Figure 8 - available via license: CC BY
Content may be subject to copyright.
Adatom migration process on different substrate surfaces: (a-d) on (0001) Al-terminated AlN surface and (e-h) on 0001 N-terminated AlN surface with growth temperature of 1450 K and injected Al:Ga = 1:1. The deep blue and light blue atoms represent Al and N atoms in the AlN substrate while the green, red, and yellow atoms represent Al, Ga and N atoms in the deposited film correspondingly. 

Adatom migration process on different substrate surfaces: (a-d) on (0001) Al-terminated AlN surface and (e-h) on 0001 N-terminated AlN surface with growth temperature of 1450 K and injected Al:Ga = 1:1. The deep blue and light blue atoms represent Al and N atoms in the AlN substrate while the green, red, and yellow atoms represent Al, Ga and N atoms in the deposited film correspondingly. 

Source publication
Article
Full-text available
The growth of AlGaN has been extensively studied, but corresponding research related to the effect of AlN substrate surface has rarely been reported in literature. In this article, the effects of AlN substrate surface on deposition of AlGaN films were investigated by molecular dynamics (MD) simulations. (0001) Al-terminated and (0001¯) N-terminated...

Contexts in source publication

Context 1
... further verify the different mobility of Al and Ga adatoms on two different surfaces, the time-resolved processes for migration of adatoms on the substrate surfaces at 1450 K and injected Al:Ga = 1:1 are displayed in Figure 8. Figure 8a-d shows the migration process of adatoms on (0001) Al-terminated AlN surface, while Figure 8e-h shows the migration process of adatoms on 0001N-terminated AlN surface. In Figure 8a,b, the adatoms successively approach the substrate then start to bond with appropriate atoms. We can see in Figure 6c that the N adatom bonds with Al atom on the substrate and another N adatom moves toward the Al adatoms. The next moment, in Figure 8d, the bond between the first N adatom and substrate Al atom breaks up and the N adatom moves toward the Ga adatom to find a new lattice site. Meanwhile, another pair of Al and N adatoms also move towards each other. A similar process can be observed in Figure 8e-h. However, when we carefully compare the migration processes on different surfaces, we find that Al and Ga adatoms gradually move away from their initial position after they approach the (0001) Al-terminated surface. By comparison, Al and Ga adatoms have little movement from their initial position after they approach the 0001 N-terminated surface. Apparently, Al and Ga adatoms have a longer migration length on (0001) Al-terminated AlN surface than on 0001 N-terminated AlN surface, facilitating the movement of Al and Ga adatoms to find the ideal lattice site. ...
Context 2
... further verify the different mobility of Al and Ga adatoms on two different surfaces, the time-resolved processes for migration of adatoms on the substrate surfaces at 1450 K and injected Al:Ga = 1:1 are displayed in Figure 8. Figure 8a-d shows the migration process of adatoms on (0001) Al-terminated AlN surface, while Figure 8e-h shows the migration process of adatoms on 0001N-terminated AlN surface. In Figure 8a,b, the adatoms successively approach the substrate then start to bond with appropriate atoms. We can see in Figure 6c that the N adatom bonds with Al atom on the substrate and another N adatom moves toward the Al adatoms. The next moment, in Figure 8d, the bond between the first N adatom and substrate Al atom breaks up and the N adatom moves toward the Ga adatom to find a new lattice site. Meanwhile, another pair of Al and N adatoms also move towards each other. A similar process can be observed in Figure 8e-h. However, when we carefully compare the migration processes on different surfaces, we find that Al and Ga adatoms gradually move away from their initial position after they approach the (0001) Al-terminated surface. By comparison, Al and Ga adatoms have little movement from their initial position after they approach the 0001 N-terminated surface. Apparently, Al and Ga adatoms have a longer migration length on (0001) Al-terminated AlN surface than on 0001 N-terminated AlN surface, facilitating the movement of Al and Ga adatoms to find the ideal lattice site. ...
