{"title":"The pseudo-wigner distribution of double and triple resonances","authors":"J.H.J Leclerc","doi":"10.1016/0022-2364(92)90375-H","DOIUrl":"https://doi.org/10.1016/0022-2364(92)90375-H","url":null,"abstract":"","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 171-182"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90375-H","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"89988622","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Theoretical treatment of relaxation in the presence of an RF field","authors":"Scott A Smith, William E Palke, J.T Gerig","doi":"10.1016/0022-2364(92)90362-B","DOIUrl":"10.1016/0022-2364(92)90362-B","url":null,"abstract":"<div><p>A general description of relaxation of an arbitrary spin system in the presence of an RF field is given. The results show clearly how the presence of the RF field makes new combinations of frequencies important to the relaxation process. Exact solutions of the resulting equations are not possible, but introduction of conventional approximations provides forms that are complicated but amenable to machine solution.</p></div>","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 18-24"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90362-B","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"90226392","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"A deuteron NMR study of neopentane adsorbed on graphite. An example for the dominance of the magnetic shielding over the electric quadrupole coupling","authors":"G Auer, B Boddenberg","doi":"10.1016/0022-2364(92)90368-H","DOIUrl":"https://doi.org/10.1016/0022-2364(92)90368-H","url":null,"abstract":"<div><p>The deuteron NMR spectra and spin-lattice relaxation times of neopentane adsorbed on the graphitized carbon black Graphon at surface coverages between 0.1 and 1.2 were measured at two different Zeeman fields (2.1 and 8.1 T) in the temperature range 80–290 K. For comparison purposes the <sup>2</sup>H NMR spectra were measured for neopentane on boron nitride, on the nongraphitized carbon black Spheron, and on the graphitized carbon black Sterling MT. The spectra of neopentane on the graphitized carbon blacks in the Zeeman field <em>B</em><sub>0</sub> = 8.1 T are practically completely determined by an extramolecular magnetic shielding-type coupling arising from the anisotropic polarization of the graphite support. The spin-lattice relaxation times are dominated at temperatures of 80 to 150 K by the quadrupole coupling, whereas above 150 K the anisotropic shielding coupling dominates at high Zeeman field. The analysis of the spin-lattice relaxation times allows one to evaluate the reorientation times of the molecules about their center of gravity as well as the translational surface diffusion coefficients. The isotropic molecular reorientation rates were found to be of the same order of magnitude as those in the bulk liquid and plastic phases. The surface diffusion coefficients (about 5 × 10<sup>−8</sup> m<sup>2</sup> s<sup>−1</sup> at the bulk melting temperature 256.6 K) are about one order of magnitude larger than those in the bulk liquid.</p></div>","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 88-100"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90368-H","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"90014908","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Geerten W Vuister , Jesús Ruff-Cabello , Peter C.M van Zijl
{"title":"Gradient-enhanced multiple-quantum filter (ge-MQF). A simple way to obtain single-scan phase-sensitive HMQC spectra","authors":"Geerten W Vuister , Jesús Ruff-Cabello , Peter C.M van Zijl","doi":"10.1016/0022-2364(92)90381-G","DOIUrl":"10.1016/0022-2364(92)90381-G","url":null,"abstract":"","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 215-220"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90381-G","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75803568","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Ultra-high-resolution multiple-pulse 1H NMR of organic conductors","authors":"A.C Kolbert, M Mehring","doi":"10.1016/0022-2364(92)90367-G","DOIUrl":"https://doi.org/10.1016/0022-2364(92)90367-G","url":null,"abstract":"<div><p>it is shown that the use of multiple-pulse decoupling and magic-angle spinning can give extremely highly resolved <sup>1</sup>H NMR spectra of some organic conductors. Although the scaled linewidths approach 2.5 ppm, the dispersion of the resonances, due to large Knight shifts, is an order of magnitude larger than the usual 'H chemical-shift dispersion. This point is illustrated with spectra from two TCNQ salts in which up to eight chemically equivalent <sup>1</sup>H's, distinguished only by the amount of resident spin density on the bound carbon, are resolved.</p></div>","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 82-87"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90367-G","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91632259","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Comparison of the coherence-transfer efficiencies of laboratory- and rotating-frame experiments","authors":"A Ramamoorthy, N Chandrakumar","doi":"10.1016/0022-2364(92)90365-E","DOIUrl":"https://doi.org/10.1016/0022-2364(92)90365-E","url":null,"abstract":"<div><p>Coherence transfer under INEPT and isotropic mixing is quantified theoretically and the predictions are verified by experiments on various homonuclear spin systems. A general expression for magnetization transfer is derived for INEPT in A<sub><em>M</em></sub>X<sub><em>N</em></sub> systems, in terms of the “leaving fraction,” trigonometric function, “spin multiplier,” and “attenuation factor.” In general, coherence transfer under INEPT is not identical from A<sub><em>M</em></sub> to X<sub><em>N</em></sub> and X<sub><em>N</em></sub> to A<sub><em>M</em></sub> when <em>M</em> ≠ <em>N</em>. Unlike INEPT, in the case of isotropic mixing all magnetization components are conserved for the spin system as a whole, transfer is in-phase, and the <em>m</em> = 0 component of spin multiplets also plays a role in coherence transfer, leading to advantages over INEPT under conditions of unresolved couplings and integer composite angular momenta. Coherence-transfer efficiencies of these experiments are compared with the predicted universal bound on spin dynamics.