Abstract
The solid-state NMR of quadrupolar nuclei is becoming more important to date. The anisotropy of quadrupolar coupling cannot be eliminated by magic-angle spinning. Although large quadrupolar couplings often prevent us to observe NMR signals of quadrupolar nuclei as sufficiently separated signals, the recent development of the equipment and methods including DNP, are spreading our opportunities of NMR observation to a wider range of materials and in deeper levels of information. The quadrupolar parameters, which can be taken from NMR spectra of quadrupolar nuclei, have a potential usefulness to distinguish atoms depending on their local electrostatic environment. MQMAS or STMAS enable us not only to observe quadrupolar nuclei in separated signals but also to get quadrupolar parameters and isotopic chemical shifts of each the separated signal component in a 2D spectrum. J- or D-HMQC, CP-HETCOR and related techniques provide us information about inter-atomic chemical bonding or geometrical correlations. When the sensitivity is insufficient, besides isotopes enrichment, for quadrupolar nuclei specifically, enhancement through intra-spin population transfer methods, RAPT, FAM, DFS, WURST and HS can be applied. WURST, when combined with QCPMG method, can provide us a method for obtaining NMR spectra for those nuclei having huge quadrupolar coupling that we cannot observe the whole signal shape by simple methods. This article is dealing with the NMR methods being standard at the present, or becoming standard in the near future, especially for the practical samples, for example, mixed samples or amorphous samples. A number of experimental hints and a couple of experimental examples of 27Al and 17O are described.
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- 1.
The ESR and Mössbauer spectra also have similar characteristics.
- 2.
It is at least two orders lower even compared to the peak frequency of the Universe’s 3.7 K background radiation, having its peak frequency at 160.2 GHz, which is around 2 orders lower to that of the earth’s environmental temperatures.
- 3.
According to Cohen 1954, the order of quadrupolar interaction is as large as \(Q_{jk}^{\prime} \left( {\partial^{2} V/\partial x_{i} \partial x_{j} } \right) \sim er_{n}^{2} \left( {\frac{e}{{r_{e}^{3} }}} \right) = eV_{0} \left( {r_{n} /r_{e} } \right)^{2}\). The quadrupolar interaction is around 10−8 compared to the electrostatic force between the charges within the nucleus.
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Acknowledgements
The author is fully thanking to Prof. Naito, an editor of this book, for his kind and enduring help and encouragement; without his help, I couldn’t complete my task. I thank Prof. Takegoshi for his frank and helpful discussion. I also thank to Dr. Hayashi who gave me instruction of the solid-state NMR especially in my launching days. I also thank to the comittee members of Japanese Solid-state NMR and Material Forum (no English site, the site only in Japanesse, http://kuchem.kyoto-u.ac.jp/bun/forum/nmr.html) and the Nuclear Magnetic Resonance Society of Japan ( http://www.nmrj.jp/index.php?page=index-e) and people who have been gathering there and giving me a plenty of fruitful infromation and discussions. Finally, I would express another deep acknowlegement to National Institute of Indurstiral Science and Technology (AIST), and New Energy and Industry Technology Developement Organization (NEDO) and people who are working there for their financial and everyday supports in everywhere.
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Takahashi, T. (2018). Quadrupole Nuclei in Inorganic Materials. In: The Nuclear Magnetic Resonance Society of Japan (eds) Experimental Approaches of NMR Spectroscopy. Springer, Singapore. https://doi.org/10.1007/978-981-10-5966-7_20
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