{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,5,29]],"date-time":"2026-05-29T23:35:27Z","timestamp":1780097727992,"version":"3.54.0"},"reference-count":47,"publisher":"AIP Publishing","issue":"18","funder":[{"name":"European Union H2020 Program","award":["668119"],"award-info":[{"award-number":["668119"]}]},{"name":"European Union COST Action","award":["CA15209"],"award-info":[{"award-number":["CA15209"]}]}],"content-domain":{"domain":["pubs.aip.org"],"crossmark-restriction":true},"short-container-title":[],"published-print":{"date-parts":[[2021,11,14]]},"abstract":"<jats:p>We consider the longitudinal quadrupole relaxation rate enhancement (QRE) of a 1H nucleus due to the time fluctuations of the local dipolar magnetic field created by a close quadrupole 14N nucleus, the electric-field gradient (EFG) Hamiltonian of which changes with time because of vibrations\/distortions of its chemical environment. The QRE is analytically expressed as a linear combination of the cosine Fourier transforms of the three quantum time auto-correlation functions GAA(t) of the 14N spin components along the principal axes A = X, Y, and Z of the mean (time-averaged) EFG Hamiltonian. Denoting the three transition frequencies between the energy levels of this mean Hamiltonian by \u03bdA, the functions GAA(t) oscillate at frequencies \u03bdA + sA\/(2\u03c0) with mono-exponential decays of relaxation times \u03c4A, where the frequency dynamic shifts sA and the relaxation times \u03c4A are closed expressions of the magnitude of the fluctuations of the instantaneous EFG Hamiltonian about its mean and of the characteristic fluctuation time. Thus, the theoretical QRE is the sum of three Lorentzian peaks centered at \u03bdA + sA\/(2\u03c0) with full widths at half maxima 1\/(\u03c0\u03c4A). The predicted peak widths are nearly equal. The predicted dynamic shifts of the peaks are much smaller than their widths and amazingly keep proportional to the transition frequencies \u03bdA for reasonably fast EFG fluctuations. The theory is further improved by correcting the transition frequencies by the 14N Zeeman effects of second order. It is successfully applied to reinterpret the QRE pattern measured by Broche, Ashcroft, and Lurie [Magn. Reson. Med. 68, 358 (2012)] in normal cartilage.<\/jats:p>","DOI":"10.1063\/5.0069362","type":"journal-article","created":{"date-parts":[[2021,10,21]],"date-time":"2021-10-21T21:37:32Z","timestamp":1634852252000},"update-policy":"https:\/\/doi.org\/10.1063\/aip-crossmark-policy-page","source":"Crossref","is-referenced-by-count":3,"title":["Nuclear relaxation rate enhancement by a 14N quadrupole nucleus in a fluctuating electric-field gradient"],"prefix":"10.1063","volume":"155","author":[{"given":"Elie","family":"Belorizky","sequence":"first","affiliation":[{"name":"Univ. Grenoble Alpes, CEA, Leti-DSYS 1 , 38000 Grenoble, France"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-7388-8448","authenticated-orcid":false,"given":"Pascal H.","family":"Fries","sequence":"additional","affiliation":[{"name":"Univ. Grenoble Alpes, CEA, IRIG-MEM 2 , 38000 Grenoble, France"}],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"317","published-online":{"date-parts":[[2021,11,11]]},"reference":[{"key":"2023062603403506400_c1","doi-asserted-by":"publisher","first-page":"804","DOI":"10.1063\/1.1744594","volume":"29","year":"1958","journal-title":"J. Chem. Phys."},{"key":"2023062603403506400_c2","doi-asserted-by":"publisher","first-page":"149","DOI":"10.1016\/0022-2364(76)90240-7","volume":"24","year":"1976","journal-title":"J. Magn. Reson."},{"key":"2023062603403506400_c3","doi-asserted-by":"publisher","first-page":"33","DOI":"10.1080\/00268978200100031","volume":"45","year":"1982","journal-title":"Mol. 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