Abstract:We present the oxidation process of epitaxial Ni (111)/GaN (0001) thin films studied by in situ synchrotron x-ray scattering, scanning electron microscopy, and transmission electron microscopy. By monitoring the evolution of the Ni (111) Bragg reflection, we reveal that two distinct oxidation processes occur. Initially, a continuous NiO layer of about 50 Å thickness is formed on the surface of Ni. The planar oxide layer saturates immediately and passivates the film from further surface oxidation. From this sta… Show more
“…For this 600 °C Ni nanoparticle oxidation, we think the "critical thickness" can be approximated by the above h(S1 end ) of the large Ni. This value is higher than the retraction of 3.5 nm reported for a Ni film oxidization at 300 °C, 50 consistent with the temperature effect on nucleation and oxide nuclei size. 49 Thus, since the radii of small Ni nanoparticles are smaller than the critical thickness under our oxidation condition, their oxidation did not proceed into the subsequent NiO thickening process (i.e., no Kirkendall voids were observed).…”
High-temperature oxidation mechanisms
of metallic nanoparticles
have been extensively investigated; however, it is challenging to
determine whether the kinetic modeling is applicable at the nanoscale
and how the differences in nanoparticle size influence the oxidation
mechanisms. In this work, we study thermal oxidation of pristine Ni
nanoparticles ranging from 4 to 50 nm in 1 bar 1%O2/N2 at 600 °C using in situ gas-cell environmental
transmission electron microscopy. Real-space in situ oxidation videos revealed an unexpected nanoparticle surface refacetting
before oxidation and a strong Ni nanoparticle size dependence, leading
to distinct structural development during the oxidation and different
final NiO morphology. By quantifying the NiO thickness/volume change
in real space, individual nanoparticle-level oxidation kinetics was
established and directly correlated with nanoparticle microstructural
evolution with specified fast and slow oxidation directions. Thus,
for the size-dependent Ni nanoparticle oxidation, we propose a unified
oxidation theory with a two-stage oxidation process: stage 1: dominated
by the early NiO nucleation (Avrami–Erofeev model) and stage
2: the Wagner diffusion-balanced NiO shell thickening (Wanger model).
In particular, to what extent the oxidation would proceed into stage
2 dictates the final NiO morphology, which depends on the Ni starting
radius with respect to the critical thickness under given oxidation
conditions. The overall oxidation duration is controlled by both the
diffusivity of Ni2+ in NiO and the Ni in Ni self-diffusion.
We also compare the single-particle kinetic curve with the collective
one and discuss the effects of nanoparticle size differences on kinetic
model analysis.
“…For this 600 °C Ni nanoparticle oxidation, we think the "critical thickness" can be approximated by the above h(S1 end ) of the large Ni. This value is higher than the retraction of 3.5 nm reported for a Ni film oxidization at 300 °C, 50 consistent with the temperature effect on nucleation and oxide nuclei size. 49 Thus, since the radii of small Ni nanoparticles are smaller than the critical thickness under our oxidation condition, their oxidation did not proceed into the subsequent NiO thickening process (i.e., no Kirkendall voids were observed).…”
High-temperature oxidation mechanisms
of metallic nanoparticles
have been extensively investigated; however, it is challenging to
determine whether the kinetic modeling is applicable at the nanoscale
and how the differences in nanoparticle size influence the oxidation
mechanisms. In this work, we study thermal oxidation of pristine Ni
nanoparticles ranging from 4 to 50 nm in 1 bar 1%O2/N2 at 600 °C using in situ gas-cell environmental
transmission electron microscopy. Real-space in situ oxidation videos revealed an unexpected nanoparticle surface refacetting
before oxidation and a strong Ni nanoparticle size dependence, leading
to distinct structural development during the oxidation and different
final NiO morphology. By quantifying the NiO thickness/volume change
in real space, individual nanoparticle-level oxidation kinetics was
established and directly correlated with nanoparticle microstructural
evolution with specified fast and slow oxidation directions. Thus,
for the size-dependent Ni nanoparticle oxidation, we propose a unified
oxidation theory with a two-stage oxidation process: stage 1: dominated
by the early NiO nucleation (Avrami–Erofeev model) and stage
2: the Wagner diffusion-balanced NiO shell thickening (Wanger model).
In particular, to what extent the oxidation would proceed into stage
2 dictates the final NiO morphology, which depends on the Ni starting
radius with respect to the critical thickness under given oxidation
conditions. The overall oxidation duration is controlled by both the
diffusivity of Ni2+ in NiO and the Ni in Ni self-diffusion.
We also compare the single-particle kinetic curve with the collective
one and discuss the effects of nanoparticle size differences on kinetic
model analysis.
“…8 Recently, NiO formed by thermal oxidation of Ni films has been proposed as the gate insulator in AlGaN/GaN HEMTs. 9 However, the thermal oxidation of Ni films can proceed through different stages 10,11 and can result into the formation of voids in the oxide layer. 10 This latter severely compromise the devices reliability and a uniform and epitaxial layer would certainly be preferred.…”
This letter reports on epitaxial nickel oxide (NiO) films grown by metal-organic chemichal vapor deposition on AlGaN/GaN heterostructures. The grown material was epitaxial, free from voids and exhibited a permittivity of 11.7, close to bulk NiO. This approach is advantageous with respect other methods such as the thermal oxidation of Ni films due to a better reproducibility and film quality. A reduction of the leakage current in Schottky diodes with an interfacial NiO layer has been observed and described using the metal-insulator-semiconductor Schottky model. The results indicate that these films are promising as gate dielectric for AlGaN/GaN transistors technology.
“…Composite Interfaces 129 contact relaxes the Fermi-level pinning and suppresses the trap-assisted tunneling current. [11] Kang et al [12] reported that a NiO layer is easily formed when Ni is oxidized at temperature 300°C. NiO is also reported to behave as a p-type semiconductor with nickel vacancies and/or oxygen interstitials.…”
Al 0.11 Ga 0.89 N/GaN samples are grown by plasma-assisted molecular beam epitaxy method on (1 1 1) silicon substrates. High purity gallium (7N) and aluminum (6N5) were used to grow Al 0.11 Ga 0.89 N, GaN, and AlN, respectively. The surface morphology, structural and optical properties of the sample has been investigated by scanning electron microscope (SEM), and high-resolution X-ray diffraction (HR-XRD), respectively. HR-XRD measurement showed that the sample has a typical diffraction pattern of hexagonal Al 0.11 Ga 0.89 N/GaN heterostructures. Ni/Ag bilayers are deposited on Al 0.11 Ga 0.89 N as the Schottky contacts. The effect of annealing in oxygen ambient on the electrical properties of Ni/Ag/Al 0.11 Ga 0.89 N is studied by currentvoltage measurement. The annealing at a temperature of 700°C for 10 min results in an increase in the ideality factor from 1.033 to 1.042 and an increase in the Schottky barrier height from 0.708 to 0.811 eV. Furthermore, the annealing in oxygen ambient also leads to an increase in the surface roughness of the contacts from 0.0098 to 0.1360 μm which is in agreement with the SEM results.
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