Context 3
... further verify the different mobility of Al and Ga adatoms on two different surfaces, the time-resolved processes for migration of adatoms on the substrate surfaces at 1450 K and injected Al:Ga = 1:1 are displayed in Figure 8. Figure 8a-d shows the migration process of adatoms on (0001) Al-terminated AlN surface, while Figure 8e-h shows the migration process of adatoms on 0001N-terminated AlN surface. In Figure 8a,b, the adatoms successively approach the substrate then start to bond with appropriate atoms. We can see in Figure 6c that the N adatom bonds with Al atom on the substrate and another N adatom moves toward the Al adatoms. The next moment, in Figure 8d, the bond between the first N adatom and substrate Al atom breaks up and the N adatom moves toward the Ga adatom to find a new lattice site. Meanwhile, another pair of Al and N adatoms also move towards each other. A similar process can be observed in Figure 8e-h. However, when we carefully compare the migration processes on different surfaces, we find that Al and Ga adatoms gradually move away from their initial position after they approach the (0001) Al-terminated surface. By comparison, Al and Ga adatoms have little movement from their initial position after they approach the 0001 N-terminated surface. Apparently, Al and Ga adatoms have a longer migration length on (0001) Al-terminated AlN surface than on 0001 N-terminated AlN surface, facilitating the movement of Al and Ga adatoms to find the ideal lattice site. ...
Context 4
... further verify the different mobility of Al and Ga adatoms on two different surfaces, the time-resolved processes for migration of adatoms on the substrate surfaces at 1450 K and injected Al:Ga = 1:1 are displayed in Figure 8. Figure 8a-d shows the migration process of adatoms on (0001) Al-terminated AlN surface, while Figure 8e-h shows the migration process of adatoms on 0001N-terminated AlN surface. In Figure 8a,b, the adatoms successively approach the substrate then start to bond with appropriate atoms. We can see in Figure 6c that the N adatom bonds with Al atom on the substrate and another N adatom moves toward the Al adatoms. The next moment, in Figure 8d, the bond between the first N adatom and substrate Al atom breaks up and the N adatom moves toward the Ga adatom to find a new lattice site. Meanwhile, another pair of Al and N adatoms also move towards each other. A similar process can be observed in Figure 8e-h. However, when we carefully compare the migration processes on different surfaces, we find that Al and Ga adatoms gradually move away from their initial position after they approach the (0001) Al-terminated surface. By comparison, Al and Ga adatoms have little movement from their initial position after they approach the 0001 N-terminated surface. Apparently, Al and Ga adatoms have a longer migration length on (0001) Al-terminated AlN surface than on 0001 N-terminated AlN surface, facilitating the movement of Al and Ga adatoms to find the ideal lattice site. ...
Context 5
... further verify the different mobility of Al and Ga adatoms on two different surfaces, the time-resolved processes for migration of adatoms on the substrate surfaces at 1450 K and injected Al:Ga = 1:1 are displayed in Figure 8. Figure 8a-d shows the migration process of adatoms on (0001) Al-terminated AlN surface, while Figure 8e-h shows the migration process of adatoms on 0001N-terminated AlN surface. In Figure 8a,b, the adatoms successively approach the substrate then start to bond with appropriate atoms. We can see in Figure 6c that the N adatom bonds with Al atom on the substrate and another N adatom moves toward the Al adatoms. The next moment, in Figure 8d, the bond between the first N adatom and substrate Al atom breaks up and the N adatom moves toward the Ga adatom to find a new lattice site. Meanwhile, another pair of Al and N adatoms also move towards each other. A similar process can be observed in Figure 8e-h. However, when we carefully compare the migration processes on different surfaces, we find that Al and Ga adatoms gradually move away from their initial position after they approach the (0001) Al-terminated surface. By comparison, Al and Ga adatoms have little movement from their initial position after they approach the 0001 N-terminated surface. Apparently, Al and Ga adatoms have a longer migration length on (0001) Al-terminated AlN surface than on 0001 N-terminated AlN surface, facilitating the movement of Al and Ga adatoms to find the ideal lattice site. ...

Similar publications

Article
Full-text available
The development of ultraviolet AlGaN multiple quantum well (MQW) light emitting diodes (LEDs) in the wavelength range between 239 and 217 nm is presented. The effects of aluminum composition in the MQW active region and of the underlying AlxGa1-xN:Si current spreading layer on the emission characteristics and operating voltages are investigated. A...

