1999
DOI: 10.1063/1.370625
|View full text |Cite
|
Sign up to set email alerts
|

Effects of growth rate of a GaN buffer layer on the properties of GaN on a sapphire substrate

Abstract: We studied the effects of the growth rate of a GaN buffer layer grown on a GaN epilayer. It was found that this growth rate plays a key role in improving the quality of the GaN film on a sapphire substrate and an optimum growth rate exists that yields the best crystal quality. A GaN film grown on a buffer layer with the optimum growth rate of 18.3 nm/min has an electron Hall mobility of 539 cm2/V s and a dislocation density of approximately 2×108 cm−2. These improvements of GaN film qualities are illustrated b… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

0
13
0
1

Year Published

2004
2004
2020
2020

Publication Types

Select...
6
2
1

Relationship

0
9

Authors

Journals

citations
Cited by 44 publications
(14 citation statements)
references
References 9 publications
0
13
0
1
Order By: Relevance
“…The rapid growth rate of the initial seed crystals causes the threedimensional (3D) island-shaped growth and the randomness of the (0 0 1) plane showing no preferred orientation. For the growth of the heterostructures with a large lattice mismatch (example: GaN or ZnO on sapphire or Si), the structural properties of the initial layers such as buffer layers, significantly affect those of the whole film [15,16]. Similarly, the reason being considered for the random inclination of the ZnO nanorod's [0 0 1] ZnO on a [1 1 1] Si substrate is that the seed crystals had no preferred orientation in the initial stage, or that the (0 0 1) planes were random, which can be confirmed by the DP from the ZnO near the ZnO seed crystal/Si substrate interface, showing the same direction as that shown by the (0 0 2) diffraction spots of the ZnO seed crystal and nanorod, as shown in the insets of Fig.…”
Section: Resultsmentioning
confidence: 99%
“…The rapid growth rate of the initial seed crystals causes the threedimensional (3D) island-shaped growth and the randomness of the (0 0 1) plane showing no preferred orientation. For the growth of the heterostructures with a large lattice mismatch (example: GaN or ZnO on sapphire or Si), the structural properties of the initial layers such as buffer layers, significantly affect those of the whole film [15,16]. Similarly, the reason being considered for the random inclination of the ZnO nanorod's [0 0 1] ZnO on a [1 1 1] Si substrate is that the seed crystals had no preferred orientation in the initial stage, or that the (0 0 1) planes were random, which can be confirmed by the DP from the ZnO near the ZnO seed crystal/Si substrate interface, showing the same direction as that shown by the (0 0 2) diffraction spots of the ZnO seed crystal and nanorod, as shown in the insets of Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Changes in the NL growth parameters such as thickness [8,[12][13][14][15], growth T [16][17][18], growth rate [19][20][21], annealing schedule from low to high T [13,[22][23][24], and extent to which the sapphire surface is exposed to NH 3 prior to NL growth [15,17,25] have all been shown to influence the NL growth and subsequent quality of the high-T GaN layers.…”
Section: Introductionmentioning
confidence: 99%
“…It can be seen that the PSS LED with BAVPC (righthand side of x-axis) exhibits the lowest FWHM of (002) and (102) diffraction peaks as compared to the C-PSS LED (lefthand side of x-axis) and FSS LED with BAVPC (centre of x-axis). The FWHM of (102) diffraction peak is related to the densities of TDs and edge dislocations [31], [32]. In addition, the FWHM of the (002) diffraction peak depends on screw and mixed-type dislocations.…”
Section: Resultsmentioning
confidence: 99%