A study into the optimal deposition temperature for ultra-thin La2O3/Ge and Y2O3/Ge gate stacks has been conducted in this paper with the aim to tailor the interfacial layer for effective passivation of the Ge interface. A detailed comparison between the two lanthanide oxides (La2O3 and Y2O3) in terms of band line-up, interfacial features, and reactivity to Ge using medium energy ion scattering, vacuum ultra-violet variable angle spectroscopic ellipsometry (VUV-VASE), X-ray photoelectron spectroscopy, and X-ray diffraction is shown. La2O3 has been found to be more reactive to Ge than Y2O3, forming LaGeOx and a Ge sub-oxide at the interface for all deposition temperature studied, in the range from 44 °C to 400 °C. In contrast, Y2O3/Ge deposited at 400 °C allows for an ultra-thin GeO2 layer at the interface, which can be eliminated during annealing at temperatures higher than 525 °C leaving a pristine YGeOx/Ge interface. The Y2O3/Ge gate stack deposited at lower temperature shows a sub-band gap absorption feature fitted to an Urbach tail of energy 1.1 eV. The latter correlates to a sub-stoichiometric germanium oxide layer at the interface. The optical band gap for the Y2O3/Ge stacks has been estimated to be 5.7 ± 0.1 eV from Tauc-Lorentz modelling of VUV-VASE experimental data. For the optimal deposition temperature (400 °C), the Y2O3/Ge stack exhibits a higher conduction band offset (>2.3 eV) than the La2O3/Ge (∼2 eV), has a larger band gap (by about 0.3 eV), a germanium sub-oxide free interface, and leakage current (∼10−7 A/cm2 at 1 V) five orders of magnitude lower than the respective La2O3/Ge stack. Our study strongly points to the superiority of the Y2O3/Ge system for germanium interface engineering to achieve high performance Ge Complementary Metal Oxide Semiconductor technology.
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21 March 2014
Research Article|
March 17 2014
Ge interface engineering using ultra-thin La2O3 and Y2O3 films: A study into the effect of deposition temperature
I. Z. Mitrovic;
I. Z. Mitrovic
a)
1
Department of Electrical Engineering & Electronics, University of Liverpool
, Brownlow Hill, Liverpool L69 3GJ, United Kingdom
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M. Althobaiti;
M. Althobaiti
2
Department of Physics and Stephenson Institute for Renewable Energy, University of Liverpool
, Liverpool L69 7ZF, United Kingdom
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A. D. Weerakkody;
A. D. Weerakkody
1
Department of Electrical Engineering & Electronics, University of Liverpool
, Brownlow Hill, Liverpool L69 3GJ, United Kingdom
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V. R. Dhanak;
V. R. Dhanak
2
Department of Physics and Stephenson Institute for Renewable Energy, University of Liverpool
, Liverpool L69 7ZF, United Kingdom
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W. M. Linhart;
W. M. Linhart
2
Department of Physics and Stephenson Institute for Renewable Energy, University of Liverpool
, Liverpool L69 7ZF, United Kingdom
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T. D. Veal;
T. D. Veal
2
Department of Physics and Stephenson Institute for Renewable Energy, University of Liverpool
, Liverpool L69 7ZF, United Kingdom
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N. Sedghi;
N. Sedghi
1
Department of Electrical Engineering & Electronics, University of Liverpool
, Brownlow Hill, Liverpool L69 3GJ, United Kingdom
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S. Hall;
S. Hall
1
Department of Electrical Engineering & Electronics, University of Liverpool
, Brownlow Hill, Liverpool L69 3GJ, United Kingdom
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P. R. Chalker;
P. R. Chalker
3
Department of Engineering, University of Liverpool
, Brownlow Hill, Liverpool L69 3GH, United Kingdom
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D. Tsoutsou;
D. Tsoutsou
4
NCSR Demokritos, MBE Laboratory, Institute of Materials Science
, 153 10 Athens, Greece
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A. Dimoulas
A. Dimoulas
4
NCSR Demokritos, MBE Laboratory, Institute of Materials Science
, 153 10 Athens, Greece
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a)
Author to whom correspondence should be addressed. Electronic mail: ivona@liverpool.ac.uk
J. Appl. Phys. 115, 114102 (2014)
Article history
Received:
January 31 2014
Accepted:
February 27 2014
Citation
I. Z. Mitrovic, M. Althobaiti, A. D. Weerakkody, V. R. Dhanak, W. M. Linhart, T. D. Veal, N. Sedghi, S. Hall, P. R. Chalker, D. Tsoutsou, A. Dimoulas; Ge interface engineering using ultra-thin La2O3 and Y2O3 films: A study into the effect of deposition temperature. J. Appl. Phys. 21 March 2014; 115 (11): 114102. https://doi.org/10.1063/1.4868091
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