Effect of deposition conditions on properties of nitrogen rich-InN nanostructures grown on anisotropic Si (110)
Introduction
Indium nitride (InN) has a wurtzite crystal structure with a small band gap of 0.7 eV [1]. InN is an interesting semiconductor material because of its potential applications in optoelectronic devices, such as high efficiency solar cells, high electron mobility sensors, and transistors [2], [3], [4], [5]. However, InN has received less attention compared with gallium nitride (GaN) and aluminum nitride primarily because of difficulties inherent in the preparation of its stoichiometric form. In addition, high-grade single crystal InN is difficult to grow due to its low dissociation temperature and less suitable substrates. Due to its low dissociation temperature, InN film should deposit at low temperatures to avoid N atom re-evaporation [6], [7]. Reactive sputtering is one of the most promising techniques of producing InN from the viewpoint of low-temperature film growth. InN layer synthesis on sapphire and glass substrates using reactive sputtering has been previously reported [8], [9], and InN deposition on different Si substrate orientations has been recently investigated [10], [11], [12], [13]. The anisotropic Si(110) surface offers a unique orientation for GaN films compared to Si(001) where it can decrease the defect density and tensile stress for film cracking [14].
Nevertheless, few organized studies of nanocrystalline InN grown on anisotropic Si (110) substrate by radio frequency (RF) sputtering have been reported thus far [15], [16]. In the current study, InN nanostructures were successfully deposited by reactive RF magnetron sputtering on anisotropic Si(110) substrates. The structure and optical properties of the resulting films were investigated under various deposition gas concentrations, RF powers, and substrate temperatures.
Section snippets
Experimental
InN films were deposited by the reactive RF sputtering of a pure indium (In) target (99.99%), in an argon (Ar) and nitrogen (N2) atmosphere. Prior to each deposition process, the In target was cleaned with a 10 min pre-sputter by Ar plasma in order to remove any previous target surface contamination. The base pressure was around 2×10−5 mbar and the deposition was maintained at constant pressure of approximately 8×10−3 mbar. Si(110) substrates were cleaned before putting in the substrate holder.
Effects of RF power
Since, the sputtered films are mostly amorphous; the growth mechanism of crystalline InN using the sputtering technique at room temperature without post-deposition annealing is important achievement which is studied under different deposition conditions in this paper. InN films were deposited on Si(110) substrates at various RF powers to investigate the effects of applied power on the film characteristics.
Fig. 1 shows the deposition rate of the deposited InN films as a function of applied RF
Conclusions
A comprehensive study on the effects of deposition conditions on the characteristics of InN film deposited on Si(110) by reactive RF sputtering was presented. Since the sputtered films are mostly amorphous, the growth mechanism of crystalline InN using the sputtering technique at room temperature without post-deposition annealing is important achievement. Under different deposition conditions, wurtzite nanocrystalline InN films with slightly N-rich and preferred growth orientation of InN(10 1)
Acknowledgments
Financial support from PRGS Grant no. 1001/PFIZIK/844071 and University Sains Malaysia are gratefully acknowledged.
References (26)
- et al.
Superlattices Microstruct.
(2005) Scr. Mater.
(2010)Vacuum
(2004)- et al.
Thin Solid Films
(1998) J. Alloy. Compd.
(2009)- et al.
Vacuum
(2014) Mater. Sci. Semicond. Process.
(1999)- et al.
Mater. Sci. Semicond. Process.
(2013) Appl. Phys. Lett.
(2012)IEEE J. Sel. Top. Quantum Electron.
(2011)
J. Appl. Phys.
Phys. Rev. B
J. Appl. Phys.
Cited by (8)
Effect of different EBL structures on deep violet InGaN laser diodes performance
2016, Optics and Laser TechnologyCitation Excerpt :Recently, III-Nitride materials have attracted significant interest because of their specific properties including wide bandgap energy, broad coverage of the electromagnetic spectrum, and high thermal stability, as well as their wide application especially in optoelectronics as light sources, including full color display, illumination, high-density data storage, laser printing, biological agent detection systems, and medical applications [1–5].
Structural, Electrical and Optical Properties of Sputtered-Grown InN Films on ZnO Buffered Silicon, Bulk GaN, Quartz and Sapphire Substrates
2018, Journal of Electronic MaterialsStructure and photoluminescence properties of InN films grown on porous silicon by MOCVD
2017, Optoelectronics Letters[0001]-Oriented InN nanoleaves and nanowires: Synthesis, growth mechanism and optical properties
2016, Acta Metallurgica Sinica (English Letters)