Citations

... Similar SW potentials have already been successfully applied to investigate an InGaN film grown on a GaN surface. [19][20][21] To begin with, an energy minimization of the system by iteratively adjusting atom coordinates was performed. Then the NPT ensemble (constant temperature and constant volume) was used to balance 300 ps at 300 K, and the time step was 1 fs. ...
Article
Exploring interfacial thermal transport of a heterojunction interface is crucial to achieving advanced thermal management for gallium nitride-based high electron mobility transistor devices. The current research primarily focuses on material enhancements and microstructure design at the interfaces of epitaxial layers, buffer layers, and substrates, such as the GaN/SiC interface and GaN/AlN interface. Yet, the influence of different concentrations of Al/Ga atoms and interface roughness on the interfacial thermal conductance (ITC) of AlGaN/GaN interface, the closest interface to the hot spot, is still poorly understood. Herein, we focus on the rough AlGaN/GaN interface and evaluate the changes in ITC under different Al–Ga atomic concentrations and interface roughness using atomistic simulations. When the interface is completely smooth and AlGaN and GaN are arranged according to common polarization characteristic structures, the ITC gradually increases as the proportion of Al atoms decreases. When the proportion of Al atoms is reduced to 20%–30%, the impact of the interface structure on heat transfer is almost negligible. For interface models with different roughness levels, as the interface roughness increases, the ITC drops from 735.09 MW m−2 K−1 (smooth interface) to 469.47 MW m−2 K−1 by 36.13%. The decrease in ITC is attributed to phonon localization induced by rough interfaces. The phonon modes at the interface are significantly different from those in bulk materials. The degree of phonon localization is most pronounced in the frequency range that contributes significantly to heat flux. This work provides valuable physical insights into understanding the thermal transfer behaviors across the rough AlGaN/GaN interfaces.
... The parameters of Al-Ga-N SW potential are shown in Table 1. More details can be found in references [24,25,30,31]. Table 1. ...
... Table 1. Stillinger-Weber potential parameters for the Al-Ga-N systems [30,31]. ...
... AlN or GaN often serves as the buffer layer for growing AlGaN due to the small lattice mismatch between them [32]. The growth model of AlGaN on AlN was established by referring to the modeling method in reference [30,31]. Dai et al. [33][34][35] developed a numerical model for the stresses and other properties of AlN films grown on a Si(111) substrate. ...
Article
Full-text available
Aluminum gallium nitride (AlGaN) is a nanohybrid semiconductor material with a wide bandgap, high electron mobility, and high thermal stability for various applications including high-power electronics and deep ultraviolet light-emitting diodes. The quality of thin films greatly affects their performance in applications in electronics and optoelectronics, whereas optimizing the growth conditions for high quality is a great challenge. Herein, we have investigated the process parameters for the growth of AlGaN thin films via molecular dynamics simulations. The effects of annealing temperature, the heating and cooling rate, the number of annealing rounds, and high temperature relaxation on the quality of AlGaN thin films have been examined for two annealing modes: constant temperature annealing and laser thermal annealing. Our results reveal that for the mode of constant temperature annealing, the optimum annealing temperature is much higher than the growth temperature in annealing at the picosecond time scale. The lower heating and cooling rates and multiple-round annealing contribute to the increase in the crystallization of the films. For the mode of laser thermal annealing, similar effects have been observed, except that the bonding process is earlier than the potential energy reduction. The optimum AlGaN thin film is achieved at a thermal annealing temperature of 4600 K and six rounds of annealing. Our atomistic investigation provides atomistic insights and fundamental understanding of the annealing process, which could be beneficial for the growth of AlGaN thin films and their broad applications.
... Moreover, phonon thermal conductivity-mean free path spectra of UWBG materials obtained through experimental and theoretical approaches can be used the predict size dependence of thermal conductivity [181,210]. Finally, the h BD s between b-Ga 2 O 3 / diamond [132], i-Ga 2 O 3 /metal [133], and AlN/AlGaN [211] interfaces have been obtained using a variety of experimental and theoretical approaches. These findings generally show that the already low thermal conductivity of UWBG materials is further reduced in their thin film form; when combined with the low h BD between these materials and their substrates, a thermal bottleneck can form and result in inadequate heat dissipation. ...
