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S. Nakamura, M. Senoh, and T. Mukai, Appl. Phys. Lett. 62, 2390 (1993); Nakamura, T. Mukai, and M. Senoh, Appl. Phys. Lett. 64, 1687 (1994); M. A. Khan, J. N. Kuznia, A. R. Bhattarai, and D. T. Olson, Appl. Phys. Lett. 62, 1786 (1993); H. Morkoç and S. N. Mohammad, Science 267, 51 (1995); H. Morkoç, S. Strite, G. B. Gao, M. E. Lin, B. Sverdlov, and M. Burns, J. Appl. Phys. 76, 1363 (1994).
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D. E. Cox, in Handbook on Synchrotron Radiation, edited by G. S. Brown and D. E. Moncton (Publisher, City, 1991), Vol. 3, p. 155.
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The fit improves significantly by allowing two different peak-widths. The fitted shoulder peak turned out to be broader [FWHM=0.034(7)°] than the main peak [FWHM=0.0285(8)°].
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The fit improves significantly by allowing two different peak-widths. The fitted shoulder peak turned out to be broader [FWHM=0.034(7)°] than the main peak [FWHM=0.0285(8)°].
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9
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21544456158
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L̄=0.94λ/FWHM(2θ)cosθ; see, for example, B. E. Warren, in X-ray Diffraction (Addison-Wesley, Reading, MA, 1969).
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L̄=0.94λ/FWHM(2θ)cosθ; see, for example, B. E. Warren, in X-ray Diffraction (Addison-Wesley, Reading, MA, 1969).
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10
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21544439635
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A super-Lorentzian function is a pseudo-Voigt function with a mixing parameter η> 1.0, η normally varies between 0.0 (pure Gaussian) and 1.0 (pure Lorentzian).
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A super-Lorentzian function is a pseudo-Voigt function with a mixing parameter η> 1.0, η normally varies between 0.0 (pure Gaussian) and 1.0 (pure Lorentzian).
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11
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21544464374
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21544445949
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J. J. Song and H. Morkoç (unpublished).
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J. J. Song and H. Morkoç (unpublished).
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