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Photo EPR Study of Trapping and Recombination Processes in Semi-Insulating 4H-SiC Crystals as Function of Temperature

Published online by Cambridge University Press:  21 March 2011

E.N. Kalabukhova
Affiliation:
Institute of Semiconductor Physics, NASU, Kiev, Ukraine
S.N. Lukin
Affiliation:
Institute of Semiconductor Physics, NASU, Kiev, Ukraine
A. Saxler
Affiliation:
Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson AFB, U.S.A.
W.C. Mitchel
Affiliation:
Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson AFB, U.S.A.
S R. Smith
Affiliation:
Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson AFB, U.S.A.
J.S. Solomon
Affiliation:
Air Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson AFB, U.S.A.
A.O. Evwaraye
Affiliation:
University of Dayton, Physics Department, Dayton, U.S.A.
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Abstract

Photo-Electron Paramagnetic Resonance (photo-EPR) measurements of semi-insulating (s.-i.) 4H SiC have been made at 37 GHz including photo excitation and photo quenching techniques in the temperature interval from 77 K to 50 K. At T = 77 K in the dark the EPR spectrum consists of a low intensity line due to boron on the cubic lattice site and a single line with isotropic g = g = 2.0025 due to a carbon-related surface defect. During illumination with ultraviolet light the EPR lines of hexagonal boron and cubic nitrogen appear in the EPR spectrum and persist after the illumination is removed. Subsequent illumination of the sample with sub-band gap, visible, light resulted in the quenching of the EPR lines from nitrogen and appearance of the IP1EPR line with g = 2.0048, g = 2.0030 caused by direct transfer of electrons from nitrogen donor to the P1 center. The lifetime of the photo-generated carriers trapped by the P1 centers is found to be more than 15- 20 hours after the photo-excitation was turned off. The deep donor P1 local center is suggested to be the as yet unidentified deep level located at EC – 1.1 eV which pins the Fermi level in this sample at this energy in the dark. As the temperature is lowered from 77K and the quasi Fermi level positions reach shallow donor and acceptor states, an additional EPR line, ID, with g = 2.0063, g = 2.0006, appears at 50 K in the excitation EPR spectrum and is attributed to the antisite defect Sic with an energy level shallower than nitrogen. At the same time the ratio of the photo-excited EPR line intensities responsible for boron on the cubic and hexagonal sites, IkB:IhB, returns to the value observed at 77 K and becomes equal to 0.4 at 50 K, showing that the concentration of boron in the hexagonal site is higher than on the cubic site.

Type
Research Article
Copyright
Copyright © Materials Research Society 2001

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References

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