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30 June 2017
High-quality nitrogen-polar gallium nitride vertical p-n diodes
Cornell University in the USA has developed vertical p-n diodes using nitrogen-polar c-plane (000-1) gallium nitride (GaN) growth [YongJin Cho et al, Appl. Phys. Lett., vol110, p253506, p2017]. The researchers report: “A very low dislocation density leads to a high reverse breakdown electric field of ~2.2MV/cm without fields plates — the highest reported for N-polar epitaxial structures.” They further claim that their devices are the highest-quality p-n diodes ever demonstrated on N-polar GaN in terms of reverse bias leakage.
The GaN crystal structure has strong charge polarization in the c-direction due to the ionic nature of the Ga-N chemical bond. The Cornell team suggests that growing material in the N-polar rather than more common Ga-polar form, reversing the polarization, could lead to new electronic and photonic device opportunities such as ultra-low-power tunneling transistors, buried barrier high-electron-mobility transistors, and interband tunnel junctions. Further polarization engineering is used to create two-dimensional electron gas (2DEG) transistor channel layers and can also be exploited to improve hole densities in p-type regions.
N-polar growth allows higher growth temperatures since the material is more robust against decomposition. However, bulk GaN substrates are usually prepared in Ga-polar form, and high-quality, low-dislocation, smooth N-polar GaN substrates have only recently become available.
The N-polar GaN (000-1) substrate for Cornell’s work was supplied by Ammono SA. The n+ doping in the substrate delivered an electron concentration around 1019/cm3. X-ray diffraction analysis suggested a dislocation density of 5x104/cm2, much lower than the 109/cm2 typical of GaN material on alternative substrates. Root-mean-square roughness over a 10μmx10μm field was ~0.4nm, according to atomic force microscopy (AFM).

Figure 1: (a) In-situ reflection high-energy electron diffraction (RHEED) pattern showing (3x3) reconstruction characteristic of N-polar surface, and (b) AFM micrograph of MBE-grown N-polar GaN p-n diodes showing atomic steps. (c) Schematic layer structure and (d) cross-section transmission electron micrograph of fabricated vertical p-n diodes. Two white grooves on sides of image highlight interface between single-crystal bulk GaN substrate and MBE-grown epi-layers.
The p-n diodes (Figure 1) were grown using Ga-rich plasma-assisted molecular beam epitaxy (PAMBE) on a Veeco Gen Xplor machine. Excess Ga droplets were removed after growth by hydrochloric acid cleaning. Analysis of the diode material suggested that “the high structural perfection of the single-crystal GaN substrate was largely transferred to the MBE-overgrown p-n diodes,” according to the researchers. The diodes were fabricated with 600nm-high mesas for electrical isolation.
A 50μm-diameter device had a 3.5V turn-on voltage, close to that expected from the ~3.4eV bandgap of GaN. At 5V forward bias, the current density was 7.8kA/cm2, and the specific differential on-resistance was 0.1mΩ-cm2. The resistance was not corrected for the probe and therefore the actual value is smaller. Under reverse bias down to -6V, the leakage was less than 10-5A/cm2. The ±5V on/off current ratio was more than 109.
“This high performance proves high-quality N-polar GaN p-n diodes with a low dislocation density are now possible by MBE,” the researchers comment.
Electroluminescence was also observed with photon energy peaks at 3.13eV and 3.39eV with 5V forward bias and 1.5kA/cm2 current density. The 3.39eV was attributed to near-band-edge (NBE) emission. The 3.13eV emissions were assigned to conduction band-to-acceptor (CBA) transitions in p-GaN layers. The magnesium doping of p-GaN gives a hole binding energy around 0.25eV.
A very weak broad deep-level transition was also observed around 2.2eV. The team writes: “The presence of the NBE and CBA peaks, and the weak intensity of the broad band peak indicate a low density of deep point defects in the p-n diodes.”

Figure 2: (a) Current density versus voltage characteristics of N-polar GaN single-crystal diodes in semilog scale showing high rectification ratio and low on-resistance. (b) Electroluminescence spectrum measured at 5V forward bias. Inset: linear-scale current density versus forward voltage.
Reverse-bias breakdown was studied using a 20μm-diameter diode. Abrupt breakdown occurred at -76V, just after the current leakage reached 10-1A/cm2 density. The researchers attribute the breakdown to trap-assisted avalanche effects as opposed to interband Zener tunneling.
Using capacitance-voltage measurements to estimate the electron concentration in the unintentionally doped (uid) GaN layer (9.6x1016/cm3), the researchers calculated that the peak electric field at breakdown was around 2.2MV/cm, occurring at the edge of the depletion region.
The team comments: “This breakdown electric field, lower than the best Ga-polar GaN p-n diodes of ~4MV/cm, nevertheless indicates the highest value for N-polar GaN p-n diodes and can be significantly improved by sculpting the electric field externally using field-plates as the Ga-polar counterparts. The full performance and true breakdown behavior of the diodes may be accessible by electrically isolating the device regions from edge sidewalls.”
N-polar GaN GaN p-n diodes MBE PAMBE Veeco
http://dx.doi.org/10.1063/1.4989581
The author Mike Cooke is a freelance technology journalist who has worked in the semiconductor and advanced technology sectors since 1997.
 
    














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    Juno Publishing and Media Solutions Ltd. All rights reserved. Semiconductor
    Today and the editorial material contained within it and related media is
    the copyright of Juno Publishing and Media Solutions Ltd. Reproduction in
    whole or part without permission from Juno Publishing and Media Solutions
    Ltd is forbidden. In most cases, permission will be granted, if the magazine
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