Abstract: A High Electron Mobility Transistor (HEMT) device can include an AlN buffer layer on a substrate and an epi-GaN channel layer on the AlN buffer layer. An AlN barrier layer can be on the Epi-GaN channel layer to provide a channel region in the epi-GaN channel layer. A GaN drain region can be recessed into the epi-GaN channel layer at a first end of the channel region and a GaN source region can be recessed into the epi-GaN channel layer at a second end of the channel region opposite the first end of the channel region. A gate electrode can include a neck portion with a first width that extends a first distance above the AlN barrier layer between the GaN drain region and the GaN source region to a head portion of the gate electrode having a second width that is greater than the first width.

Abstract: III-Nitride heterostructures with low p-type sheet resistance and III-Nitride heterostructure devices with gate recess and devices including the III-Nitride heterostructures are disclosed.

Abstract: Gallium nitride high-electron-mobility transistors (GaN HEMTs) are at a point of rapid growth in defense (radar, SATCOM) and commercial (5G and beyond) industries. This growth also comes at a point at which the standard GaN heterostructures remain unoptimized for maximum performance. For this reason, the shift to the aluminum nitride (AlN) platform is disclosed. AlN allows for smarter, highly-scaled heterostructure design that improves the output power and thermal management of GaN amplifiers. Beyond improvements over the incumbent amplifier technology, AlN allows for a level of integration previously unachievable with GaN electronics. State-of-the-art high-current p-channel FETs, mature filter technology, and advanced waveguides, all monolithically integrated with an AlN/GaN/AlN HEMT, is made possible with aluminum nitride. It is on this AlN platform that nitride electronics may maximize their full high-power, highspeed potential for mm-wave communication and high-power logic applications.

Abstract: The long-missing polarization-induced two-dimensional hole gas is finally observed in undoped Group III nitride semiconductor structures and in undoped Group II or Group III oxide semiconductor structures. Experimental results providing unambiguous proof that a 2D hole gas in GaN grown on AlN does not need acceptor doping, and can be formed entirely by the difference in the internal polarization fields across the semiconductor heterojunction are presented.

Abstract: The long-missing polarization-induced two-dimensional hole gas is finally observed in undoped Group III nitride semiconductor structures and in undoped Group II or Group III oxide semiconductor structures. Experimental results providing unambiguous proof that a 2D hole gas in GaN grown on AlN does not need acceptor doping, and can be formed entirely by the difference in the internal polarization fields across the semiconductor heterojunction are presented.

Abstract: A High Electron Mobility Transistor (HEMT) device can include an AlN buffer layer on a substrate and an epi-GaN channel layer on the AlN buffer layer. An AlN barrier layer can be on the Epi-GaN channel layer to provide a channel region in the epi-GaN channel layer. A GaN drain region can be recessed into the epi-GaN channel layer at a first end of the channel region and a GaN source region can be recessed into the epi-GaN channel layer at a second end of the channel region opposite the first end of the channel region. A gate electrode can include a neck portion with a first width that extends a first distance above the AlN barrier layer between the GaN drain region and the GaN source region to a head portion of the gate electrode having a second width that is greater than the first width.

Abstract: III-Nitride heterostructures with low p-type sheet resistance and III-Nitride heterostructure devices with gate recess and devices including the III-Nitride heterostructures are disclosed.