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85033000128
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V.G. Grachev: Institute of Materials Sciences, 252180 Kiev, Ukraine
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V.G. Grachev: Institute of Materials Sciences, 252180 Kiev, Ukraine
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85033000321
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note
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One may see from Fig. 1 and from Fig. 1 in [20] that the resonance from Fe4/2 at ≈ 320 mT is above the corresponding line from Fe6/2.
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32
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85033012941
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note
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Two weakly temperature-dependent transitions of rhFe at 150 mT are superimposed by a strong resonance of Fe4/2 for B ∥ [001]. Therefore these transitions are not suited to monitor rhFe [22], if signals from Fe4/2 are present at the same time.
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33
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85032998387
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note
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The reflection from the surface of the crystal plate becomes anisotropic upon rotation. This destroys the MCD-signal.
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34
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85033015490
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note
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Because of symmetry the projection of the polarization of the light, intended to achieve alignment, onto the local center axes cannot be chosen very differently for the various sites (see Fig. 4). Filling up only one site, for example, while depleting the others will therefore not be feasible, if rhFe can be aligned at all.
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39
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84923712144
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University of Osnabrück, to be published
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M. Mazur and O.F. Schirmer: University of Osnabrück, to be published
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Mazur, M.1
Schirmer, O.F.2
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42
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84923712143
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University of Osnabrück, private communication
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H. Donnerberg: University of Osnabrück, private communication.
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Donnerberg, H.1
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43
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85032998118
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note
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Hannon [8] reports on a similar finding of Wemple.
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44
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0016487566
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K.W. Blazey, O.F. Schirmer, W. Berlinger, and K.A. Müller: Solid State Commun. 16, 589 (1975)
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(1975)
Solid State Commun.
, vol.16
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Blazey, K.W.1
Schirmer, O.F.2
Berlinger, W.3
Müller, K.A.4
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