AVS 62nd International Symposium & Exhibition | |
Electronic Materials and Processing | Wednesday Sessions |
Session EM+AS+MS+SS-WeA |
Session: | Surface and Interface Challenges in Wide Bandgap Materials |
Presenter: | Charles Eddy, Jr., U.S. Naval Research Laboratory |
Authors: | C.R. Eddy, Jr., U.S. Naval Research Laboratory N. Nepal, Sotera Defense Solutions M.J. Tadjer, U.S. Naval Research Laboratory T.J. Anderson, U.S. Naval Research Laboratory A.D. Koehler, U.S. Naval Research Laboratory J.K. Hite, U.S. Naval Research Laboratory K.D. Hobart, U.S. Naval Research Laboratory |
Correspondent: | Click to Email |
For the past 25 years, compound semiconductors comprised of elements from group III-B of the periodic table and nitrogen have attracted a sustained, high-level of research focus. More recently they have found growing application to rf and power electronics in the form of advanced transistor structures such as the high electron mobility transistor (HEMT) with and without insulated gates. Key performance parameters for such devices (cut-off frequency for rf transistors and on-resistance for power transistors) are often dominated by the contact resistance. The current best approach to contact resistance minimization involves aggressive processing requirements that challenge device fabrication, especially when insulated gates are required. A potential solution is the regrowth of highly conducting semiconductor contact layers where ohmic contacts are needed.
Here we report on initial efforts to employ regrown indium nitride (InN) contact layers by atomic layer epitaxy (ALE) as a low temperature solution to the ohmic contact challenge for III-N transistors. Recently, we have reported that good crystalline quality InN can be grown at less than 250°C by ALE [1]. Here we employ such conditions to grow very thin layers and assess them morphologically and electrically.
InN regrown contact layers of 5nm thickness grown on sapphire are very smooth (rms roughness < 0.17nm) and possess sheet resistances as low at 3.6 kΩ/sq, corresponding to electron sheet carrier densities of 2-3 x1013 cm-2 and mobilities of 50 cm2/V-s. These electron mobilities are higher than previously reported (30 cm2/V-s) for much thicker films (1.3 μm) [2]. Similarly grown 22.5 nm thick InN layers on highly resistive silicon were processed with mesa isolation regions and 20/200 nm thick titanium/gold contact metals. Without any contact annealing, an ohmic contact resistance of 9.7x10-7 Ω-cm2 (1.2 Ω-mm) was measured, comparable to the best high temperature alloyed contact to an AlGaN/GaN HEMT.
In our initial non-alloyed ohmic contact process, contact regions were recessed down to the GaN buffer layer to establish physical contact between the highly-conductive InN layer and electrons in the HEMT channel. A 25 nm thick InN layer was then grown by ALE, and the InN-filled ohmic regions were then capped with a Ti/Al/Ti/Au layers. Using the metals as an etch mask, the InN outside of the ohmic regions was etched away. We will report on initial results of application of ALE InN regrown contact layers and the modified fabrication approaches to AlGaN/GaN HEMTs.
1. N. Nepal, et al., J Cryst. Growth and Design, 13, 1485-1490 (2013).
2. Kuo et al., Diamond & Related Materials20, 1188 (2011).