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Oral 16<br />
Abstract<br />
The Interplay of MD <str<strong>on</strong>g>and</str<strong>on</strong>g> QM calculati<strong>on</strong>s to elucidate singlet state relaxati<strong>on</strong><br />
Pär Håkanss<strong>on</strong>, Giuseppe Pileio, <str<strong>on</strong>g>and</str<strong>on</strong>g> Malcolm H Levitt<br />
Department of Chemistry, University of Southampt<strong>on</strong>, SO17 1BJ, Southampt<strong>on</strong>, UK<br />
(e-mail: p.hakanss<strong>on</strong>@sot<strong>on</strong>.ac.uk)<br />
Under certain c<strong>on</strong>diti<strong>on</strong>s systems of two spin-1/2<br />
support singlet states that are immune to the intra-pair dipolar Molecular model of N 2O in DMSO<br />
relaxati<strong>on</strong> superoperator therefore often showing characteristic<br />
decay c<strong>on</strong>stants T S which exceed T 1 by an order of magnitude<br />
or more. These enhanced lifetimes are of particular interest as<br />
polarizati<strong>on</strong> (<str<strong>on</strong>g>and</str<strong>on</strong>g> indeed hyperpolarizati<strong>on</strong>) can be stored for<br />
l<strong>on</strong>ger time intervals with important applicati<strong>on</strong> in MRI, for<br />
example. Because of the extended time regime, many other<br />
“minor” relaxati<strong>on</strong> mechanism interplay to relax these states.<br />
An exact knowledge of these mechanisms can indicate the<br />
c<strong>on</strong>diti<strong>on</strong>s to maximize <str<strong>on</strong>g>and</str<strong>on</strong>g> extend even further singlet<br />
lifetimes. However, even relatively small molecules in soluti<strong>on</strong><br />
impose a number of challenges in the task of modeling T 1 <str<strong>on</strong>g>and</str<strong>on</strong>g><br />
T S from molecular dynamics simulati<strong>on</strong> (MD) <str<strong>on</strong>g>and</str<strong>on</strong>g> quantum mechanics calculati<strong>on</strong>s QM.<br />
Computati<strong>on</strong>al cost is <strong>on</strong>e major bottleneck. In additi<strong>on</strong>, in order to accurately model l<strong>on</strong>g T S ,<br />
attenti<strong>on</strong> is required to the weak <str<strong>on</strong>g>and</str<strong>on</strong>g> rather poorly explored relaxati<strong>on</strong> mechanisms such as spinrotati<strong>on</strong>.<br />
In this work we use novel approaches to address chemical shift anisotropy, spin-rotati<strong>on</strong> <str<strong>on</strong>g>and</str<strong>on</strong>g><br />
inter-molecular dipole-dipole relaxati<strong>on</strong> mechanisms within the joint framework of MD <str<strong>on</strong>g>and</str<strong>on</strong>g> QM<br />
calculati<strong>on</strong>s. We take particular care of molecular flexibility. The CSA c<strong>on</strong>tributi<strong>on</strong>, for example, is<br />
computed using a timescale-separated spin Hamilt<strong>on</strong>ian, paying particular attenti<strong>on</strong> to internal<br />
molecular degrees of freedom. In the case of spin-rotati<strong>on</strong>, the explicit time dependent spin<br />
Hamilt<strong>on</strong>ian is c<strong>on</strong>sidered. We dem<strong>on</strong>strate a good quantitative agreement between experiments <str<strong>on</strong>g>and</str<strong>on</strong>g><br />
calculati<strong>on</strong>s without adjustable parameters. We discuss the field-dependence of T S <str<strong>on</strong>g>and</str<strong>on</strong>g> T 1 .<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