Article
Full-text available
This review introduces relevant nanoscale thermal transport processes that impact thermal abatement in power electronics applications. Specifically, we highlight the importance of nanoscale thermal transport mechanisms at each layer in material hierarchies that make up modern electronic devices. This includes those mechanisms that impact thermal transport through: (1) substrates, (2) interfaces and 2-D materials and (3) heat spreading materials. For each material layer, we provide examples of recent works that (1) demonstrate improvements in thermal performance and/or (2) improve our understanding of the relevance of nanoscale thermal transport across material junctions. We end our discussion by highlighting several additional applications that have benefited from a consideration of nanoscale thermal transport phenomena, including RF electronics and neuromorphic computing.
... After proper SiC surface treatment via gas etching, subsequent optimized growth conditions are also required to obtain high-quality AlGaN epilayers on SiC. Since Al adatoms have relatively low surface mobility [75,76], 3D AlN islands are frequently formed at the initial stage and coalesce incoherently afterwards, generating high-density edge dislocations at the grain boundaries [62]. On the contrary, proper growth conditions can enhance the lateral expansion of 3D islands, leading to the bending and annihilation of TDs inside the AlN epilayers. ...
Article
Rapid advancement of wide bandgap AlGaN semiconductor materials offers tremendous opportunities in the field of ultraviolet (UV) optoelectronics for a wide range of advanced applications. Additionally, SiC has large bandgap and excellent material properties, also making itself a suitable material for UV photodetection. More importantly, high-quality AlGaN alloys can be epitaxially grown on SiC substrates because of the very small lattice mismatch between them (less than 1%), which enables a possible monolithic integration of those two materials and allows us to take advantage of their material and physical properties to realize high-performance UV optoelectronics and eventually the integrated UV photonics systems. Herein, we review recent progress in the development of UV optoelectronics based on AlGaN-SiC platform, mainly focusing on: (1) the growth strategies and material characterizations of AlGaN epilayers on SiC; (2) the fabrication and performance evaluation of UV optoelectronic devices built on the platform, including UV LEDs/lasers and UV photodetectors. Thereafter, we briefly discuss the initial efforts in the pursuit of monolithic integration of those UV optoelectronic devices. Finally, the challenges and potential advances associated with individual UV optoelectronic components as well as UV integrated photonics system on the prosperous AlGaN-SiC platform are outlined, providing insights and perspectives for possible device- and system-level innovation in future.
... For nanomaterials, it is also found to play a critical role in changing conventional bulk properties, such as elastic modulus [5], piezoelectricity [6], thermal conductivity [7], etc. Thus, surface property is important for the determination of material properties and structure performances [8][9][10][11]. The concept of surface free energy (called surface energy for short) was first introduced in fluid mechanics for studying surface phenomena. It is equal to the reversible work per unit area needed to create a surface, which is also widely referred to as surface tension in fluid mechanics. ...
Article
Full-text available
Surface property is an important factor that is widely considered in crystal growth and design. It is also found to play a critical role in changing the constitutive law seen in the classical elasticity theory for nanomaterials. Through molecular static simulations, this work presents the calculation of surface properties (surface energy density, surface stress and surface stiffness) of some typical cubic and hexagonal crystals: face-centered-cubic (FCC) pure metals (Cu, Ni, Pd and Ag), body-centered-cubic (BCC) pure metals (Mo and W), diamond Si, zincblende GaAs and GaN, hexagonal-close-packed (HCP) pure metals (Mg, Zr and Ti), and wurzite GaN. Sound agreements of the bulk and surface properties between this work and the literature are found. New results are first reported for the surface stiffness of BCC pure metals, surface stress and surface stiffness of HCP pure metals, Si, GaAs and GaN. Comparative studies of the surface properties are carried out to uncover trends in their behaviors. The results in this work could be helpful to the investigation of material properties and structure performances of crystals.
