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Figure 3
(a) The presence and absence of the b.c.c. (110) reflection at T = 1173 K (open squares □) and at T = 1193 K (crosses +). These measurements were obtained from the Fe powder using an X-ray beam of λ = 1.0 Å. The solid line is the fit of a pseudo-Voigt function to the data (□). (b) The absence and presence of the f.c.c. (200) reflection at T = 1173 K (open squares □) and T = 1193 K (crosses +). The solid line is the fit of a pseudo-Voigt function to the data (+).

Journal logoJOURNAL OF
SYNCHROTRON
RADIATION
ISSN: 1600-5775
Volume 5| Part 3| May 1998| Pages 929-931
https://doi.org/10.1107/S0909049597015513
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