The effect of a broad activation energy distribution on deuteron spin–lattice relaxation

dc.contributor.authorE.E. Ylinen
dc.contributor.authorM. Punkkinen
dc.contributor.authorA. Birczyński
dc.contributor.authorZ.T. Lalowicz
dc.contributor.organizationfi=Wihurin fysiikantutkimuslaboratorio|en=Wihuri Physical Laboratory|
dc.contributor.organization-code1.2.246.10.2458963.20.26581883332
dc.contributor.organization-code2606701
dc.converis.publication-id1458014
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/1458014
dc.date.accessioned2025-08-27T22:42:18Z
dc.date.available2025-08-27T22:42:18Z
dc.description.abstract<p> Deuteron NMR spectra and spin–lattice relaxation were studied experimentally in zeolite NaY(2.4) samples containing 100 % or 200% of CD<sub>3</sub>OH or  CD<sub>3</sub>OD molecules of the total coverage of Na atoms in the temperature range 20 K – 150 K. The activation energies describing the methyl and hydroxyl motions show broad distributions. The relaxation data were interpreted by improving a recent model [Solid State Nucl. Magn. Reson. 49−50, 33–41 (2013)], in which the nonexponential relaxation curves are at first described by a sum of three exponentials with adjustable relaxation rates and weights. Then a broad distribution of activation energies (the mean activation energy <em>A</em><sub>0</sub> and the width s) was assumed for each essentially different methyl and hydroxyl position. The correlation times were calculated from the Arrhenius equation (containing the pre-exponential factor <em>t</em><sub>0</sub>), individual relaxation rates computed and classified into three classes, and finally initial relaxation rates and weights for each class formed. These were compared with experimental data, motional parameters changed slightly and new improved rates and weights for each class calculated, etc. This method was improved by deriving for the deuterons of the A and E species methyl groups relaxation rates, which depend explicitly on the tunnel frequency <em>w</em><sub>t</sub>. The temperature dependence of <em>w</em><sub>t</sub> and of the low–temperature correlation time were obtained by using the solutions of the Mathieu equation for a threefold potential. These dependencies were included in the simulations and as the result sets of <em>A</em><sub>0</sub>, s and <em>t</em><sub>0</sub> obtained, which describe the methyl and hydroxyl motions in different positions in zeolite.</p> <p>  </p>
dc.format.pagerange29
dc.identifier.jour-issn0926-2040
dc.identifier.olddbid202643
dc.identifier.oldhandle10024/185670
dc.identifier.urihttps://www.utupub.fi/handle/11111/47746
dc.identifier.urnURN:NBN:fi-fe2021042714139
dc.language.isoen
dc.okm.affiliatedauthorYlinen, Eero
dc.okm.affiliatedauthorPunkkinen, Matti
dc.okm.discipline114 Physical sciencesen_GB
dc.okm.discipline114 Fysiikkafi_FI
dc.okm.internationalcopublicationinternational co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherElsevier
dc.publisher.countryUnited Kingdomen_GB
dc.publisher.countryBritanniafi_FI
dc.publisher.country-codeGB
dc.relation.doi10.1016/j.ssnmr.2015.10.006
dc.relation.ispartofjournalSolid State Nuclear Magnetic Resonance
dc.relation.volume71
dc.source.identifierhttps://www.utupub.fi/handle/10024/185670
dc.titleThe effect of a broad activation energy distribution on deuteron spin–lattice relaxation
dc.year.issued2015

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