... Similar study results were obtained by Lundin et al. and Touzi et al. 53,43 Furthermore, Lundin et al. also found that although the Al component decreased with the rise of III-nitride, the rate of decrease in the high ammonia atmosphere was significantly faster than that in the low. In addition, as the ratio of the III-nitride flow rate rose in the total gas, the growth rate also grews, 26,47,49,55,56 thus it was difficult to achieve rapid growth of the AlGaN layer and obtain a high Al component simultaneously by adjusting the III-nitride flow rate. Figure 6 demonstrated the effect of the TMAl/III flow rate ratio on the growth rate of AlGaN. ...
... the layer grown by MOCVD, gas phase reactions and fluid transport determined the species, concentration and transport rate of the particles that reached the surface of the substrate, but the quality of layer growth, including surface morphology, impurity component and defect distribution depended to a large extent on the interaction between the gas phase precursor and the surface of the substrate, namely the surface reaction, which included adsorption, desorption, surface diffusion, adsorption of particles into the crystal lattice. 56 When the temperature was high or the long speed was slow, the particles reaching the surface could quickly diffuse from the adsorption site to the growth kinetics or corner, and then merged into the crystal lattice, namely two-dimensional kinetics flow growth. When the temperature was low, the growing velocity was faster or the chemical bond between the adsorbed particles and the adsorption site was stronger, the particles reaching the surface could not rapidly diffuse from the adsorption site to the step or the corner, so that three-dimensional volmer-weber occurred, causing a large number of dislocations and uneven distribution of grain boundary and impurities. ...
Article
Full-text available
Due to the broad application prospects of optoelectronic devices and microwave devices at high temperature and power, the process of Metal Organic Chemical Vapor Deposition (MOCVD) of AlGaN of the key material AlGaN has been extensively researched in the past 30 years. In order to enhance the quality of AlGaN layers, researchers continuously analyzed their growth mechanism and optimized the growth process through experimental and theoretical studies. In this work, based on reviewing previous studies, we summarize the research progress for AlGaN grown by MOCVD and discuss the existing problems and future research priorities.
... In this study, we perform MD simulations to investigate the growth of AlxGa1−xN films on AlN template by Large-scale Atomic/Molecular Massively Parallel Simulator (LAMMPS) [18]. The (0001) Al-terminated AlN is chosen as the template because it has been proven that AlGaN film grown on (0001) Al-terminated surface has better crystal quality than that grown on (000-1) Nterminated surface [19,20]. The effects of growth temperature and film thickness on the dislocation of deposited AlGaN film are investigated. ...
Article
Full-text available
In this article, we study the deposition of AlGaN film on AlN template by molecular dynamics (MD) simulations. The effects of growth temperature and film thickness on the dislocation of deposited AlGaN film are simulated and studied. The atomic structure of deposited AlGaN film is also investigated. We find that the dislocations usually occur at the interface between AlN template and AlGaN film and then extend towards the growth direction. The dislocation density decreases with the increase of AlGaN film thickness, which indicates that increasing the thickness of deposited AlGaN film to a certain extent is beneficial to reducing dislocation. In addition, increasing the growth temperature can also effectively reduce the dislocation in deposited AlGaN film. Furthermore, the crystallinity of deposited AlGaN film could be improved by increasing the growth temperature. This is consistent with the dislocation discussion. The mobility of adatoms increases as the growth temperature increases. So it is easier for adatoms to find their ideal lattice points at higher temperature. Thus the dislocation and other defects can be effectively reduced and the crystal quality of deposited AlGaN film could be improved.
Article
Full-text available
The structure and thermal boundary conductance of the wurtzite GaN/AlN (0001) interface are investigated using molecular dynamics simulation. Simulation results with three different empirical interatomic potentials have produced similar misfit dislocation networks and dislocation core structures. Specifically, the misfit dislocation network at the GaN/AlN interface is found to consist of pure edge dislocations with burger vector of 1 3 ⁄ 〈12 ̅ 10〉 and the misfit dislocation core has an 8-atom ring structure. Although different interatomic potentials lead to different dislocation properties and thermal conductance values, all have demonstrated a significant effect of misfit dislocations on the thermal boundary conductance of the GaN/AlN (0001) interface.