</p></div>","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 60-68"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90365-E","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91632260","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Kinetics of the in vivo31P1H nuclear overhauser effect of the human-calf-muscle phosphocreatine resonance","authors":"Peter Bachert, Matthias E Bellemann","doi":"10.1016/0022-2364(92)90372-E","DOIUrl":"https://doi.org/10.1016/0022-2364(92)90372-E","url":null,"abstract":"<div><p>In <sup>31</sup>P<sup>1</sup>H double-resonance experiments in a 1.5 T whole-body MR system, we observed <em>in vivo</em> the truncated driven, transient, and steady-state <sup>31</sup>P-<sup>1</sup>H nuclear Overhauser effect of the phosphocreatine resonance in <sup>31</sup>P MR spectra of human gastrocnemius muscle. Maximum signal enhancements of 0.52 ± 0.01, 0.20 ± 0.01, and 0.79 ± 0.02 were measured, respectively. Fitting the data with theoretical functions which solve the multispin Solomon equations for <em>N</em> protons (S spins) dipolar coupled to a <sup>31</sup>P nucleus (I spin) yields cross-relaxation times <span><math><mtext>2</mtext><mtext>[Σ</mtext><msub><mi></mi><mn><mtext>i=1−N </mtext><msup><mi></mi><mn>σ</mn></msup><mtext>IS</mtext><mtext>(i)</mtext></mn></msub><mtext>]</mtext></math></span> in the order of 20 s. <em>In vivo</em> experiments are feasible for studying relaxation mechanisms in coupled <sup>31</sup>P<sup>1</sup>H spin systems in intact tissue.</p></div>","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 146-156"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90372-E","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91632262","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Hyperfine-axis orientation in rhombic metal complexes from ENDOR-induced EPR and quadrupolar coupling determination","authors":"S.P Greiner , R.W Kreilick","doi":"10.1016/0022-2364(92)90364-D","DOIUrl":"https://doi.org/10.1016/0022-2364(92)90364-D","url":null,"abstract":"<div><p>The ENDOR resonances from ligand nuclei in paramagnetic transition-metal complexes exhibit a shift from the nuclear Larmor frequency because of the dipolar and Fermi contact interactions with the unpaired electron. The dipolar interaction has orientation dependence associated with its magnitude, where the position of the nuclei with respect to the metal atom determines the resonant frequencies and spectral lineshape. In this paper effects of rhombic g and metal hyperfine tensors on the EPR powder pattern and ENDOR spectra are illustrated. The EPR angular selection is modified from that encountered in axial systems and the technique of ENDOR-induced EPR is utilized to elucidate the orientation of magnetic axes with respect to one another. Quadrupole couplings in ENDOR spectra have often been analyzed using an equation from which cross terms have been omitted. The cross terms make important contributions to the spectra in some cases and the effect of these terms has been examined in order to determine when the complete equation for the quadrupole interaction must be utilized to analyze correctly ENDOR spectra.</p></div>","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 43-59"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90364-D","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91678224","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Indirect detection via the dipolar demagnetizing field","authors":"R Bowtell","doi":"10.1016/0022-2364(92)90361-A","DOIUrl":"https://doi.org/10.1016/0022-2364(92)90361-A","url":null,"abstract":"<div><p>A new method for indirectly detecting the magnetization of one spin species via the NMR signal of a second species is described. This method, which does not require that the spins of the two species be chemically coupled or even on the same molecule, relies on the nonlinear effect of the demagnetizing field produced by the nuclei themselves. It involves allowing I spins belonging to one spin species to precess under the influence of the demagnetizing field produced by S spins of a different species. The demagnetizing field generates an echo of the I magnetization. This echo carries information about the state of S magnetization and so offers a method of indirect detection. In certain circumstances this method can yield a signal-to-noise ratio higher than that given by direct detection. To demonstrate the process of echo formation, experiments have been carried out at 11.7 T on an aqueous solution of <sup>13</sup>C-enriched potassium cyanide. Here the water protons form the I spins, while the <sup>13</sup>C nuclei in the cyanide group form the S spins. The experimental results are in agreement with the theory outlined in this paper. Experimental methods which allow the application of this form of indirect detection to spectroscopy and imaging are also described.</p></div>","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 1-17"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90361-A","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91678251","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Analysis of inversion-magnetization-transfer experiments","authors":"S.V Santhana Mariappan, Dallas L Rabenstein","doi":"10.1016/0022-2364(92)90376-I","DOIUrl":"https://doi.org/10.1016/0022-2364(92)90376-I","url":null,"abstract":"","PeriodicalId":100800,"journal":{"name":"Journal of Magnetic Resonance (1969)","volume":"100 1","pages":"Pages 183-188"},"PeriodicalIF":0.0,"publicationDate":"1992-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0022-2364(92)90376-I","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91590514","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}