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Polarization‐dependent extended x‐ray absorption fine structure measurements of metastable fcc Co on (100) diamond
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11.This beam line is equipped with a fixed exit double crystal monochromator that uses (311) Si crystals thus, no harmonic rejection was required.
12.E. A. Stern, in X-Ray Absorption: Basic Principles of EXAFS, SEXAFS, and XANES, edited by D. C. Koningsberger and R. Prins (Wiley, New York, 1988), Chap. 1.
13.At least two successive energy scans were collected at a minimum of three slightly different azimuthal angles to eliminate the Bragg reflections from the diamond substrate. A different azimuthal angle was obtained by rotating the sample about an axis normal to the sample by ∼2°. For more information see K. M. Kemner, Z. Wang, R. A. Mayanovic, and B. A. Bunker, Nucl. Instrum. Methods B 71, 345 (1992).
14.The data in Fig. 2, for values of 3.0–16.0 were Fourier transformed with a 0.5 modified Hanning window function to reduce truncation ripple. For further details, see D. E. Sayers and B. A. Bunker, in X-Ray Absorption: Basic Principles of EXAFS, SEXAFS, and XANES, edited by D. C. Koningsberger and R. Prins (Wiley, New York, 1988), Chap. 6.
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16.For further details concerning the collinear multiple scattering effect for hcp Co see, K. M. Kemner, V. G. Harris, W. T. Elam, and J. C. Lodder, Mater. Res. Soc. Symp. Proc. 375, 21 (1995).
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