Schottky structures based on Mg-doped GaN layers grown by metalorganic chemical vapor deposition (MOCVD) on sapphire substrate are studied by thermal admittance spectroscopy from 90 K to room temperature. Evidence of two impurity levels results from the analysis of the observed peaks in the conductance curves, whose positions and strengths are temperature dependent. The experimental results are analyzed within a detailed theoretical study of the steady-state and small-signal electrical characteristics of the structure. Numerical simulations are based on the solution of the basic semiconductor equations for the structure consisting of two Schottky diodes connected back-to-back by a conduction channel formed by the GaN layer.
IntroductionSuccessful Mg-doping of GaN has led to a breakthrough in the use of this wide band-gap compound semiconductor both for optoelectronics and for high-power, high-frequency electronic devices. As Schottky-type junctions are the building blocks of these devices, we have performed a thorough analysis of the conduction mechanism in GaN : Mg double Schottky structures. We use numerical simulation to fully explain the experimental results obtained by thermal admittance spectroscopy. It is shown that, due to the simultaneous role of Mg both as a dopant and as a deep impurity, the classical analysis of the Arrhenius plot underestimates the defect ionization energy. Moreover, we show the existence of a second shallow acceptor state with an activation energy of several tens of meV.
Experimental ResultsEpitaxial growth by metalorganic chemical vapor deposition (MOCVD) of the GaN layers studied in this work has been detailed elsewhere [1]. The structures consist of a nucleation layer grown directly on top of the sapphire substrate, followed by a 1 µm thick undoped buffer layer and a 2 µm thick Mg-doped layer. Coplanar metallic contacts (Ni/Au) of 0.5 mm diameter and separated by 2 mm, were evaporated on top of the layers.In Fig. 1, frequency responses of the conductance G divided by ω = 2πf, where ƒ is the measurement frequency, of a typical sample, are shown for temperatures ranging from room temperature (RT) down to 90 K. Between RT and 200 K, the G/ω curves show a large peak at the cutoff frequencies fc in C-f curves (not shown here). The amplitude of this peak decreases as the temperature is lowered. At around 200 K, a shoulder emerges from the high-frequency side of the mentioned peak and is resolved into another peak for temperatures below 170 K. Its position is also temperature dependent.Published in : Physica Status Solidi B. Basic Research (2001), vol. 228, iss. 2, pp. 385-389. Authors : N. D. Nguyen, M. Germain, M. Schmeits, B. Schineller, and M. Heuken Status : Postprint (Author's version)
Fig. 1. Experimental curves of conductance G divided by ω = 2πf as function of frequency ƒ for temperatures ranging from a) 293 (RT) to 210 K and b) 190 to 90 K (curves from top to bottom)
Numerical SimulationIt is known that Mg gives rise to an acceptor-type energy level in the GaN bandgap. ...