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Mössbauer-Active Transition Metals Other than Iron

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Mössbauer Spectroscopy and Transition Metal Chemistry

Abstract

The previous chapters are exclusively devoted to the measurements and interpretation of 57Fe spectra of various iron-containing systems. Iron is, by far, the most extensively explored element in the field of chemistry compared with all other Mössbauer-active elements because the Mössbauer effect of 57Fe is very easy to observe and the spectra are, in general, well resolved and they reflect important information about bonding and structural properties. Besides iron, there are a good number of other transition metals suitable for Mössbauer spectroscopy which is, however, less extensively studied because of technical and/or spectral resolution problems. In recent years, many of these difficulties have been overcome, and we shall see in the following sections a good deal of successful Mössbauer spectroscopy that has been performed on compounds of nickel (61Ni), zinc (67Zn), ruthenium (mainly 99Ru), tantalum (181Ta), tungsten (mainly 182W, 183W), osmium (mainly 189Os), iridium (191Ir, 193Ir), platinum (195Pt), and gold (197Au). The nuclear γ-resonance effect in the case of technetium (99Tc), silver (107Ag), hafnium (176Hf, 177Hf, 178Hf, 180Hf), rhenium (187Re), and mercury (199Hg, 201Hg) has been of relatively little use to the chemists, so far. There are various reasons responsible for this, viz., (1) extraordinary difficulties in measuring the resonance effect because of the long lifetime of the excited Mössbauer level and hence the extremely small transition line width (e.g., in 67Zn), (2) poor resolution of the resonance lines due to either very small nuclear moments or the very short lifetime of the excited Mössbauer level resulting in very broad resonance lines, (3) insufficient resonance effects due to unusually high transition energies between the excited and the ground nuclear levels, which in turn increase the recoil energy and thus reduces the recoilless fraction of emitted and observed γ-rays.

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Notes

  1. 1.

    The observed ratio of the nuclear magnetic moments μ e/μ g is generally taken to be constant for the nuclear states of a given Mössbauer transition. This, however, is not necessarily so, because there may be slight differences in the interactions between the nuclear magnetic moment (with radial distribution due to orbital and spin motions of unpaired nucleons) and an applied magnetic field (which is uniform over the nuclear magnetization distribution) on the one hand, and with an internal hyperfine field (which may also have radial distribution) on the other hand. Such differences will be reflected in differences of the ratio μ e /μ g observed for the two cases of interaction. This is called “hyperfine anomaly”.

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Authors and Affiliations

  1. Inst. Anorganische und Analytische Chemie, Universität Mainz, Staudingerweg 9, 55099, Mainz, Germany

    Prof. Dr. Philipp Gütlich & Prof. Dr. Alfred X. Trautwein

  2. MPI für Bioanorganische, Chemie, Stiftstr. 34-36, 45470, Mülheim, Germany

    Dr. Eckhard Bill

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  1. Prof. Dr. Philipp Gütlich
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  2. Dr. Eckhard Bill
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  3. Prof. Dr. Alfred X. Trautwein
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Gütlich, P., Bill, E., Trautwein, A.X. (2011). Mössbauer-Active Transition Metals Other than Iron. In: Mössbauer Spectroscopy and Transition Metal Chemistry. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-88428-6_7

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