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H. Uzu, private communication.
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28
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0001087855
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The Compton profile anisotropy is often invoked to highlight relatively small oscillating terms reflecting coherence properties of the ground state wave function. See e.g. E.D. Isaacs, A. Shukla, P.M. Platzman, D.R. Hamann, B. Barbiellini, C.A. Tulk, Phys. Rev. Lett. 82 (1999) 600. In magnetite, the [1 0 0] profile is dominated by atomic d-like behavior and it does not contain a significant interference term from the nearest neighbor Fe-Fe overlap. Therefore, in the [1 0 0]-[1 1 0] difference profile, the [1 0 0] profile essentially allows us to subtract an underlying atomic contribution to the [1 1 0] profile and to thus highlight interference effects in the [1 1 0] profile.
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29
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34447531377
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[1 0 0] 〉 as background does not introduce any spurious features in the anisotropy defined by Eq. (3).
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31
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34447522915
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BB = 5.61 a . u . yields the good fit shown in Fig. 3.
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32
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34447532907
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The error in our values of f is estimated to be ± 0.02.
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33
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34447522583
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max.
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34
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34447524466
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mag (p) (in particular the peak at 1.12 a.u.) which involve the same area as the negative contributions.
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35
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