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Oral 22<br />

Abstract<br />

Theory <str<strong>on</strong>g>and</str<strong>on</strong>g> applicati<strong>on</strong>s of the fast electr<strong>on</strong>ic relaxati<strong>on</strong> of complexed<br />

paramagnetic lanthanide Ln 3+ i<strong>on</strong>s, but Gd 3+ , in soluti<strong>on</strong><br />

Pascal H. Fries<br />

CEA, INAC, SCIB (UMR-E 3 CEA-UJF),<br />

Laboratoire de Rec<strong>on</strong>naissance I<strong>on</strong>ique et Chimie de Coordinati<strong>on</strong>,<br />

38054, Grenoble, France<br />

Following a precise method proposed by Aime et al., 1 the very short relaxati<strong>on</strong> times T<br />

1e<br />

( = T2e<br />

) of<br />

the total electr<strong>on</strong>ic angular momenta J of the heavy paramagnetic Ln 3+ i<strong>on</strong>s from Tb 3+ to Yb 3+<br />

were recently derived in four series of isostructural complexes from the measured variati<strong>on</strong> with<br />

field B<br />

0<br />

of the nuclear relaxati<strong>on</strong> rates of selected nuclei of the lig<str<strong>on</strong>g>and</str<strong>on</strong>g>s. 2 Combined with earlier<br />

data, these additi<strong>on</strong>al values of T<br />

1e<br />

, in the range 0.1 – 0.63 ps, make it possible to infer a remarkable<br />

statistical ordering across the Ln 3+ series. A theory of lanthanide electr<strong>on</strong>ic relaxati<strong>on</strong> due to the<br />

time fluctuati<strong>on</strong>s of the lig<str<strong>on</strong>g>and</str<strong>on</strong>g> field coefficients induced by the very frequent collisi<strong>on</strong>s with the<br />

solvent molecules is briefly presented. 2-4 This theory, bey<strong>on</strong>d the Redfield approximati<strong>on</strong>, explains<br />

the surprisingly weak variati<strong>on</strong> of electr<strong>on</strong>ic relaxati<strong>on</strong> with the nature of the lig<str<strong>on</strong>g>and</str<strong>on</strong>g>, the solvent, the<br />

temperature, <str<strong>on</strong>g>and</str<strong>on</strong>g> the field. It also c<strong>on</strong>firms the experimental tendency that complexes of Tb 3+ <str<strong>on</strong>g>and</str<strong>on</strong>g><br />

Dy 3+ are most efficient to accelerate the nuclear relaxati<strong>on</strong> rates. From selected examples, it is<br />

shown how such complexes can serve (i) to save time in parallel NMR arrangements, 5 which allow<br />

the simultaneous investigati<strong>on</strong> of several systems during a single high-resoluti<strong>on</strong> experiment <str<strong>on</strong>g>and</str<strong>on</strong>g><br />

(ii) to gain new supramolecular structural informati<strong>on</strong> around Ln 3+ centers with atomic precisi<strong>on</strong>. 6<br />

The NMR instruments <str<strong>on</strong>g>and</str<strong>on</strong>g> methods, which are available for measuring T<br />

1e<br />

of Ln 3+ i<strong>on</strong>s, but Gd 3+ ,<br />

in complexes <str<strong>on</strong>g>and</str<strong>on</strong>g> for using these complexes in applicati<strong>on</strong>s, are compared.<br />

References<br />

1<br />

2<br />

3<br />

4<br />

5<br />

6<br />

S. Aime, L. Barbero, M. Botta, <str<strong>on</strong>g>and</str<strong>on</strong>g> G. Erm<strong>on</strong>di, J. Chem. Soc., Dalt<strong>on</strong> Trans., 225 (1992).<br />

A. M. Funk, P. H. Fries, P. Harvey, A. M. Kenwright, <str<strong>on</strong>g>and</str<strong>on</strong>g> D. Parker, J. Phys. Chem. A 117,<br />

905 (2013).<br />

P. H. Fries <str<strong>on</strong>g>and</str<strong>on</strong>g> E. Belorizky, J. Chem. Phys. 136, 074513 (2012).<br />

P. H. Fries, Eur. J. Inorg. Chem., 2156 (2012).<br />

P. H. Fries <str<strong>on</strong>g>and</str<strong>on</strong>g> D. Imbert, J. Chem. Eng. Data 55, 2048 (2010).<br />

P. H. Fries, J. Chem. Phys. 136, 044504 (2012).<br />

<str<strong>on</strong>g>8th</str<strong>on</strong>g> <str<strong>on</strong>g>C<strong>on</strong>ference</str<strong>on</strong>g> <strong>on</strong> Fast Field Cycling NMR Relaxometry, Turin 23-25 May 2013

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