{"title":"Analytical descriptions of (multiple-contact) cross-polarization dynamics and spin-lattice relaxation in solid alanine","authors":"Jérôme Hirschinger, Jésus Raya","doi":"10.1016/j.jmro.2023.100128","DOIUrl":null,"url":null,"abstract":"<div><p>In this work, several exact and approximate analytical solutions to the quantum master equation are derived using both classical and non-classical coupling models to describe the kinetics of Hartmann-Hahn cross-polarization (HHCP) and multiple-contact CP (MC<img>CP). Moreover, the analytical solution originally obtained by Naito and McDowell [J. Chem. Phys. 84 (1986) 4181.] is shown to be incorrect and the different regimes of spin diffusion and <span><math><msub><mi>T</mi><mrow><mn>1</mn><mi>ρ</mi></mrow></msub></math></span> relaxation are characterized by the amplitude of the second stage of the HHCP dynamics and the HHCP/MC<img>CP crossing time. The analysis of the <sup>1</sup>H–<sup>13</sup>C HHCP and MC<img>CP dynamics together with (Lee-Goldburg) <sup>1</sup>H <span><math><msub><mi>T</mi><mrow><mn>1</mn><mi>ρ</mi></mrow></msub></math></span> relaxation experimental data provides a consistent picture of spin dynamics in solid alanine and explains the apparent discrepancies previously observed between <span><math><msub><mi>T</mi><mrow><mn>1</mn><mi>ρ</mi></mrow></msub></math></span> and <span><math><msub><mi>T</mi><mn>1</mn></msub></math></span> relaxation measurements. The CH and CH<sub>3</sub> protons relax as expected <em>via</em> spin diffusion towards the NH<sub>3</sub> protons but the assumption of common proton spin temperature, in which the bottleneck of relaxation is at the NH<sub>3</sub> sites, generally valid for <span><math><msub><mi>T</mi><mn>1</mn></msub></math></span> relaxation breaks down for <span><math><msub><mi>T</mi><mrow><mn>1</mn><mi>ρ</mi></mrow></msub></math></span> relaxation. A diffusion-limited situation in which nuclear Zeeman energy is transferred to the lattice faster than can be supplied by spin diffusion is observed instead.</p></div>","PeriodicalId":365,"journal":{"name":"Journal of Magnetic Resonance Open","volume":"16 ","pages":"Article 100128"},"PeriodicalIF":2.6240,"publicationDate":"2023-07-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2666441023000365/pdfft?md5=8634b4f0bfee2e20f4a4370925e073c3&pid=1-s2.0-S2666441023000365-main.pdf","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Magnetic Resonance Open","FirstCategoryId":"1","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2666441023000365","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
In this work, several exact and approximate analytical solutions to the quantum master equation are derived using both classical and non-classical coupling models to describe the kinetics of Hartmann-Hahn cross-polarization (HHCP) and multiple-contact CP (MCCP). Moreover, the analytical solution originally obtained by Naito and McDowell [J. Chem. Phys. 84 (1986) 4181.] is shown to be incorrect and the different regimes of spin diffusion and relaxation are characterized by the amplitude of the second stage of the HHCP dynamics and the HHCP/MCCP crossing time. The analysis of the 1H–13C HHCP and MCCP dynamics together with (Lee-Goldburg) 1H relaxation experimental data provides a consistent picture of spin dynamics in solid alanine and explains the apparent discrepancies previously observed between and relaxation measurements. The CH and CH3 protons relax as expected via spin diffusion towards the NH3 protons but the assumption of common proton spin temperature, in which the bottleneck of relaxation is at the NH3 sites, generally valid for relaxation breaks down for relaxation. A diffusion-limited situation in which nuclear Zeeman energy is transferred to the lattice faster than can be supplied by spin diffusion is observed instead.