title: Perspectives of Deuteron Field-Cycling NMR Relaxometry for Probing Molecular Dynamics in Soft Matter.
abstract: Due to the single-particle character of the quadrupolar interaction in molecular systems, (2)H NMR poses a unique method for probing reorientational dynamics. Spin-lattice relaxation gives access to the spectral density, and its frequency dependency can be monitored by field-cycling (FC) techniques. However, most FC NMR studies employ (1)H; the use of (2)H is still rare. We report on the application of (2)H FC NMR for investigating the dynamics in molecular liquids and polymers. Commercial as well as home-built relaxometers are employed accessing a frequency range from 30 Hz to 6 MHz. Due to low gyromagnetic ratio, high coupling constants, and finite FC switching times, current (2)H FC NMR does not reach the dispersion region in liquids (toluene and glycerol), yet good agreement with the results from conventional high-field (HF) relaxation studies is demonstrated. The pronounced difference at low frequencies between (2)H and (1)H FC NMR data shows the relevance of intermolecular relaxation in the case of (1)H NMR. In the case of the polymers polybutadiene and poly(ethylene-alt-propylene), very similar relaxation dispersion is observed and attributed to Rouse and entanglement dynamics. Combination with HF (2)H relaxation data via applying frequency-temperature superposition allows the reconstruction of the full spectral density reflecting both polymer as well as glassy dynamics. Transformation into the time domain yields the reorientational correlation function C2(t) extending over nine decades in time with a long-time power law, C2(t) ∝ t(-0.45±0.05), which does not conform to the prediction of the tube-reptation model, for which ∝ t(-0.25) is expected. Entanglement sets in below C2(t = τe) ≅ S(2) = 0.001, where τe is the entanglement time and S the corresponding order parameter. Finally, we discuss the future prospects of the (2)H FC NMR technique.
authors.affiliation: Experimentalphysik II, Universität Bayreuth , 95440 Bayreuth, Germany.
authors.forename: M
authors.initials: M
authors.lastname: Flämig
authors.affiliation: Institut für Festkörperphysik, TU Darmstadt , Hochschulstrasse 6, 64289 Darmstadt, Germany.
authors.forename: M
authors.initials: M
authors.lastname: Becher
authors.affiliation: Experimentalphysik II, Universität Bayreuth , 95440 Bayreuth, Germany.
authors.forename: M
authors.initials: M
authors.lastname: Hofmann
authors.affiliation: Experimentalphysik II, Universität Bayreuth , 95440 Bayreuth, Germany.
authors.forename: T
authors.initials: T
authors.lastname: Körber
authors.affiliation: Institut für Festkörperphysik, TU Darmstadt , Hochschulstrasse 6, 64289 Darmstadt, Germany.
authors.forename: B
authors.initials: B
authors.lastname: Kresse
authors.affiliation: Institut für Festkörperphysik, TU Darmstadt , Hochschulstrasse 6, 64289 Darmstadt, Germany.
authors.forename: A F
authors.initials: AF
authors.lastname: Privalov
authors.affiliation: Institute of Complex Systems, Forschungszentrum Jülich , D-52425 Jülich, Germany.
authors.forename: L
authors.initials: L
authors.lastname: Willner
authors.affiliation: Faculty of Mathematics and Computer Science, University of Warmia & Mazury , Słoneczna 54, 10-710 Olsztyn, Poland.
authors.forename: D
authors.initials: D
authors.lastname: Kruk
authors.affiliation: Institut für Festkörperphysik, TU Darmstadt , Hochschulstrasse 6, 64289 Darmstadt, Germany.
authors.forename: F
authors.initials: F
authors.lastname: Fujara
authors.affiliation: Experimentalphysik II, Universität Bayreuth , 95440 Bayreuth, Germany.
authors.forename: E A
authors.initials: EA
authors.lastname: Rössler