Structural and Optical Properties of GaN Film on Copper and Graphene/Copper Metal Foils Grown by Laser Molecular Beam Epitaxy

2020 ◽  
Vol 20 (6) ◽  
pp. 3929-3934 ◽  
Author(s):  
C. Ramesh ◽  
P. Tyagi ◽  
S. Bera ◽  
S. Gautam ◽  
Kiran M. Subhedar ◽  
...  

We report the direct growth of crystalline GaN on bare copper (Cu) and monolayer-graphene/Cu metal foils using laser molecular beam epitaxy technique at growth temperature of 700 °C. The surface morphology investigated with field emission scanning electron microscopy revealed that the size of GaN grains for film grown on bare Cu falls in range of 90 to 160 nm whereas large grains with size of ˜200 to 600 nm was obtained for GaN grown on graphene/Cu foil under similar growth condition. The transverse optical mode of cubic GaN and E2 (high) phonon mode for wurtzite GaN phases were obtained on the GaN film grown on Cu and graphene/Cu metal foils as deduced by Raman spectroscopy. The photoluminescence (PL) spectroscopy studies showed that the near band edge emission peaks for GaN on Cu and graphene/Cu consist two major peaks at 3.26 and 3.4 eV, corresponding to cubic and wurtzite GaN, respectively. The Raman and PL studies disclosed that the mixed phase growth of GaN occurs on these foils and better structural and optical quality for GaN on graphene/Cu foil. The direct growth of GaN on two dimensional graphene on polycrystalline metal foils is beneficial various transferrable and flexible opto-electronics device applications.

AIP Advances ◽  
2013 ◽  
Vol 3 (9) ◽  
pp. 092109 ◽  
Author(s):  
S. S. Kushvaha ◽  
M. Senthil Kumar ◽  
K. K. Maurya ◽  
M. K. Dalai ◽  
Nita D. Sharma

2002 ◽  
Vol 299 (1) ◽  
pp. 79-84 ◽  
Author(s):  
M Xu ◽  
C.X Liu ◽  
H.F Liu ◽  
G.M Luo ◽  
X.M Chen ◽  
...  

2020 ◽  
Vol 20 (6) ◽  
pp. 3866-3872
Author(s):  
Ch. Ramesh ◽  
J. Pandey ◽  
P. Tyagi ◽  
A. Soni ◽  
M. Senthil Kumar ◽  
...  

The optical properties of laser-assisted molecular beam epitaxy grown homo-epitaxialGaN nanowall networks (NWNs) were investigated using power dependent photoluminescence (PL) spectroscopy and compared with homo-epitaxial GaN thin film. The pore size and tip width of GaN NWN sample is ˜120–180 nm and 10–15 nm, respectively. The ultraviolet-visible spectroscopy study shows that the GaN NWNs have low optical light reflection and minimum Fabry-Perot cavity effect than GaN film. The room temperature PL spectroscopy reveals that the GaN NWNs possesses enhanced band gap of 3.51 eV with blue shift of 90 meV than the GaN film (3.42 eV). The excitation density dependent PL spectroscopy measurements reveal that the GaN NWNs nanowall and near band emission (NBE) peak position and its linewidth invariant. The intensity of NBE peak for GaN film and nanowalls varies linearly whereas NBE to defect related yellow luminescence peak intensity ratio shows a non-linear variation on the excitation density. The excitation density in PL measurements plays a key role when the sample quality compared on the basis of PL data.


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