Abstract
This work discusses the frequency shift of Raman mode A1(LO) for InGaN epitaxial layers grown on polar (0002) and non-polar (11–20) planes concerning strain state, indium composition, and the probe excitation energy. Furthermore, it proposes MOCVD growth conditions to grow fully relaxed polar and non-polar InGaN layers, without indium droplets formation. Then, using the probe excitation energies of 2.33 eV and 2.68 eV, Raman measurements exhibited phonon mode A1(LO) frequency shift in polar and non-polar InGaN. Besides, theoretical calculations showed that for x < 0.20, and changing the excitation energy from 2.33 to 2.68 eV, the expected frequency shift is less or equal to 15 cm−1. Also, the XRD spectra exhibited two different indium compositions for non-polar a-plane InGaN and one composition for polar c-plane InGaN. According to XRD, for non-polar a-plane InGaN, the frequency shift measured corresponds to an indium composition gradient along the growth direction and the probe excitation energy change. On the other hand, for polar c-plane InGaN, the frequency shift measured is attributed to the probe excitation energy change. Also, AFM showed that there is an excellent island coalescence in GaN and InGaN epitaxial growth. The average surface roughness for polar InGaN was 75.678 nm and was 61.216 nm for non-polar InGaN. Moreover, these values are ten times smaller than their peak-to-peak distance, and the growth follows the Stranski–Krastanov model. FWHM for all samples corresponds to a total dislocations density of ~ 109/cm2 near the surface.
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References
S.R. Routray, T.R. Lenka, CSIT 6(1), 83–96 (2018)
S. Almosni et al., Sci. Technol. Adv. Mater. 19(1), 336–369 (2018)
S.C. Jain, M. Willander, J. Narayan, R. Van Overstraeten, J. Appl. Phys. 87, 965 (2000)
G.B. Stringfellow, J. Crystal Growth 468, 11–16 (2017)
F.K. Yam, Z. Hassan, Superlattices and Microstruct. 43, 1–23 (2008)
R. Luo, P. Xiang et al., Jpn. J. Appl. Phys. 50, 105501 (2011)
J. Wei Ho, L. Zhang, Q. Wee, et. al., J. Crystal Growth 383: 1- 8 (2013).
M. Wei, X. Wang et al., Mater. Sci. Semicond. Process. 14, 97–100 (2011)
B. Ting Liu, P. Ma, X.-L. Li, J.-X. Wang and J.-M. Li, Chin. Phys. Lett. 34:5 (2017)
E. Arslan, M.K. Ozturk et al., J. Phys. D 41, 155317 (2008)
K. Matsumoto, T. Ono, Y. Honda, S. Murakami, M. Kushimoto, H. Amano, Jpn. J. Appl. Phys. 57, 091001 (2018)
H. Çakmak, E. Arslan, M. Rudzinski, P. Demirel, H.E. Unalan, W. Strupinski, R. Turan, M. Örtürk, E. Özbay, J. Mater. Sci. Mater. Electron. 25, 3652–3658 (2014)
M. Meyer, J. Stellmach, C. Meissner, M. Pristovsek, M. Kneissi, J. Crystal Growth 310, 4913–4915 (2008)
S. Pereira, M.R. Correia, E. Pereira, K.P. O’Doneell, E. Alves, A.D. Sequeira, N. Franco, I.M. Watson, C.J. Deatcher, Appl. Phys. Lett. 80, 3913 (2002)
A.G. Bhuiyan, A. Mihara, T. Esaki, K. Sugita, A. Hashimoto, A. Yamamoto, N. Watanabe, H. Yokoyama, N. Shigekawa, Phys. Status Solidi C 9(3–4), 670–672 (2012)
A. Kursat Bilgili, Ö. Akpinar, G. Kurtulus, M. Kemal Ozturk, S. Ozcelik and E. Ozbay, J. Mater. Sci. 29: 12373–13380 (2018)
J.G. Kim, Y. Kamei, A. Kimura, N. Hasuike, H. Harima, K. Kisoda, T. Hotta, K. Sasamoto, A. Yamamoto, Phys. Status Solidi C 9(3–4), 730–732 (2012)
M. Azadmand, E. Bonera, D. Chrastina, S. Bietti, S. Tsukamoto, R. Nötzel and S. Sanguinetti, Jpn. J. Appl. Phys. 58: SC1020 (2019).
Y. Guo, X.L. Liu et al., Appl. Surface Sci. 256, 3352–3356 (2010)
D. Alexson, L. Bergman, R.J. Nemanich, M. Dutta, M.A. Stroscio, C.A. Parker, S.M. Bedair, N.A. El-Masry, F. Adar, J. Appl. Phys. 89, 798 (2001)
M. Kumar, M. Becker, T. Wernicke, R. Singh, Appl. Phys. Lett. 105, 142106 (2014)
M.R. Correia, S. Pereira, E. Pereira, J. Frandon, E. Alves, Appl. Phy. Lett. 83, 4761 (2003)
S. Hernández, R. Cuscó, D. Pastor, L. Artús, K.P. O’Donnell, R.W. Martin, I.M. Watson, Y. Nanishi, E. Calleja, J. App. Phys. 98, 013511 (2005)
C. Roder, S. Einfeldt et al., J. App. Phys. 100, 103511 (2006)
M. Azadmand et. al., Jpn. J. Appl. Phys. 58: SC1020 (2019).
S. Lazic, M. Moreno, J.M. Calleja, A. Trampert, K.H. Ploog, F.B. Naranjo, S. Fernandez, E. Calleja, Appl. Phys. Lett. 86, 061905 (2005)
J. S. Arias-Cerón, H. Vilchis, D.M. Hurtado-Castañeda, V.M. Sánchez-R, Mater. Sci. Semicond. Process. 74: 98–101 (2018).
H. Vilchis, V.M. Sánchez-R, Mater. Sci. Semicond. Process. 37: 68–72 (2015)
H. Vilchis, V.M. Sánchez-R., A. Escobosa, Thin Solid Films 520 (16) 5191–5194 (2012)
H. Vilchis, V.M. Sánchez-R., A. Escobosa, J. Phys. 167: 012–049 (2009)
H. Vilchis. Víctor M. Sánchez-R., A. Escobosa, 5th International Conference on Electrical Engineering, Computing Science and Automatic Control (CCE 2008).
Acknowledgements
Thanks to Consejo Nacional de Ciencia y Tecnología de México (CONACyT) for its financial support (PNPC) to Ph. D. program at Solid State Electronics Section, Electrical Engineering Department, CINVESTAV. Also, the authors would like to thank D. Ramírez for his technical assistance in the MOCVD system, A. Tavira for the XRD measurements, and M. Galvan and M. Avendaño for their technical support in Raman and AFM measurements.
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Marín-García, C.A., Cerón, J.S.A. & Sánchez-R, V.M. Longitudinal optical Raman mode A1 to calculate the indium molar fraction of epitaxial InGaN layers grown by LP-MOCVD on polar and non-polar planes. J Mater Sci: Mater Electron 31, 7455–7460 (2020). https://doi.org/10.1007/s10854-020-02966-y
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DOI: https://doi.org/10.1007/s10854-020-02966-y