in the MWIR, LWIR, and VLWIR on type-II photodiodes. Additionally, we have developed a polyimide-based technique that significantly reduces surface leakage in LWIR devices.

I-V characteristic of small devices passivated with polyimide (left). Variation of the dynamic resistance with the size of the diodes (right).

Using our experience for FPA fabrication and our expertise on LWIR type-II InAs/GaSb superlattice single element detectors, we started developing FPAs in the LWIR (8-12μm). As the wavelength increases (the bandgap decreases), the devices become more sensitive to surface effects, making the FPA fabrication process more critical. Thanks to enhancement in our growing, etching, cleaning, hybridation techniques, we managed to fabricate the world's first and best 320x256 FPA based on type-II InAs/GaSb superlattice photodetectors with a cutoff wavelength higher than 8 μm. This FPA with the highest cutoff wavelength demonstrated yet for type-II superlattice is able to perform imaging of human beings from 81 K to 120 K. It can also perform imaging of soldering iron up to 200 K. The array is able to detect temperature differences as small as 20 mK. The quantum efficiency of the array reaches over 80% when an AR coating is deposited.

LWIR Type-II InAs/GaSb superlattice FPA imaging obtained at 80K.

Negative Luminescence

Negative Luminescence (NL) is an expression describing the manipulation of the radiative balance of a low band gap minority carrier device with the ambient. This phenomenon can be observed by the extraction of carriers from the active region of a photodiode through the application of reverse bias. There are numerous potential applications of NL devices, which include dynamic cold shields for focal plane arrays and fast infrared scene simulators.

Spectra of electroluminescence and negative luminescence of LWIR Type-II photodetectors at 250 K.

NL has been observed in various infrared material systems mostly in the mid-infrared spectral range around 5 μm. At CQD, for the first time, NL was demonstrated in a III-V based system covering the entire infrared spectral range between 5 and 13 μm with longwavelength infrared (LWIR) InAs/GaSb superlattice photodiodes.

Nanoscale Structures for Enhanced Type-II Photodetectors

Highly uniform nanopillars of Type-II InAs/GaSb superlattices. The diameter of such nanopillars can be less than 50 nm.

To further enhance this technology, we are exploring nanoscale structures with the goal of achieving higher temperature operation and wavelength tunability. Theoretical calculations show that devices based on these quantum-size structures can be realized with much higher performance. However, a key technical issue is the fabrication of large arrays of "nanopillars" with good uniformity. We have successfully used electron beam lithography and plasma etching techniques to realize the first nanometer-sized structures in Type-II InAs/GaSb superlattice structures with excellent uniformity over large areas.

Last Updated 03/20/2009