28 June 2015 to 3 July 2015
Africa/Johannesburg timezone
SAIP2015 Proceeding published on 17 July 2016

Determination of the band gap of AlGaN epilayers by FTIR reflectance spectroscopy

30 Jun 2015, 16:10
1h 50m
Board: A.034
Poster Presentation Track A - Division for Physics of Condensed Matter and Materials Poster1

Speaker

Ms Bereneice Sephton (NMMU)

Level for award<br>&nbsp;(Hons, MSc, <br> &nbsp; PhD, N/A)?

Hons

Apply to be<br> considered for a student <br> &nbsp; award (Yes / No)?

No

Please indicate whether<br>this abstract may be<br>published online<br>(Yes / No)

Yes

Would you like to <br> submit a short paper <br> for the Conference <br> Proceedings (Yes / No)?

No

Abstract content <br> &nbsp; (Max 300 words)<br><a href="http://events.saip.org.za/getFile.py/access?resId=0&materialId=0&confId=34" target="_blank">Formatting &<br>Special chars</a>

AlGaN alloys are used in high-power, high-temperature and high-frequency devices such as field-effect transistors, UV-light emitting LED’s and laser diodes. Different electrical and optical properties can be obtained by varying the alloy composition of AlxGa1-xN by changing the amount of Al in the alloy. It is therefore essential to characterize the alloys to establish the various physical properties as a function of Al content.

Optical characterization is preferred as this technique has the advantage of being non-contact and non-destructive. In this work, infrared reflection spectroscopy was employed to evaluate 5 AlxGa1-xN epilayers grown with varying Al content by metalorganic vapour phase deposition (MOCVD) on sapphire substrates. Samples were investigated using a Bruker V80 FTIR/Raman instrument, in the wavenumber range 50000 – 10 cm-1. Measurements were taken at room temperature at 8 cm-1 resolution, using a Pike 10Spec specular reflection attachment, taking 100 scans. The band gap of the respective samples is obtained from the obtained reflectance spectrum at the transition between the interference fringes and a straight line in the spectra. In addition, the thickness of the layers could be obtained from the interference fringes. Results obtained indicated that the band gap varied between 3.6 and 5.1 eV, while the epilyer thicknesses were between 0.9 and 1.3 m. The results corresponded very well with data obtained by techniques such as photoluminescence and growth parameters.

Main supervisor (name and email)<br>and his / her institution

JAA Engelbrecht Japie.Engelbrecht@nmmu.ac.za

Primary author

Co-authors

Presentation Materials

There are no materials yet.